準周期構造の理論的基礎 Theoretical introduction to...
Transcript of 準周期構造の理論的基礎 Theoretical introduction to...
準周期構造の理論的基礎Theoretical introduction to
quasiperiodic structures
Nobuhisa Fujita
IMRAM Tohoku University
Sendai 980-8577 Japan
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1
Outline
1 Introduction pp3-8
2 Z-modules for quasicrystals pp9-23
3 Quasiperiodic tilings (QPTs) pp24-31
4 Methods for generating QPTs pp32-61
5 Approximants pp62-78
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― 準周期構造の理論と基礎 ―
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1 Introduction
ED pattern from a rapidly quenched Al-Mn alloy
D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
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D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
5-fold rotational symmetry is not compatible with periodicity still the diffraction peaks are very sharp
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Quasicrystals as a new class of ordered solids
D Levine and PJ Steinhardt Phys Rev Lett 53 (1984) 2477mdash2480
1 Long-range quasiperiodic translational order
A QC exhibits a self-similar arrangement of Bragg peaks (120633functions) whose indexing needs 119896 (gt 119889) independent basis vectors for indexing (119889 the number of space dimensions)
2 Non-crystallographic point group symmetry
A QC exhibits a point group symmetry forbidden in periodic crystals (eg 119899-fold rotational axes with 119899 being a natural number excluding 1 2 3 4 and 6)
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Paradigm shift in crystallography the New definition of crystals (1992)
International Union of Crystallography Report of the Executive Committee for 1991 Acta Cryst A48 (1992) 922mdash946
The definition proposed by the IUCr Commission on Aperiodic Structures (IUCr 1991)
by crystal we mean any solid having an essentially discrete diffraction diagram and
aperiodic crystal we mean any crystal in which three-dimensional lattice periodicity
can be considered to be absent
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Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
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Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
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120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
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119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Dual-grid method≃ Cut-and-project method ≃ Section method
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Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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Outline
1 Introduction pp3-8
2 Z-modules for quasicrystals pp9-23
3 Quasiperiodic tilings (QPTs) pp24-31
4 Methods for generating QPTs pp32-61
5 Approximants pp62-78
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― 準周期構造の理論と基礎 ―
2
1 Introduction
ED pattern from a rapidly quenched Al-Mn alloy
D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
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D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
5-fold rotational symmetry is not compatible with periodicity still the diffraction peaks are very sharp
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― 準周期構造の理論と基礎 ―1 Introduction
4
Quasicrystals as a new class of ordered solids
D Levine and PJ Steinhardt Phys Rev Lett 53 (1984) 2477mdash2480
1 Long-range quasiperiodic translational order
A QC exhibits a self-similar arrangement of Bragg peaks (120633functions) whose indexing needs 119896 (gt 119889) independent basis vectors for indexing (119889 the number of space dimensions)
2 Non-crystallographic point group symmetry
A QC exhibits a point group symmetry forbidden in periodic crystals (eg 119899-fold rotational axes with 119899 being a natural number excluding 1 2 3 4 and 6)
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― 準周期構造の理論と基礎 ―1 Introduction
5
Paradigm shift in crystallography the New definition of crystals (1992)
International Union of Crystallography Report of the Executive Committee for 1991 Acta Cryst A48 (1992) 922mdash946
The definition proposed by the IUCr Commission on Aperiodic Structures (IUCr 1991)
by crystal we mean any solid having an essentially discrete diffraction diagram and
aperiodic crystal we mean any crystal in which three-dimensional lattice periodicity
can be considered to be absent
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― 準周期構造の理論と基礎 ―1 Introduction
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Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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7
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
1 Introduction
ED pattern from a rapidly quenched Al-Mn alloy
D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
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― 準周期構造の理論と基礎 ―
3
D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
5-fold rotational symmetry is not compatible with periodicity still the diffraction peaks are very sharp
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― 準周期構造の理論と基礎 ―1 Introduction
4
Quasicrystals as a new class of ordered solids
D Levine and PJ Steinhardt Phys Rev Lett 53 (1984) 2477mdash2480
1 Long-range quasiperiodic translational order
A QC exhibits a self-similar arrangement of Bragg peaks (120633functions) whose indexing needs 119896 (gt 119889) independent basis vectors for indexing (119889 the number of space dimensions)
2 Non-crystallographic point group symmetry
A QC exhibits a point group symmetry forbidden in periodic crystals (eg 119899-fold rotational axes with 119899 being a natural number excluding 1 2 3 4 and 6)
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― 準周期構造の理論と基礎 ―1 Introduction
5
Paradigm shift in crystallography the New definition of crystals (1992)
