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Computational Studies on High Temperature …ipc/meetipc/pdf/seminar_kuroki.pdfHigh Temperature...
Transcript of Computational Studies on High Temperature …ipc/meetipc/pdf/seminar_kuroki.pdfHigh Temperature...
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Computational Studies on High Temperature Superconductivity
The University of Electro-Communications Kazuhiko Kuroki
Osaka University, IPC Advanced Seminar 2011.12.16
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Superconductivity occurs at very low temperature
Disappearance of resistivity below a certain temperature Tc : superconducting transition temperature
What is superconductivity ?
First discovered by Kamerlingh Onnes In Mercury in 1911 this year 2011 marks the 1st centennial of the discovery of superconductivity
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http://sakaki.issp.u-tokyo.ac.jp/user/kittaka/contents/others/tc-history.html
「銅系」
「鉄系」
History of the highest Tc
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http://sakaki.issp.u-tokyo.ac.jp/user/kittaka/contents/others/tc-history.html
As Fe
La O
cuprates
「鉄系」
Discovery of “high Tc” superconductivity
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http://sakaki.issp.u-tokyo.ac.jp/user/kittaka/contents/others/tc-history.html
As Fe
La O
cuprates
Iron pnictides
Discovery of “high Tc” superconductivity
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Atoms
nucleous
atomic orbitals
atom
electrons
orbitals
s
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Solids solid(crystal)
electron kinetic energy
electron-electron interaction
lattice vibration = phonons
electron- phonon interaction
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Necessity of Model Hamiltonian
kinetic energy of electrons =complicated band structure
Model Hamiltonian : consider only essential bands near the Fermi level, also simplify the electron-electron and/or electron-phonon interactions
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reciprocal lattice momentum space real space lattice
wave number : k=2π/λ
p=hk
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square lattice
triangular lattice
real space reciprocal space
real space reciprocal space
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Energy band, Fermi sea, Fermi surface
µ, EF : Fermi energy, chemical potential constant energy surface with E(k)= EF :
Electrons : Fermions In the ground state (T=0), the electrons are filled from the bottom of the band up to the Fermi energy.
Fermi surface of free electron gas is a sphere
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Fermi distribution function
average number of electrons occuping a single state with energy ε at temperature T
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Tightbinding models
“site”
electron with up spin
electron with down spin
“hopping integral”
In 1D
In 2D
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creation, annihilation operators in real space
number representation
anticommutation relation of Fermion operators
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Tight binding model expressed in second quantization form
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creation, annihilation operators in momentum space
band dispersion
the number of k’s =the number o sites (# of unit cells)
“diagonal” ; number operator in momentum space
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Grand partition function and Fermi’s distribution function
=
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Tight binding model on a square lattice
when only the nearest neighbor hopping is considered :
When there are M sites in a unit cell, and each site contains L orbitals, it is a ML band model
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Fermi surface
Fermi surface at half-filling
Fermi surface is “well nested” when it has a large overlap with the one translated by a certain “nesting vector Q”
filled
empty
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Effect of distant hoppings Fermi surface for band filling n=0.85
t’/t =-0.2
t’/t =-0.45 flattening of the band
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Tightbinding model band dispersion on various lattices
square lattice triangular
honeycomb
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or
Introduction of electron-electron interaction number operator
Hamiltonian in real space
Hamiltonian in momentum space
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most straight forward way : exact diagonalization of the Hamiltonian matrix
Difficulty in solving a many body problem
basis to obtain H matrix :
