Hidden d-waveO ital Tplet behindHidden d-waveO ital T plet behind s±Superconductivity T. TzenOng,...
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Hidden d-wave Orbital Triplet behind
s± Superconductivity
T. Tzen Ong, Joerg Schmalian, Piers ColemanCenter for Materials Theory, Department of Physics & Astronomy Rutgers University
Institute for Theory of Condensed Matter, Karlsruhe Institute of Technology
T. Tzen Ong & P. Coleman, arXiv:1303.6325, T. Tzen Ong, P. Coleman & Joerg Schmalian, In preparation
ΓM
� � � = 0 � � � = 4
�� � d-wave
orbital triplet!
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• Coulomb repulsion -> Higher angular
momentum superconducting states
•3He-B with spin-orbit coupling
• Orbital helicity in Fe-SC band structure
• Hidden d-wave orbital triplet in Fe-based SCs
�� � � �� ������������ �
• Experimental consequences & Open Issues
Outline
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Phase Diagram of Fe-Based SuperconductorsCoulomb Repulsion & SC Order Parameter!
Nodeless Nodal
⟨�↓�↑⟩ � � �� ����� = 0
Cuprates
FeSe
Fe-Based SCs
Ba0.6K0.4Fe2As2
• Coulomb repulsion -> higher angular momentum SC states with
nodes
• Cuprates, ruthenates, heavy fermion SCs, 3He-B
Fe-SCs are exceptional ?
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� ARPES shows an isotropic
gap at Z
� Rules out d-wave
superconducting order
parameter!
X.P. Wang and H. Ding et. al. EPL 99, 67001, (2012)
T. Qian and H. Ding et. al. PRL 106, 187001, (2011)
Fully Gapped State in Electron Pocket System
� Fully gapped SC
state, Tc = 55K
� Electron pockets
only.
Single layer FeSe
D. Liu et. al. Nat. Commun., 3, 931,(2012)
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Lines Nodes in Hole-Doped KFe2As2
Reid, Taillefer et. al., PRL 109, 087001, (2012)
Tafti, Taillefer et. al., Nat. Phys. 9, 349 (2013)
Finite thermal
conductivity →Line nodes with
nodal quasi-
particles
dxy-wave or
octet structures± superconductor
Naturally implies d-wave state
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Octet Structure in Hole-Doped KFe2As2
Okazaki, Shin et. al., Science 337, 1314 (2012)
• Competition
between s-wave
and d-wave?
• Or higher angular
momentum SC
state → Octet
structure from
ARPES!
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3He-B
!"# � ∑ Δc',)*+ , -./. � -0/0 1/23)456+,4*
-./.
-0/0 �� Fully-gapped p-wave
superfluid and minimizes
on-site repulsion!
Superfluid O.P rotates in
k-space:
�� � �7�8
Topological invariant:
9 � � :-2< :=+ > ?:=+ � 1
�
ΓEF
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Spin-Orbit Coupling
AB � �CΓ
AB � C
D�:Helicity vector
H"G �H5+*I J > - ⋅ /=5++
• Helical basis, MN � O+ ⋅ /= � �1
• Spin-orbit field couples orbital
angular momentum and spin
• P � Q � R
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H"# �H5+)* Δ:=+ ⋅ /=)456+4*+
� !. T.
��
3He-B with Spin-Orbit Coupling
H"G �H5+*I J > - ⋅ /=5++
U � � � V � W
��
D�Γ
Spin-orbit field couples Q � RO+ and :=+ have
same helicity
→ � � XYZ,AB3
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Γ
U � � � V � �
+
-
+
-
O+ and :=+ have
opposite helicity
→ � � [ \]^_
Reduces repulsion
@ cost of
condensation energy
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� Coulomb repulsion -> Higher angular
momentum superconducting states
• Are Fe-based SCs an exception?
� 3He-B with spin-orbit coupling
• Q � R � 0 → s± in helical basis
• Q � R � 2 → d-wave in helical basis
• Orbital helicity in Fe-SC band structure
• Hidden d-wave orbital triplet in Fe-based SCs
• Q � a � 0 → low-spin s± state
• Q � a � 4 → high-spin octet state
• QPT from low-spin to high-spin SC state?