International Union of Crystallography Report of the Executive Committee for 1991 Acta Cryst A48 (1992) 922mdash946
The definition proposed by the IUCr Commission on Aperiodic Structures (IUCr 1991)
by crystal we mean any solid having an essentially discrete diffraction diagram and
aperiodic crystal we mean any crystal in which three-dimensional lattice periodicity
can be considered to be absent
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― 準周期構造の理論と基礎 ―1 Introduction
6
Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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7
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
D Shechtman et al Phys Rev Lett 53 (1984) 1951mdash1953
5-fold rotational symmetry is not compatible with periodicity still the diffraction peaks are very sharp
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― 準周期構造の理論と基礎 ―1 Introduction
4
Quasicrystals as a new class of ordered solids
D Levine and PJ Steinhardt Phys Rev Lett 53 (1984) 2477mdash2480
1 Long-range quasiperiodic translational order
A QC exhibits a self-similar arrangement of Bragg peaks (120633functions) whose indexing needs 119896 (gt 119889) independent basis vectors for indexing (119889 the number of space dimensions)
2 Non-crystallographic point group symmetry
A QC exhibits a point group symmetry forbidden in periodic crystals (eg 119899-fold rotational axes with 119899 being a natural number excluding 1 2 3 4 and 6)
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― 準周期構造の理論と基礎 ―1 Introduction
5
Paradigm shift in crystallography the New definition of crystals (1992)
International Union of Crystallography Report of the Executive Committee for 1991 Acta Cryst A48 (1992) 922mdash946
The definition proposed by the IUCr Commission on Aperiodic Structures (IUCr 1991)
by crystal we mean any solid having an essentially discrete diffraction diagram and
aperiodic crystal we mean any crystal in which three-dimensional lattice periodicity
can be considered to be absent
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― 準周期構造の理論と基礎 ―1 Introduction
6
Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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7
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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― 準周期構造の理論と基礎 ―
9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Quasicrystals as a new class of ordered solids
D Levine and PJ Steinhardt Phys Rev Lett 53 (1984) 2477mdash2480
1 Long-range quasiperiodic translational order
A QC exhibits a self-similar arrangement of Bragg peaks (120633functions) whose indexing needs 119896 (gt 119889) independent basis vectors for indexing (119889 the number of space dimensions)
2 Non-crystallographic point group symmetry
A QC exhibits a point group symmetry forbidden in periodic crystals (eg 119899-fold rotational axes with 119899 being a natural number excluding 1 2 3 4 and 6)
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― 準周期構造の理論と基礎 ―1 Introduction
5
Paradigm shift in crystallography the New definition of crystals (1992)
International Union of Crystallography Report of the Executive Committee for 1991 Acta Cryst A48 (1992) 922mdash946
The definition proposed by the IUCr Commission on Aperiodic Structures (IUCr 1991)
by crystal we mean any solid having an essentially discrete diffraction diagram and
aperiodic crystal we mean any crystal in which three-dimensional lattice periodicity
can be considered to be absent
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― 準周期構造の理論と基礎 ―1 Introduction
6
Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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― 準周期構造の理論と基礎 ―1 Introduction
7
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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― 準周期構造の理論と基礎 ―
9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Paradigm shift in crystallography the New definition of crystals (1992)
International Union of Crystallography Report of the Executive Committee for 1991 Acta Cryst A48 (1992) 922mdash946
The definition proposed by the IUCr Commission on Aperiodic Structures (IUCr 1991)
by crystal we mean any solid having an essentially discrete diffraction diagram and
aperiodic crystal we mean any crystal in which three-dimensional lattice periodicity
can be considered to be absent
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― 準周期構造の理論と基礎 ―1 Introduction
6
Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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― 準周期構造の理論と基礎 ―1 Introduction
7
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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― 準周期構造の理論と基礎 ―
9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Aperiodic order Three known categoriesQuasiperiodic structure (QCs incommensurate modulation composite crystals)
A structure that show Bragg peaks (120633 functions) in diffraction patterns which require 119896 (gt 119889) independent reciprocal basis vectors for indexing where 119889 is the of space dimensions and 119896 lt infin
Limit-periodic structureA structure with recursive (or hierarchical) superlattice structures superposed on a basic periodic latticeK Niizeki and N Fujita Philos Mag 87 (2007) 3073mdash3078 and references cited therein
Limit-quasiperiodic structureA structure that can be obtained as an incommensurate section of a limit-periodic structure in higher dimensionsK Niizeki and N Fujita J Phys A Math Gen 38 (2005) L199mdashL204 and references cited therein
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― 準周期構造の理論と基礎 ―1 Introduction
7
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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― 準周期構造の理論と基礎 ―
9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
5m 8mm 10mm 12mm 18mm ത5ത32119898
2-dim 3-dim
Metallic alloysSoft matter Metallic
alloys