For instance, for a 20 site system with 10 up spin and 10 down spin electrons, the number of basis is (20C10)2 ~ 3 x 1010 diagonalization of ~1010 × 1010 matrix is necessary ! (for only 20 sites<< 1023)
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electron-phonon interaction
Theory of conventional superconductivity : phonon-mediated pairing and BCS theory
“Feynman diagrams”
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electron-electron effective interaction mediated by phonons
V is called the pairing interaction rewrite H-µN as H
extract the interaction of the form
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mean field approximation
Then the Hamiltonian is approximated as
where
“order parameter”, “gap function”
not diagonal
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Bogoliubov transformation : creation, annhilation operators of “quasiparticles”
required for anticommutation relation
Expressing the Hamiltonian in terms of α, α, and enforcing
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: ground state
: ground state energy
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since the “quasiparticles” are “free particles”
this gives
Then, from the definition of ∆
This is an equation that self-consistently determines ∆ :
“gap equation”
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gives the dispersion of the excitation of quasiparticles there is a gap around ξ=0 , the ground state is protected by the gap
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superconductivity occurs due to pair scattering
V (k-k’): pairing interaction pair scattering
( ) ( ) ( ) 0V − ∆ ∆ <k k' k k'
tanh[ ( ) / ]( ) ( ) ( )2 ( )
BE k T VE
∆ = − − ∆∑k'
k'k k k' k'k'
gap equation
In order to have a finite ∆
V
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tanh[ ( ) / ]( ) ( ) ( )2 ( )
Bk T Vελε
∆ = − − ∆∑k'
k'k k k' k'k'
λ
Tc T
Linearized gap equation : neglect O(∆2) or T~Tc
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if V(q)=constant,
tanh[ ( ) / ]( ) ( ) ( )2 ( )
BE k T VE
∆ = − − ∆∑k'
k'k k k' k'k'
shows that ∆ is independent of k
This means that finite ∆ is obtained only when V<0 : attractive interaction phonon mediated interaction satisfies the condition
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assuming that V is small, Tc is approximately given as,
ωD is the maximum frequency of the phonons, usually is O(100K)
is the density of states at the Fermi energy, usually
for strong coupling superconductors with further analysis have shown that the upper bound for Tc is few 10K
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antiferromagnetic spin ordering in the parent, undoped compound
Cuprate high Tc superconductors
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Properties of the cuprates and possibility of unconventional superconductivity
necessity of purely electronic model Hamiltonian
Tc beyond 100K
superconductivity near antiferromagnetism
strong electron correlation
d-wave pairing
phonon mediated Cooper pairing is unlikely
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Crystal field effect
t2g
eg
x2-y2
3z2-r2
xy
yz, zx cubic (regular octahedron) Tetragonal
(elongated octahedron)
La(+3)2-x Sr(+2)x Cu(+2+x) O(-2)4 : partially replacing La by Sr induces holes in Cu dx2-y2 orbital
La(+3)2 Cu(+2) O(-2)4 :undoped parent compound, d 9
lift of degeneracy of 3d orbitals due to crystal field
atom
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dp model
three sites per unit cell, each site has one orbital = three band model
considers Cu3dx2-y2 and O2p orbitals that can hybridize with Cu3dx2-y2
strongly 3d with some mixture of 2p
strongly 2p with some mixture of 3d
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Single band Hubbard model
consider only the band that intersects the Fermi level
single band model = single site per unit cell one orbital per site
t~0.4eV, U~8t
undoped parent compound = one electron / site =band filling (n) =1
on-site interaction
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Mott insulating state and antiferromagnetism half-filled(undoped case)
Electrons are localized due to the on-site U : Mott insulator In order to gain kinetic energy : antiferromagnetic spin ordering
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Many body techniques
Quantum Monte Carlo method for finite size clusters ( up to O(100~1000) sites)
Diagrammatic approach
Combination
auxiliary field QMC
variational Monte Carlo
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,
1 ( 1)N
i ji j
i jS S
N−− ⋅∑
White et al.Phys Rev.B40(1989) 506
spin correlation function
Spin correlation function calculated by AFQMC
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Cooper pairing due to repulsive interaction ???
