the hubbard model in cold atoms and in the high-tc...
TRANSCRIPT
Daniel E. Sheehy
The Hubbard model in cold atomsand in the high-Tc cuprates
“What are the key outstanding problems from condensed matter physics whichultracold atoms and molecules can address?”
Aspen, June 2009
• Recently: Fermion Hubbard model in cold atom exp’ts Jordens et al Nature 2008, Schneider et al Science 2008
doping xAF SC
T
PG FL
T*
Tc
TNMFL
• Key Outstanding problem: Normal phase of cuprates
Pseudogap state ofunderdoped cuprates Optimal doping:
Marginal Fermi liquid
Quantum critical point?
Emergent particle-hole symmetry?
Meinders et al PRB 1993Honma & Hor PRB 2008Chakraborty et al 0807.2854
Outline
• Cuprate high-Tc superconductors: 2D Hubbard model
Neglects a lot of stuff!
BSCCO-2212
Bond ordered state inpseudogap state?
Kohsaka et al Nature 2008Macridin & Jarrell PRB 2008
Next: Cuprates
One e- per Cu
“half-filled”: Pauliwould allow 2 e-/site
Next: Hubbard Model
Cuprate high-Tc superconductors
YBCOCopper-oxygen planes (1,2,or 3)
other stuff
Cu CuO
Cu
O
O Cu
O
• Physics of SC: CuO planes
– Layers: copper-oxygen planes
• cuprates are layered
Hubbard model
t: Hopping matrix element between sites
U>0: Model Coulomb repulsion
!! "#><
++$=i
iiji
ijji nnUcccctH%
%%%%,,
)( † †
!!! jiiccn =
†nearest neighbor
P.W. Anderson, The theory of superconductivity in the high-Tc cuprates
• Question: What physics of the cuprates is captured by the Hubbard model?Answer: Noone knows
Cold atoms in optical lattices: Direct realizationSuperfluid-Mott transition of bosons:
Jaksch et al PRL 1998, Fisher et al 1989
Repulsive fermions:Hofstetter et al PRL 2002
Greiner et al Nature 2001; Spielman et al PRL 2007
Jordens et al Nature 2008, Schneider et al Science 2008…
Next: AF state
• One fermion per site– band theory: metal
Mott insulator
Half filling: Antiferromagnetic Mott insulator
!
U >> t– Large : No double occupancy!
• Antiferromagnetic order?Aligned spins:no virtual hops
AF alignment:virtual hops OK
Map to Heisenberg AF
!
H = J Si "< i, j>
# S j
Auerbach, “Interacting electronsand quantum magnetism”
!
J ~ t2/U
Next: cuprate phase diagram
• Quantitatively accurate at half filling (“parent compound”)– e.g., Birgeneau et al PRB 1999
Spin correlations above AF transition
X=0: AntiferromagnetWell understood!!
X~0.05: d-wave SC below Tc
++
-
-
!
px
!
py
Momentum-space Fermi surface:d-wave gap
Optimal Doping: x~0.2
Underdoped cuprates: Pseudogap behavior below T*
Hole concentration
Phase diagram of the hole-doped cuprates
Schematic!
doping xAF SC
T
PG FL
T*
Tc
TNMFL
Review: Norman and Pepin cond-mat/0302347
Marginal Fermi liquid: Unusual behaviorat optimal doping
Fermi liquid
Next: Pseudogap
Tc = 83K
Lowest T: no low-energytunneling
Cooper pair binding
!
2"
Highest T curve: tunnelingno problem
Where is the onset ofsuperconductivity?
What is the Pseudogap?• Numerous Exp’ts: Strong correlations above Tc Suppression of
low-energy states
Renner et al PRL 1998
BiSrCaCuO Tunneling: Inject electrons
into SC
SC
• Pseudogap: How to observe in cold-atom experiments?
RF spectroscopy, Photoemission (Stewart Nature 2008) Next: Scenarios
Pseudogap scenarios
doping xAF SC
T
PG FL
T*
Tc
TNMFL
Why is T* so large?
• Onset of order below T*
-d-density wave (Chakravarty et al PRB 2001)
-current loop order (Aji et al PRB 2008)
-bond order (Macridin et al PRB 2008)
– Next: Bond order
Has not been observed!
Why would an ordered phase be unstable to superdonductivity?
• Pairing above Tc - phase fluctuations (Emery + Kivelson Nature 95 , Franz and Tesanovic, PRL 01)
- BEC-BCS crossover (Maly et al PRB 96)
Nearest neighbor singlet correlations
!