Non-crystallographic point groups for quasicrystals
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― 準周期構造の理論と基礎 ―1 Introduction
8
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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― 準周期構造の理論と基礎 ―
9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
2 Z-Modules for quasicrystals
Reciprocal (= Fourier) module 120028lowast
≃ A dense (ne discrete) point set in the 119941-dim wave-number (or reciprocal) space generated as the integer linear combinations of 119948 (gt 119941) reciprocal basis vectors used to index the Bragg peaks
Direct (= Bravais) module 120028
≃ A dense (ne discrete) point set in the 119941-dim real (or direct) space generated as the integer linear combinations of 119948 (gt 119941) basis vectors used to index the quasi-lattice points or tiling vertices
Additive Abelian group over an integer ring (Z) Alternatives to lattices for periodic crystals
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― 準周期構造の理論と基礎 ―
9
(Z-加群)
( 119948 rank 119941 space dimensions )
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Ex) Fourier module for decagonal QC
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
10
ℳ10lowast = σ119895=1
4 119899119895119944119895 119899119895 isin ℤ
120591 =1 + 5
2= 2cos(
120587
5)
(golden mean)
Point group
1
t
1199441
1199442
1199443
1199444 (119944120787)
10mm
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Minimal basis set for indexing the Bragg peaks
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
11
119889 = 2119896 = 4
119889 = 2119896 = 6
119889 = 3119896 = 6
g 6
g 5
g 4
g 2
g 3
g 1
Point groups
octakaidecagonaldodecagonal
decagonaloctagonalpentagonalicosahedral
5m 8mm 10mm 12mm 18mm ത5ത32119898
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
For a planar 119899-gonal quasicrystal the minimal number of basis vectors is 119896 = 120601 119899 where 120601 119899(Eulerrsquos 120601-function) is the number of positive integers up to 119899 that are co-prime with 119899
120601 119899 = 119899ς119895 1 minus1
119901119895(119901119895 isin all prime factors of 119899)
σ119895120601 119889119895 = 119899 (119889119895 isin all divisors of 119899)
1199441
1199442
1199443
1199444
119944119899
119944120584 + 119944119889119895+120584 + 1199442119889119895+120584 +⋯+ 119944119899minus119889119895+120584 = 0 | 1 le 120584 le 120601(119889119895)1le119889119895lt119899
Check There are 119899 minus 120601 119899 independent constraints for the 119899 unit vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
12
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
Hyper-space119896-dim
ℳlowastReciprocal space
(perpendicular dims)(119896 minus 119889)-dim Reciprocal space
(physical dims)119889-dim
Observed Bragg peaks
119896 basis vectors
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
13
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Lifting up the of space dimensions
119889-dim Fourier module ℳlowast of rank 119896can be lift up to 119896-dim reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
14
ℒlowast
The amplitude of each Bragg peak in the 119889-dimensional Fourier space is assigned to the corresponding reciprocal hyper-lattice point in 119896 dimensions
Reciprocal space(perpendicular dims)
(119896 minus 119889)-dim Reciprocal space(physical dims)
119889-dim
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Complementary components 119944119895perp
119866ℳlowast point group of the Fourier module ℳlowast of the QC
119866ℒlowast point group of the 119896-dim reciprocal hyper-lattice ℒlowast
119866ℒlowast should have a subgroup 119867 which is isomorphic to 119866ℳlowast (ie 119866ℒlowast sup 119867 cong 119866ℳlowast) and which does not mix the physical and orthogonal components ie
ഥ119863 =119863 00 119863perp where ഥ119863 isin 119867 and 119863 isin 119866ℳlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
15
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Lifting up the of space dimensions[119896-dim basis vectors ഥ119944119947 = (119944119947 119944119947
perp) of ℒlowast]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
16
[1] K Niizeki J Phys Math Gen 22 (1989) 193mdash204[2] A Yamamoto Acta Cryst A52 (1996) 509mdash560
+ + ++
g 6
g 5
g 4
g 2
g 3
g 1
ḡ 5
ḡ 4
ḡ 2
ḡ 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Structure factors
119878(119918)| 119918 isin ℳlowast
ҧ119878(ഥ119918)| ഥ119918 isin ℒlowast
120588119889 119955 =
119918isinℳlowast
119878(119918)119890119894119918sdot119955
120588119896 ത119955 = ഥ119918isinℒlowast
ҧ119878(ഥ119918)119890119894ഥ119918sdotത119955
Fourier tr(119948-dim)
Fourier tr(119941-dim)
projection section
(Direct space)(Reciprocal space)
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
Physical dims(d-dim)
Hyper-space(k-dim)
17
lt
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
ℒ
The real charge density in the physical space is a 119889-dim section of a periodic array of atomic surfaces in 119896-dim hyper-space obtained as the Fourier transform of the 119896-dim structure factors
Charge density (periodic in hyper-space)
Direct space(perpendicular dims)
(119896 minus 119889)-dim Direct space(physical dims)
119889-dim
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
18
120588119889 119955 = 120588119896 ത119955 |ത119955=(119955120782)
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
119861 =
ഥ1199441ഥ1199442
⋮ഥ119944119899
119860 =
ഥ1199381ഥ1199382⋮ഥ119938119899
= (119861minus1)119879
ഥ119938119894 ∙ ഥ119944119895 = 120633119894119895
119896-dim bases ഥ119938119895 of the direct hyper-lattice ℒ= Fourier tr of the reciprocal hyper-lattice ℒlowast
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
19
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
119896-dimensional bases ഥ119938119895 = (119938119895 119938119895perp) of ℒ
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