tanh[ ( ) / ]( ) ( ) ( )2 ( )
BE k T VE
∆ = − − ∆∑k'
k'k k k' k'k'
gap equation
U >0
=
this equation obviously does not have a finite gap solution
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+ + … U U U
=
effective pairing interaction
collect contributions from certain types of diagrams
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bare susceptibility
spin and charge susceptibilities (in random phase approximation)
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Magnetic (spin) susceptibility
spin susceptibility without electron-electron interaction at ω=0
RPA spin susceptibility with electron-electron interaction U
expression is valid for
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for a fixed U, the divergence can occur by lowering the temperature ; can increase at certain wave vectors at low temperatures
as
at a certain wavevector q=Q where is maximized
magnetization for inifinitesimaly small magnetic field divergence of the susceptibility signals spontaneous ordering of spins
Ideal square lattice, Fermi surface at half-filling : strongly nested
filled
empty
is large at the nesting vector q=Q when f is close to a step function
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sponteneous spin ordering (antiferromagnetism) with a wave vector Q can take place at low temperature when the Fermi surface is strongly nested
even when the Fermi surface nesting is degraded (by carrier doping for instance), large (spin fluctuations) remains
( ) ( ) ( ) 0V − ∆ ∆ <k k' k k'
pairing int. mediated by spin fluctuation at q=Q SC gap ∆ (k)= −∆ (k+Q) d-wave pairing
large
condition for SC :
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d-wave SC on square lattice
Bickers et al, PRB 43 (1991) 8044
dx2-y2-wave SC Tc~O(0.01t)
calculate the pairing interaction and solve the gap equation for O(1000)~O(10000) lattice sites
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Yokoyama, Tanaka, Ogata, Tsuchiura JPSJ 73 (2004) 1119
energy gain due to d-wave superconductivity Variational Monte Carlo (VMC)
T.A. Maier et al, PRL 95 (2005) 237001
inversed SC susceptibility by Dynamical Cluster Approximatoin (DCA)
U=8
Other approaches for d-wave superconductivity in the Hubbard model
dx2-y2-wave SC Tc~O(0.01t)
Tc =O(10)K~100K
high Tc, but still “low Tc” compared to the energy scale of t (kinetic energy of electrons)
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U = 8, ty = 1, tx2 = 1.2 in units of tx1 KK and R. Arita, PRB 2001,2002 Bulut et al PRB 1992 Maier & Scalapino arXiv:11070401
Q Q
HTC spin fluctuation mediated pairing from disconnected Fermi surfaces : single orbital case
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Discovery of SC in LaFeAsO
As
Fe
La
O
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High Tc up to 55 K by La->Sm,Nd
room T
liq N
Tc (K)
liq 4He
year 2008
LaFeAsOF
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Possible unconventional pairing
X.F. Wang et al
H. Mukuda et al magnetism near superconductivity
no coherence peak, NQR
First principles calculation : electron phonon coupling too weak for Tc=50K
Boeri et al
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Material dependence of Tc in iron pnictides
C.H. Lee et al, JPSJ 77 (2008) 083704
LaFePO
La
Nd
Tb
also by J. Zhao, Nat. Mat. 7, 953 (2008)
regular tetrahedron
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Material dependence of SC gap a number of experiments suggest fully open gap (with multiple gaps or anisotropy) for the arsenides,
Hashimoto et al, penetration depth PrFeAsO
Ding et al, Ba122, ARPES
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Material dependence of SC gap for LaFePO (Tc~5K), experiments show presence of line nodes in the SC gap
Fletcher et al, PRL 102, 147001 (2009)
also Hicks et al., PRL 2009
thermal conductivity in magnetic field
M. Yamashita et al., PRB 2010
penetration depth
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Material Specific Hamiltonian for studying unconventional SC
material specific tight binding model
Superconductivity
electron-electron interaction
+
lattice structure, elements
Fermi surface multiplicity, shape, orbital weights
first principles band calculation ( pwscf, Wien2K) maximally localized Wannier orbitals (wannier90)
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Five orbital model
hole electron
hole
electron
all five iron 3d orbitals are necessary to correctly reproduce the band structure and the Fermi surface
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Fermi surface nesting and “s±” SC
two types of (π,0) spin fluctuations originating from different orbitals cooperating
pairing int. mediated by spin fluctuation at q=Q SC gap ∆ (k)= −∆ (k+Q)
fully gaped “s±” Mazin et al PRL 2008
+
+ −
−
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low high
KK et al., PRB 79 (2009) 224511
xy
xy z2
z2
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i, j: site、m,n: orbitals
Effective Hamiltonian
apply multi-orbital random phase approximation : typically, ~50×50×10 sites × 5 orbitals ~ 104 ~ 105 orbitals
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high
Mazin, Nomura, Ikeda, Wang, KK, Chubukov, Ji, Daghofer….