• Experimental consequences & Open Issues
Outline
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• Crystalline Symmetry – Introduces new internal orbital
iso-spin degrees of freedom ( )
Internal Orbital Iso-Spin
c�d → c��d
Orbital Rashba coupling :
Inter-orbital hopping leads to coupling between kinetic
orbital motion and internal orbital iso-spin
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Orbital Rashba Field
• Orbital Rashba field : Coupling between kinetic angular
momentum (�) and atomic orbital iso-spin (�).
– U= � � � �– analogous to spin-orbit Rashba coupling.
• Kinetic Hamiltonian:
eW �Hc�,�,d* f� � C � g� ⋅ � c�,�h,d�
• g� � f78 � , W, f7�68�,�3 ≡ g�D�• Pauli matrices in orbital iso-spin space, � Helicity vector
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Orbital Helicity
�j � f� � � �kD � g�• Orbital helical basis. Hole pocket: a � 1, Electron pockets: a � �1
– Hole and electron pocket quasi-particles, l+m and n+m.
Ran, Lee et. al., PRB 79, 014505 (2009)
��,d*
��,d*
Γ
• Quasi-particles: linear superposition of
xz and yz orbitals.
• l+m � �+ 5+, .�,m � I+ 5+, 0�,m
• n+m � �+ 5+, 0�,m I+ 5+, .�,m
D�
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s± Superconductivity in Band Basis
• !"# � Δ ∑ l+↑*
l6+↓*
+ n+↑*
n6+↓*
� !. T.
• !"# � Δ ∑ 5+ )↑*
�+2 I+
2 aN � 2 �+I+a� 56+ )h↓
*+ � H.C.
• l+m � �+ 5+, .�,m � I+ 5+, 0�,m
• n+m � �+ 5+, 0�,m I+ 5+, .�,m
• Quasi-particles coherence factors, �+ and I+have d-wave form
factors
�� �d-wave Orbital Triplet!
� C�∑ c��d* �7�68� �B� �78�C ,�d�3c6��hdh*
� �H.C.
Orbital Basis = d-wave Orbital Triplet!
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Orbital Triplet Superconductivity with
Orbital Rashba Coupling
e �H��,�,d* f� � C�B � g� ⋅ � � �� ⋅ ��C ��,�h,d�
Helicity:Helicity:Helicity:Helicity:���
���� > �j�� ≡ � � ��
��� c���
Δ.�60� a�
Δ.0aN
�
Superconducting��-vector:
�+ ≡
Δ.�60�
0Δ.0
• Balian-Werthammerspinor:
�+,),m ≡ 5+,),m , 1a21/2 5+,),m* �
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In-Phase Rotation = s± Superconductivity
Γ
M
• U= � � � � � W• Low angular momentum
state = s±
� � ��
D��
��x2-y2
xy
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Octet Structure in KFe2As2
Okazaki, Shin et. al., Science 337, 1314 (2012)
� ∼ �����
��D�
� � �
�� and D� out-of-phase -> High angular momentum SC
state : U= � � � � � �
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t0 = 1.0, t1 = 0.15, t3 = 0.7, t4 = 0.7, µ = -4.0, ∆xy = 0.5, ∆x2-y2 = -0.25
Electron Pocket System
��D�
� � �
Γ
M
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Excited Cooper pairs with reverse chirality
Raman Active Modes
A1g Leggett
mode
2Δ
• Gapless Leggett mode
at QPT between low-
spin and high-spin SC
state!
Octet SC state s± superconductor
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• �� � d-wave orbital triplet SC state
– Orbital helicity of band structure
• Low-spin state = Fully gapped �� SC states
• High-spin state
– Fully gapped state in el-system
– Octet SC gap in hole systems
• Experimental consequences
– Raman active modes
– Gapless Leggett mode at QPT
– Topological invariant of d-vector
Conclusion
ΓM
T. Tzen Ong & P. Coleman, arXiv:1303.6325
T. Tzen Ong, P. Coleman & Joerg Schmalian, In preparation