20
+ + +
+
a 6
a 5
a 4
a 2
a 3
a 1
ā 5
ā 4
ā 2
ā 1
++
Physical components
Perpendicular components
5m 8mm 10mm 12mm 18mm ത5ത32119898
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
119811119842119851119838119836119853119825119838119836119842119849119851119848119836119834119845
hyper-lattices for quasicrystals
bull2-dim QC A unique hyper-lattice exists for 119899-gonal case
(119899 = 5 8 10 12 18 hellip)
bull3-dim QC Three hyper-lattices exist for icosahedral case P-type (SI) F-type (FCI) I-type (BCI)
ℒ119875 ≔ 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866
ℒ119865 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 σ119895=16 119899119895 = 0 mod 2
ℒ119868 = 1198991 ത1198861 + 1198992 ത1198862 + 1198993 ത1198863 + 1198994 ത1198864 + 1198995 ത1198865 + 1198996 ത1198866 119899119894 = 119899119895 mod 2
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
21
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Direct (= Bravais) module ℳ(projection of ℒ onto the physical sub-space)
Df) ℳ = σ119895=1119896 119899119895119938119895 119899119895 isin ℤ
Physical dims(d-dim)
Hyper-space(k-dim)
Perpendicular dims ((k-d)-dim)
Direct space
Reciprocal space
ℳ
ℳlowast ℒlowast
ℒ
ℳperplowast
ℳperp
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
22
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Self-similarity of ℳ (and ℳlowast)Z-modules for quasicrystals are scale invariant There exists an irrational number 120649 called the Pisot
unit such that 120591ℳ=ℳ and 120591 gt 1
Pisot unit for important classes of QCs
ℳ5
ℳ10
120783 + 120787
120784
ℳ8
120783 + 120784
ℳ12
120784 + 120785
ℳ18
120649120783 = 120783 + 120647 + 120647minus120783
120649120784 = 120649120783 120649120783 minus 120783
(120647 = 119942120645119946120791 )
ℳ119868hF
ℳ119868hI
120783 + 120787
120784
ℳ119868hP
120784 + 120787
[1] DS Rokhsar et al Phys Rev B 35 (1987)5487mdash5495[2] LS Levitov and J Rhyner J Phys France 49 (1988) 1835mdash1849[3] K Niizeki J Phys Math Gen 22 (1989) 193mdash204
[12] [12][3] [3] [3] [3]
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― 準周期構造の理論と基礎 ―2 Z-modules for quasicrystals
23
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
3 Quasiperiodic tilings (QPTs)
P1 tiling
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 10
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― 準周期構造の理論と基礎 ―
24
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
72deg
72deg
72deg
144deg
72deg
36deg
36deg
216deg
kite
dart
P2 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1025
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
72degRhombus
+
36degRhombus
P3 tiling
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
R Penrose Math Intel 2 (1979) 32ndash37 B Gruenbaum GC Shephard Tilings and Patterns (Freeman New York 1987) Chap 1026
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Square+
45degRhombus
Ammann-Beenker tiling (8mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
27
F P M Beenker Eindhoven University of Technology Report No 82-WSK-04 (Eindhoven 1982)
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Square+
Equilateral triangle
Stampfli tiling(12mm)
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
28
P Stampfli Helv Phys Acta 59 (1986) 1260ndash1263J Hermisson C Richard M Baake J Phys I France 7 (1997) 1003ndash1018
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Fibonacci chain (or tiling) (1-dim)
The 119909 coordinate of every lattice point is represented as 119909 = 119894 +119895
120591
which belongs to the 1-dim Z-module ℳ = 119898+ 119899120591 | 119898 119899 isin ℤ
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
119909
120591 =1+ 5
2(golden mean)
L L L L L L L LS S S S S
Lrsquo Srsquo Lrsquo Lrsquo Srsquo Lrsquo Srsquo Lrsquo
LSLLSLSLLSLLShellip cong LrsquoSrsquoLrsquoLrsquoSrsquoLrsquoSrsquoLrsquohellip (Lrsquo=LS Srsquo=L) Cf 120591ℳ=ℳ
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
29
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Lifting up the of space dimensions
Perpendiculardims 119909perp
Physical dims 119909∥
ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381 ഥ1199381ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382 ഥ1199382
Zigzag chain
1 1 1 1 1 1 1 11t 1t 1t 1t 1t
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
30
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Cut-and-project methodS
pa
n o
f w
ind
ow
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
119909perp
119909∥
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― 準周期構造の理論と基礎 ―3 Quasiperiodic tilings (QPTs)
31
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
4 Methods for generating QPTs
Cut-and-projection
Section method
Substitution method(inflation-deflation)
Dual-grid method
(NG de Bruijn 1981)
Methods for constructing QPTs
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― 準周期構造の理論と基礎 ―
32
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Cut-and-project methodS
pa
n o
f w
ind
ow
119909perp
119909∥
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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33
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Section methodS
pa
n o
f w
ind
ow
119909perp
119909∥
Atomic surface
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
34
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Cut-and-project method≃ Section method
Sp
an o
f w
ind
ow
119909perp
119909∥
Check An atomic surface intersect with the physical space if and only if the corresponding lattice point is within the strip
ഥ1199381 = 1minus1
120591 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
35
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
36
Check All the squares which intersect with the horizontal axis are colored in red The left base points of the red square are inside the strip
119909∥
119909perp
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method≃ Cut-and-project method ≃ Section method