low
Graser et al. Mishra et al. KK et al. Wang et al. Thomale et al
KK et al., Graser et al, Yanagi Ikeda&Arita…
pnictogen height dependent sc gap
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λ at a fixed T can used as a qualitative measure for Tc
Linearized gap equation
λ
T
case A
case B
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“Height” as a switch between high Tc nodeless and low Tc nodal pairings
low Tc nodal
high Tc nodeless
U=1.2, U’=0.9, J=J’=0.15 n=6.1 (10% dope) T=0.02 (eV)
KK et al., PRB 79 (2009) 224511
Nd
La P
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Bond angle dependence of Fermi surface multiplicity
H. Usui and KK, PRB 84 (2010) 024505
2
3
2
FS for 10% doping
Fe-As bond length= fixed
This kind of Fermi surface variation first found in T. Miyake et al, JPSJ 79 (2010) 123713
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C.H. Lee et al, JPSJ 77 (2008) 083704
LaFePO
La
Nd
Dy
Bond angle dependence of SC
T=0.005eV Sm
H. Usui and KK, PRB 84 (2010) 024505
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La2CuO4 (Tc~40K) HgBa2CuO4(Tc~90K) low high
Single layer system
La Hg
Material dependence of Tc in cuprates
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stronger Fermi surface roundness (“larger t’ ”) higher Tc
E. Pavarini, et al, PRL 87.047003(2001) K. Tanaka, et al, PRB 70.092503(2004)
Fermi surface shape and Tc
't
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'tE. Pavarini, et al, PRL 87.047003(2001)
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Fermi surface shape and Tc : theory
stronger Fermi surface roundness lower Tc microscopic theories for Hubbard type models
t-J model or large U Hubbard model; larger t’ favorable for superconductivity C.T. Shih et al 2004, P. Prelovsek&A. Ramsak 2005 , H.Yokoyama and M.Ogata
FLEX, single band Hubbard
DCA for d-p model Kent et al, 2008 Tc La > Hg ( for all hoppings)
SCR theory : explains material dependence T.Moriya & K. Ueda 1994
inversed SC susceptibility
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Γ Γ Γ Γ
La Hg
width of Green line:strength of dz2 orbital character
dx2-y2 +dz2 two orbital model importance of the dz2 orbital: H. Kamimura et al 1990, C.DiCastro 1991 O.K.Andersen et al J. Phys. Chem. Solids 1995, E.Pavarini et al PRL 2001
Sakakibara et al, PRL 105 (2010) 057003
“dx2-y2”=Cudx2-y2+Opσ
“dz2”=Cudz2+Opz
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Energy level diagram
2 2 2on site on sitex y z
E E E− −−
∆ = −
2 2" "x y
d−
2Cuz
dO zp
2" "z
dOpσ
2 2Cux y
d−
measures the contribution of the dz2 orbital to the Fermi surface
E∆
present model
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Correlation between Tc and ∆E
La
essentially single orbital
Sakakibara et al, 2010
vary ∆E directly “by hand” in the two orbital model of La214
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U = 8, ty = 1, tx2 = 1.2 in units of tx1 KK and R. Arita, PRB 2001,2002 Bulut et al PRB 1992 Maier & Scalapino arXiv:11070401
Q Q
HTC spin fluctuation mediated pairing from disconnected Fermi surfaces : single orbital case
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Maier & Scalapino arXiv:11070401
Dynamical Cluster Approximation
room temperature SC possible ??
SC susceptibility