1
2"# $ #"( )
• Scanning tunneling in pseudogap
Kohsaka et al Nature 2008
Anderson, Sachdev, …
Bond order• Exotic magnetic order: Valence bond
Broken rotational symmetry
– Next: Quantum critical point
Recent Dynamical Mean Field resultsMacridin et al PRB 2008
Similar bond-ordered phases
• Pseudogap: Subtle ordering
Quantum critical point scenarioTallon + Loram cond-mat/0005063Sachdev Science 2000Orenstein & Millis Science 2000
e.g., d-density wave, current loop order, valence bond order…
Heavy-fermionSC CePd2Si2
AF fluctuations mediate SC Mathur et al Nature 1998
Next: Marginal FL/”Strange metal”
• Strong fluctuations mediate SC?
• Terminates at a quantum critical point?
Under “dome” near optimal doping!
doping xAF SC
T
PG FL
T*
Tc
TNMFL
– Enlarged symmetry– Lack of energy scale– Marginal Fermi liquid
doping xAF SC
T
PG FL
T*
Tc
TNMFL
E.g., T-linear in-plane resistivity:
Strange metal/Marginal Fermi liquidAnomalous temperature dependencies at optimal doping
Ando et al, PRL 2004
Exactly linear at optimal doping
Deviations from linearity inunderdoped region (pseudogap)
Varma et al PRL 1989
Next: Quantum critical point
Matsuura PRB 1992
Next: Can the Hubbard model capture this?
Honma and Hor, PRB 2008
Universal vanishing of thermopower at optimal doping!
Evidence for Quantum Critical point: ThermopowerThermopower: Voltage drop under an applied temperature difference
!
S = "#V
#T
Chakraborty et al 0807.2854
Hubbard model Thermopower Beni PRB 1974Lewis PRB 1976Mukerjee PRB 1995
• Hubbard model in the atomic limit:
!! "#><
++$=i
iiji
ijji nnUcccctH%
%%%%,,
)( † †
!
t" 0 (no hopping, strong coupling)
• Thermopower:
!
S" ln1# x
2x
Vanishes at xc=1/3!
• Vanishing thermopower: Particle-hole symmetry Entropy carried by particles or holes?
• Idea: Thermopower data implies emergent particle-hole symmetry at optimal dopingChakraborty et al 0807.2854
– Away from atomic limit: – How can we test this scenario in cold-atom experiments?
xc<1/3
Next: Why p-h symmetry?
• Dynamical mean-field theory: Particle-hole symmetry at
!
x " 0.2
Vidhyadhiraja PRL 2009
• Dope 1 hole
Lower Hubbard band:Filled
Upper Hubbard band:Empty
Single-particle density of states
UN statesN states
Energy
Spectral Weight Transfer • Half filling
Meinders et al PRB 1993Chakraborty et al 0807.2854
(Still in atomic limit!)
Hole doping: Introduction of low energy excitations
UN-1 states N-1 states
2 states
!
µ
!
(",#)
Next: Dope more holes…
Energy
Spectral Weight Transfer 2 Meinders et al PRB 1993Chakraborty et al 0807.2854
• Dope xN holes? x=fraction of sites with holes
• Real space picture:
Two ways to put in a hole… Two ways to put in a particle…
UN(1-x) states N(1-x) states
2xN states
!
(",#)
!
µ
• Particle hole symmetry point:
!
1" x = 2x
!
x =1
3
U
!
µ
DeMarco: Measure thermopower & transport• How to probe in cold-atom Hubbard experiments?
Other probes sensitive to p-h symmetry?
• Phase diagram based on DMFT:
Park et al PRL 2008
Mott transition of 2-D Hubbard model• 2-D: No long-range order for continuous symmetries
– No AF order! – Can have Mott transition: Ising
Spins localized, but no LRO
• Cold-atoms: Test scenarios for the Mott transition– Role of local magnetic correlations
– Many electronic materials: Coupled to lattice
Critical point
Phase sep.
Entropy of insulator is lower than Fermi liquiddue to short-range correlations
Concluding remarks• Key Outstanding problem: Normal phase of cuprates/Hubbard model
Pseudogap state ofunderdoped cuprates Optimal doping:
Marginal Fermi liquid
doping xAF SC
T
PG FL
T*
Tc
TNMFL
– Emergent particle-hole symmetry?
• Quantum critical point? – Other evidence: Transport in phase underneath SC dome (Large B field)
Boebinger et al PRL 1996
Bond ordered state inpseudogap?
Kohsaka et al Nature 2008Macridin & Jarrell PRB 2008
• Can we probe the pseudogap in cold atom experiments?