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
37
119909∥
119909perp
The base points of all the red squares are projected down to the physical space to form the vertices of the aperiodic tiling ndash the dual-grid method
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
L S
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Self-similarity ndash an geometrical basis
If we remove the vertex between L and S in every LS pair we get a new segment Lrsquo This is done simply by narrowing the window
[Cut-and-project method]
119909∥
119909perp
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38
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Self-similarity ndash an geometrical basis
L S
[Cut-and-project method]
119909∥
119909perp
ഥ1199381 + ഥ1199382 = 1205911
1205912 ഥ1199381 = 1 minus
1
120591
Lrsquo Srsquo
Here the window is reduced by a factor of 1120591 The new Lrsquo tile corresponds to the projection of a diagonal of the square unit cell
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
39
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909∥
119909perp
Lrsquo Srsquo
ഥ1199391 = 1205911
1205912 ഥ1199392 = 1 minus
1
120591
If the unit cell is chosen as a parallelogram as shown the new tiles Lrsquo and Srsquo correspond to the projection of the edges of the parallelogram
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
40
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Self-similarity ndash an geometrical basis[Cut-and-project method]
119909prime∥
119909primeperp
Lrsquo Srsquo
The Affine transformation ҧ119860 which rescales the 119909∥ and 119909perp axes by 1120591 and minus 120591 respectively will recover the original setting (cut-and-projection)
ҧ119860 ∙ ഥ1199391 = 1 minus1
120591 ҧ119860 ∙ ഥ1199392 =
1
120591 1 ҧ119860 =
1120591 00 minus120591
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
41
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method ndash practice in 1 dim
Grid points
1st series
2nd series
n1= -1 0 1 2 3 4 5 6
n2= 0 1 2 3
4
5
6
7
(22)
(12)
(11)
(23)(33)
(43)
(44)
(54)
(64)
(65)
Grid lines(1st series)
Grid lines(2nd series)
One-to-one correspondence
Intersecting cells(red squares)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
42
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Two-dimensional grid lines (in hyper-space)
1198991+ 1199041 ഥ1199381 + 120579ഥ1199382 (minusinfin lt 120579 lt infin) hellip 1st series
120579ഥ1199381 + 1198992+ 1199042 ഥ1199382 (minusinfin lt 120579 lt infin) hellip 2nd series
( 1199041 1199042 hellip phason shift parameters )
One-dimensional grid points (in physical sub-space)
(1198991+ 1199041)ഥ1199381 + 120579ഥ1199382 = (119909 0) rarr 120579 = 1120591(1198991+ 1199041)
rarr 119909 = (2 minus 1120591)(1198991+ 1199041) hellip 1st series
120579ഥ1199381 + (1198992+ 1199042)ഥ1199382 = (119909 0) rarr 120579 = 120591 (1198992+ 1199042)
rarr 119909 = (1 + 2120591)(1198992+ 1199042) hellip 2nd series
ഥ1199381 = 1 minus1
120591 ഥ1199382 =
1
120591 1
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
43
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Base points of the two unit cells that contact each other at a grid point (in the physical space)
(1st series) x = ( 2 - 1120591 ) (n1+s1) 120579 = 1120591(n1+s1)
n2 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1-1 n2) hellip indices for the squares
(2nd series) x = ( 1 + 2120591) (n2+s2) 120579 = 120591(n2+s2)
n1 = 120579 minus Frac[120579] = Floor[120579]
(n1 n2) (n1 n2-1) hellip indices for the squares
The vertices of the tiling are the projections of these base pointsbase point (n1 n2) harr vertex coordinate x = n1 + n2 120591
Dual-grid method ndash practice in 1 dim
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
44
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Dual-grid method ndash practice in 2 dims
Embedding dimension = 5
(119909 119910 119911 119906 119907)physical perpendicular
space space
1199381∥
edge vectors inthe physical space
1199382∥
1199383∥
1199384∥
1199385∥
P3 tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
45
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 25 cos 120593119895 sin 120593119895 cos 2120593119895 sin 2120593119895 12
where 120593119895 =2120587119895
5 119895 = 12345
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
physical space perpendicular space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
46
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method ndash practice in 2 dims5-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384+ 1198995ഥ1199385
Hyper-grids in 5-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ11993852nd grids 1198992+ 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ1199384+ 1205795ഥ11993854th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205795ഥ11993855th grids (1198995+ 1199045 )ഥ1199385 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 52(1198991 + 1199041 )1199381∥ + 120579(1199382
∥ minus 1199385∥
2nd grids 52(1198992 + 1199042 )1199382∥ + 120579(1199383
∥ minus 1199381∥)
3rd grids 52(1198993 + 1199043 )1199383∥ + 120579(1199384
∥ minus 1199382∥ )
4th grids 52(1198994 + 1199044 )1199384∥ + 120579(1199385
∥ minus 1199383∥ )
5th grids 52(1198995 + 1199045 )1199385∥ + 120579(1199381
∥ minus 1199384∥ )
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
(120579119895 free parameter)
(120579 free parameter)
47
Phason shifts
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
48
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
1198991 1198991+ 11198991 minus 1
1198992+ 1
1198992
1198992minus 1
(119909 119910 0 0 0)
1st grids
2nd grids
1198992+ 2
1198991+ 21198991 minus 2
an intersection of grid lines
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
49
