Advanced Nuclear Physicshagino/lectures/nuclth18/...Contents Nuclear Many-Body Problems (Low-energy)...
Transcript of Advanced Nuclear Physicshagino/lectures/nuclth18/...Contents Nuclear Many-Body Problems (Low-energy)...
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Advanced Nuclear Physics
Nuclear Theory Group,Tohoku UniversityKouichi Hagino
原子核理論特論
東北大学原子核理論研究室萩野浩一
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Contents
Nuclear Many-Body Problems
(Low-energy) Nuclear Physics
to understand rich nature of atomic nuclei starting from nucleon-nucleon interactions
- size, mass, density, shape- excitations- decays- nuclear reactions
two kinds of particle: protons and neutrons
Nuclei: many-body systems of nucleons (protons and neutrons)
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Contents
Nuclear Many-Body Problems
Liquid drop modelSingle-particle motion and shell structureHartree-Fock approximationBruckner theoryPairing correlations and superfluid Nucleiphysics of neutron-rich nucleiRandom phase approximation (RPA)Nuclear reactions and superheavy elements
(physics of Nihonium)
this lecture: microscopic descriptions of atomic nuclei
Nuclei: many-body systems of nucleons (protons and neutrons)
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References
Bohr-Mottelson Ring-Schuck Rowe Frobrich-Lipperheide
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Lecture notes:
http://www.nucl.phys.tohoku.ac.jp/~hagino/lecture.html
(Tohoku University → Physics → Nuclear Theory→ Kouichi Hagino → Lectures)
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Introduction: atoms and atomic nuclei
~ 50 cm
~ 10-10 m
cellsDNA
~ 10-8 m
atom
Everything is made of atoms.
~ µm = 10-6 m
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Introduction: atoms and atomic nuclei
~ 50 cm
~ 10-10 m
cellsDNA
~ 10-8 m
atom
~ 10-15 m
atomic nucleus
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NuclearPhysics
Nucleus as a quantum many body system
charge mass (MeV) spin, parityProton +e 938.256 ½+
Neutron 0 939.550 ½+
Basic ingredients:
(note) n → p + e- + νe (10.4 min)
1 fm = 10-15 m
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protons
neutrons
Nucleons are not stopping inside a nucleus.(they move relatively freely)
a self-bound system
Yet, they are not completely independent.A nucleus keeps its shape while nucleons influence among themselves so that a nucleon does not escape.
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protons
neutrons
Nucleons are not stopping inside a nucleus.(they move relatively freely)
Yet, they are not completely independent.A nucleus keeps its shape while nucleons influence among themselves so that a nucleon does not escape.
a self-bound system
What happens if a photon is absorbed into a nucleus? - one nucleon simply starts moving faster?
photon
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protons
neutrons
Nucleons are not stopping inside a nucleus.(they move relatively freely)
Yet, they are not completely independent.A nucleus keeps its shape while nucleons influence among themselves so that a nucleon does not escape.
a self-bound system
What happens if a photon is absorbed into a nucleus? - one nucleon simply starts moving faster?
Very coherent motion can happen
Collective motions
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protons
neutrons
Nucleons are not stopping inside a nucleus.(they move relatively freely)
Yet, they are not completely independent.A nucleus keeps its shape while nucleons influence among themselves so that a nucleon does not escape.
a self-bound system
What happens if a photon is absorbed into a nucleus? - one nucleon simply starts moving faster?
Very coherent motion can happen
Collective motions
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a variety of motions→ very rich!
Very coherent motion can happen
Collective motions
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Nuclear Chart: 2D map of atomic nuclei
neutron number
proton number
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Periodic Table of elements (1869)
Mendeleev(1834-1907)
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タカとフジ(メンデレーエフの孫)
Periodic Table of elements (1869)
Mendeleev(1834-1907)
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Periodic Table of elements (1869)protons only, no information on neutrons
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Nuclear Chart: an extended version of periodic table
neutron number
proton number isotopes
16O (Z=8, N=8, A=16)17O (Z=8, N=9, A=17)18O (Z=8, N=10, A=18)
A=Z+N
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neutron number
proton number
・Stable nuclei in nature: 287 ・Nuclei artificially synthesized :about 3,000・Nuclei predicted:about 7,000 ~ 10,000
Nuclear Physics: Several static and dynamical propertiesof those nuclei
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neutron number
proton number how many neutrons can be attached?
what is the shape of nuclei?is there any exotic structure? what is the heaviest nucleus? how do nuclei decay?….. etc. etc.