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method ndash practice in 2 dims(119909 119910 0 0 0) = (1198991+ 1199041)ഥ1199381+ (1198992+ 1199042)ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ1199384+ 1205795ഥ1199385
1205793 = ഥ1199443 119909 119910 0 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
1205795 = ഥ1199445 119909 119910 0 0 0 = 1198995 + 1199045+ 120575rsquorsquo 1198995 = 1205795 minus 1199045 120575rsquorsquo = 119865119903119886119888(1205795minus 1199045)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4 5) hellip 5-dim reciprocal basis vecs
These equations determine five integers 1198991 1198992 1198993 1198994 1198995 which provide the indices of the base points of the four 5-dim unit cells that contact each other at the above intersection point (xy) of the 1st and 2nd grid lines rarr
① (1198991 1198992 1198993 1198994 1198995 )
② (1198991minus 1 1198992 1198993 1198994 1198995)
③ 1198991 1198992minus 1 1198993 1198994 1198995④ (1198991minus 1 1198992minus 1 1198993 1198994 1198995)
(similar formulas can be obtained foran intersection of ith and jth grid lines)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
50
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Dual-grid method ndash practice in 2 dims
(119909 119910 0 0 0)
①②
③④
1198991
1198992
Each intersection of two grid lines gives one
rhombus in the tiling
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
51
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Outer boundary (rhombic icosahedron)Projection of a 5-dim hyper-cubic unit cell into the 3-dim perpendicular space
Rhombic Penrose tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (3-dim)
52
P3 tiling
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Embedding dimension = 4
(119909 119910 119911 119906)
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Dual-grid method ndash practice in 2 dimsAmmann-Beenker tiling
edge vectors inthe physical space
45˚
1199384∥ 1199383
∥
1199382∥
1199381∥
physical perpendicular
space space
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
53
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
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Dual-grid method ndash practice in 2 dims
ഥ119938119895 = 1 2 cos(120593119895) sin(120593119895) cos(3120593119895) sin(3120593119895)
where 120593119895 =120587(119895minus1)
4 119895 = 1234
Check ഥ119938119946 sdot ഥ119938119947 = 120633119946119947 hellip the Kronecker delta
45˚ 1199381perp
perpendicular space
119911
119906
1199382perp
1199383perp
1199384perp
45˚ 1199381∥
physical space
119909
119910
1199382∥
1199383∥
1199384∥
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
54
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
4-dim hyper-cubic lattice ℒ = 1198991ഥ1199381+ 1198992ഥ1199382+ 1198993ഥ1199383+ 1198994ഥ1199384
Hyper-grids in 4-dim hyper-space1st grids (1198991+ 1199041 )ഥ1199381 + 1205792ഥ1199382+ 1205793ഥ1199383+ 1205794ഥ11993842nd grids 1198992 + 1199042 ഥ1199382 + 1205791ഥ1199381+ 1205793ഥ1199383+ 1205794ഥ1199384
3rd grids (1198993+ 1199043 )ഥ1199383 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205794ഥ11993844th grids (1198994+ 1199044 )ഥ1199384 + 1205791ഥ1199381+ 1205792ഥ1199382+ 1205793ഥ1199383
2-dim grid lines (the physical-space sections of the hyper-grids)
1st grids 2(1198991 + 1199041 )1199381∥ + 1205791199383
∥
2nd grids 2(1198992 + 1199042 )1199382∥ + 1205791199384
∥
3rd grids 2(1198993 + 1199043 )1199383∥ + 1205791199381
∥
4th grids 2(1198994 + 1199044 )1199384∥ + 1205791199382
∥
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Dual-grid method ndash practice in 2 dims
(120579119895 free parameter)
(120579 free parameter)
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
55
Phason shifts
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
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Dual-grid method ndash practice in 2 dims
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
56
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
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Dual-grid method ndash practice in 2 dims
(x y 0 0)
1st grids
2nd grids
1198992 + 1
11989921198992minus 1
1198992+ 2
1198991 1198991+ 11198991 minus 11198991 minus 2
an intersection of grid lines
― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
57
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
(119909 119910 0 0 0) = (1198991+ 1199041)ത1198861+ (1198992+ 1199042)ത1198862 + 1205793ത1198863+ 1205794ത1198864
1205793 = ഥ1199443 119909 119910 0 0 = 1198993+ 1199043 + 120575 1198993 = 1205793minus 1199043 120575 = 119865119903119886119888(1205793minus 1199043)
1205794 = ഥ1199444 119909 119910 0 0 = 1198994 + 1199044+ 120575rsquo 1198994 = 1205794 minus 1199044 120575rsquo = 119865119903119886119888(1205794minus 1199044)
where ഥ119944119895 = ഥ119938119895 ( 119895 = 1 2 3 4) hellip 4-dim reciprocal basis vecs
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
These equations determine four integers 1198991 1198992 1198993 1198994 which provide the indices of the base points of the four 4-dim unit cells that contact each other at the intersection (xy) of the 1st and 2nd grid lines rarr
(similar formulas can be obtained foran intersection of ith and jth grid lines)
① (1198991 1198992 1198993 1198994 )
② (1198991minus 1 1198992 1198993 1198994)
③ 1198991 1198992minus 1 1198993 1198994④ (1198991minus 1 1198992minus 1 1198993 1198994 )
58
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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― 準周期構造の理論と基礎 ―
62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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― 準周期構造の理論と基礎 ―
63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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― 準周期構造の理論と基礎 ―5 Approximants
66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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― 準周期構造の理論と基礎 ―5 Approximants
70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
(x y 0 0)
②
③④
1198991
1198992
①
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Dual-grid method ndash practice in 2 dims
Ammann-Beenkertiling (8mm)
Each intersection of two grid lines gives one rhombus or
square in the tiling
59
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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― 準周期構造の理論と基礎 ―
64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Dual-grid method ndash practice in 2 dims
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
Ammann-Beenker tiling (in 2-dim physical space) Mapping the vertices of the tiling intothe orthogonal complement (2-dim)
Outer boundary (regular octagon) Projection of the 4-dim hyper-cubic unit cell into the 2-dim perpendicular space
60
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Perl scripts for constructing the rhombic Penrose tiling (P3) and the Ammann-Beenker tiling
Tilings encyclopedia
Book
httpwwwtagentohokuacjplabotsainobuhisaAmmannBeenker2povpl
httpwwwtagentohokuacjplabotsainobuhisaPenrose2povpl1199041 + 1199042+ 1199043 + 1199044+ 1199045 = integer rarr rhombic Penrose tiling (P3)1199041 + 1199042+ 1199043 + 1199044+ 1199045 = half integer rarr anti-Penrose tiling
Some resources on aperiodic tilings
httptilingsmathuni-bielefeldde
B Gruenbaum GC Shephard Tilings and Patterns W H Freeman and Company New York 1987 (Chapter 10)
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― 準周期構造の理論と基礎 ―4 Methods for generating QPTs
61
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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― 準周期構造の理論と基礎 ―5 Approximants
65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
5 Approximants[Cut-and-project method]
119909∥
119909perp
ഥ1199381 = 1 minus120783
120649 ഥ1199382 =
1
120591 1
Win
do
w
Fibonacci chain (without linear phason strain)
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62
L L L L L L L LS S S S S L S L L S L L S
5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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5 Approximants[Cut-and-project method]
119909∥
119909perp
32 approximant to Fibonacci chain
Phason strain119878 = Δℓ
L S L L S L L LL S L S S L S L L S L SWin
do
w
ഥ1199381 = 1 minus120784
120785 ഥ1199382 =
1
120591 1
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63
ℓ
Δ
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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― 準周期構造の理論と基礎 ―5 Approximants
69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
5 Approximants[Cut-and-project method]
119909∥
119909perp
53 approximant to Fibonacci chain
Phason strain119878 = Δℓ
Win
do
w
ഥ1199381 = 1 minus120785
120787 ഥ1199382 =
1
120591 1
L S L L S L LL S L S L S L L S L LL S
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64
ℓ
Δ
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Rational approximations of 120591
119865119899+1 = 119865119899 + 119865119899minus1 (1198650 = 0 1198651 = 1 1198652 = 1 1198653 = 2 1198654 = 3 1198655 = 5 1198656 = 8hellip )
120591 =1 + 5
2= 1 +
1
120591= 1 +
1
1 +1
1 +1
1 +1
1+
Continued fraction expansion of τ =1+ 5
2(golden mean)
120591 cong 1 +1
1 +1
1 +1
1 + 1
= 1 +1
1 +1
1 +11986521198653
= 1 +1
1 +11986531198654
= 1 +11986541198655
=11986561198655
Rational approximation of τ τ cong119865119899+1
119865119899
Fibonacci numbers
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65
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199385perp +
1
1205911199381perp + 1199384
perp = 120782 zminusdir
1199381perp minus 1199384
perp +1
120591(1199382
perp minus 1199383perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199381perp
1199382perp
1199383perp
1199384perp
1199385perp
5-dim basis vectors of the P3 tiling(with no linear phason strain)
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66
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
1199385||minus 120591(1199381
||+ 1199384
||) = 120782 xminusdirection
1199381||minus 1199384
||minus 120591(1199382
||minus 1199383
||) = 120782 yminusdir
physical space
1199381∥
1199382∥
1199383∥
1199384∥
1199385∥
119909
119910
1199395perp +
119902
1199011199391perp + 1199394
perp = 120782 zminusdir
1199391perp minus 1199394
perp +119904
119903(1199392
perp minus 1199393perp) = 120782 uminusdir
perpendicular space
119911
119907 119906
1199391perp
1199392perp
1199393perp
1199394perp
1199395perp
119901
119902119903
119904approximation
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― 準周期構造の理論と基礎 ―5 Approximants
5-dim basis vectors of an approximant(modified with a linear phason strain)
67
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
5-dim basis vectors of an approximant(modified with a linear phason strain)
1199381 =
1(2120591)
4120591 + 3(2120591)minus119901119904
1 2
1199382 =
minus1205912
3 minus 1205912119901 minus 119902minus119903
1 2
1199383 =
minus1205912
minus 3 minus 1205912119901 minus 119902119903
1 2
1199384 =
1(2120591)
minus 4120591 + 3(2120591)minus119901minus119904
1 2
1199385 =
1021199020
1 2
119938119895 =
119938119895||
119939119895perp
1 2
NB z and u axes are
arbitrarily scaled
119901
119902119903
119904approximation
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68
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Periodicity of 119901
119902119903
119904approximant
A general 5-dim lattice vector with indices ℎ1 ℎ2 ℎ3 ℎ4 ℎ5
rarr Perpendicular space components
ℎ11198871perp + ℎ21198872
perp + ℎ31198873perp + ℎ41198874
perp + ℎ51198875perp
=
2119902ℎ5 minus 119901ℎ1 + (119901 minus 119902)ℎ2 + (119901 minus 119902)ℎ3 minus 119901ℎ4119904ℎ1 minus 119903ℎ2 + 119903ℎ3 minus 119904ℎ4
(ℎ1 + ℎ2 + ℎ3 + ℎ4 + ℎ5) 2
Note that the 2-dim lattice basis vectors 1199291 and 1199292 of 119901
119902119903
119904
approximant along the 119909 and 119910 directions should in general be indexed as 119895 119896 119896 119895 119894 and 119897 119898minus119898minus119897 0 respectively