Nuclear Chart: an extended version of periodic table
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Extension of nuclear chart: frontier of nuclear physics
neutron-rich nuclei (RIBF)
halo nuclei
superheavy elements
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Neutron-rich nuclei (RIBF at RIKEN)
r-process nucleosynthesis
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2017年10月17日朝日新聞
NAOJ B.P. Abbott et al., PRL119 (‘17) 161101このときに元素合成が?
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重力波源から来た電磁波(の時間変化)
実線:r-プロセスが起こった場合
破線:起こらなかった場合
http://www.cfca.nao.ac.jp/pr/20171016
M. Tanaka et al.,Astron. Soc. Jpn. 69 (‘17) 102
2017年10月17日朝日新聞
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Prediction of island of stability: an important motivation of SHE study
Yuri Oganessianisland of stability around Z=114, N=184W.D. Myers and W.J. Swiatecki (1966), A. Sobiczewski et al. (1966)
modern calculations: Z=114,120, or 126, N=184 e.g., H. Koura et al. (2005)
nuclei in nature
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neutron number
proton number how many neutrons can be attached?
what is the shape of nuclei?is there any exotic structure? what is the heaviest nucleus? how do nuclei decay?….. etc. etc.
Nuclear Chart: an extended version of periodic table
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a nucleus is not always spherical
Quantum shape dynamics
「形の量子論」
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Density Distribution
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Density Distribution High energy electron scattering
Born approximation:
(Fourier transform of the density)
Form factor
e-
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Born approximation
θV(r)
incident flux:
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Electron scattering
Form factor
e- e-
* relativistic correction:
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Fermi distribution
(fm-3)(fm)
(fm)
Saturationproperty
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Momentum Distribution
Fermi gas approximation
kx
ky
kz
Fermi energy: (MeV)
(note: spin-isospin degeneracy)
ρ = 0.17 fm-3 kF ~ 1.36 fm-1
kF
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V
陽子 中性子
~ 40 MeV(フェルミ近似より)
~ 8.5 MeV(実験データより)
~ 48.5 MeV
原子核の中で核子が感じるポテンシャル
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Nuclear Mass
B(binding energy)
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B(N,Z)/A ~ 8.5 MeV (A > 12) Short range nuclear force
a long range interaction: → B/A ~ A
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if each nucleon can interact only α-nucleons close by:
A
B/A
B ~ α A/2 B/A ~ α/2 (const.)
rint
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if each nucleon can interact only α-nucleons close by:
A
B/A
B ~ α A/2 B/A ~ α/2 (const.)
rint rint
a small nucleus
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if each nucleon can interact only α-nucleons close by:
B ~ α A/2 B/A ~ α/2 (const.)
rint rint
a small nucleus
A
B/A
α+1
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rint
A
B/A
α+1
rint
nuclear interactionCoulomb interaction
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rintrint
nuclear interactionCoulomb interaction
A
B/A
Coulombcorrection
a peak
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1. B(N,Z)/A ~ 8.5 MeV (A > 12) Short range nuclear force2. Effect of Coulomb force for heavy nuclei
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Nuclear Chart
Stable nuclei:
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1. B(N,Z)/A ~ -8.5 MeV (A > 12) Short range nuclear force2. Effect of Coulomb force for heavy nuclei3. Fusion for light nuclei4. Fission for heavy nuclei
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(Bethe-Weizacker formula: Liquid-drop model)
Volume energy:
Surface energy:
Semi-empirical mass formula
Coulomb energy:
Symmetry energy:
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How well does the Bethe-Weizacker formula reproduce the data?
not so bad
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cf. N,Z = 2, 8, 20, 28, 50, 82, 126: large binding energy“magic numbers”
How well does the Bethe-Weizacker formula reproduce the data?
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(note) Atomic magic numbers (Noble gas)He (Z=2), Ne (Z=10), Ar (Z=18), Kr (Z=36), Xe (Z=54), Rn (Z=86)
shell structure
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level density
uniform non-uniform
Why do closed-shell-nuclei become stable?
smaller total energy(more stable)