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69
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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79
Periodicity of 119901
119902119903
119904approximant
Their modified perpendicular space components would then be
1199291prime = 1198951198871
perp + 1198961198872perp + 1198961198873
perp + 1198951198874perp + 1198941198875
perp =
2119901 119896 minus 119895 minus 119902 119896 minus 119894 0
(119894 + 2119895 + 2119896) 2
1199292prime = 1198971198871
perp +1198981198872perp minus1198981198873
perp minus 1198971198874perp =
02(119904119897 minus 119903119898)
0
These perpendicular space components would vanish if 1199291 and 1199292 are the lattice bases of the approximant so that
119901
119902=119896 minus 119894
119896 minus 119895
119903
119904=
119897
119898 119894 + 2119895 + 2119896 = 0
(119894 minus 119896) + 2(119895 minus 119896) + 5119896 = 0
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70
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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72
How to generate an approximant with dual-grids
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73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Periodicity of 119901
119902119903
119904approximant
There exists non-zero integer 119899 such that
119894 minus 119896 = 119901119899 119895 minus 119896 = 119902119899 and5119896 = minus 119901 + 2119902 119899
Thus the values of 119894 119895 and 119896 are determined uniquely (up to a sign) according to the values of 119901 and 119902 and so are the values 119897 and 119898according to the values of 119903 and 119904 through
119897 = plusmn119903 119898 = plusmn119904
p+2qと5の最小公倍数を与えるようにnを決める
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― 準周期構造の理論と基礎 ―5 Approximants
71
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Periodicity of 119901
119902119903
119904approximant
Lattice basis vectors in the physical space
1199291 = 1198951199381||+ 1198961199382
||+ 1198961199383
||+ 1198951199384
||+ 1198941199385
||= 1199021198991199381
||+ 1199021198991199384
||+ 1199011198991199385
||
1199292 = 1199031199381||+ 1199041199382
||minus 1199041199383
||minus 1199031199384
||
The corresponding increments in the perpendicular space
1199291perp = 1198951199381
perp + 1198961199382perp + 1198961199383
perp + 1198951199384perp + 1198941199385
perp = 1199021198991199381perp + 1199021198991199384
perp + 1199011198991199385perp
1199292perp = 1199031199381
perp + 1199041199382perp minus 1199041199383
perp minus 1199031199384perp
The linear phason strain tensor 119878 (Definition 119961perp~119878119961∥)
1199291perp 1199292
perp = 119930 1199291 1199292
119930 = 1199291perp 1199292
perp 1199291 1199292minus1 NB) 119930 is a 3x2 matrix in the present case
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― 準周期構造の理論と基礎 ―5 Approximants
72
How to generate an approximant with dual-grids
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― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
How to generate an approximant with dual-grids
第一回新学術領域ハイパーマテリアル若手研究会Web開催2020528
― 準周期構造の理論と基礎 ―5 Approximants
73
Replace the hyper-cubic lattice basis vectors (ഥ119938119895 and ഥ119944119895)
into modified basis vectors (119938119895 and 119944119895) while performing
the dual-grid method (see p50)
ഥ119938119895 = 119938119895|| 119938119895
perp rarr 119938119895 = 119938119895|| 119939119895
perp
ഥ119944119895 (def ഥ119938119895 sdot ഥ119944119895 = 120633119894119895) rarr 119944119895 (def 119938119895 sdot 119944119895= 120633119894119895)
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Approximant No1
1199291
1199292
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
1
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
74
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Examples Approximant No2
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 119938120783+ 119938120784minus 119938120785minus 119938120786
1
1
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
75
1199291
1199292
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Examples Approximant No3
1199291 = 120784119938120783minus 120785119938120784minus 120785119938120785+ 120784119938120786+ 120784119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
1
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― 準周期構造の理論と基礎 ―5 Approximants
76
1199291
1199292
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
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― 準周期構造の理論と基礎 ―
79
Examples Approximant No4
1199291 = 119938120783minus 120786119938120784minus 120786119938120785+ 119938120786+ 120788119938120787
1199292 = 120784119938120783+ 119938120784minus 119938120785minus 120784119938120786
1
2
1
2
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― 準周期構造の理論と基礎 ―5 Approximants
77
1199291
1199292
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
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― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
第一回新学術領域ハイパーマテリアル若手研究会Web開催2020528
― 準周期構造の理論と基礎 ―
79
Approximant No5
1199291 = 120785119938120783minus 120789119938120784minus 120789119938120785+ 120785119938120786+ 120790119938120787
1199292 = 120785119938120783+ 120784119938120784minus 120784119938120785minus 120785119938120786
2
3
2
3
Examples
第一回新学術領域ハイパーマテリアル若手研究会Web開催2020528
― 準周期構造の理論と基礎 ―5 Approximants
78
1199291
1199292
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
第一回新学術領域ハイパーマテリアル若手研究会Web開催2020528
― 準周期構造の理論と基礎 ―
79
Exercises
a Compare approximant tilings generated with different values of phason shifts
b Apply the dual-grid method for generating Ammann-Beenker tiling (octagonal or 8-gonal QC)
c Generate a few simplest approximants to the Ammann-Beenker tiling
第一回新学術領域ハイパーマテリアル若手研究会Web開催2020528
― 準周期構造の理論と基礎 ―
79