Strongly Correlated Physics With Ultra-Cold Atoms
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1 Strongly Correlated Physics With Ultra-Cold Atoms Predrag Nikolić Rice University
2 Acknowledgments Collaborators Subir Sachdev Eun-Gook Moon Anton Burkov Arun Paramekanti Sponsors W.M.Keck Program in Quantum Materials 2/31
3 Overview Ultra-cold atoms: the new frontier in strongly correlated physics Interacting fermions in the unitarity limit BCS-BEC crossover in uniform systems BCS-BEC crossover in optical lattices Rotating fermion quantum liquids near unitarity Unification with condensed matter Conclusions 3/31
4 The new frontier in strongly correlated physics Many-body physics: collective phenomena of many particles, N>>1 Examples: Fermi liquid, Bose-Einstein condensate (BEC) Strongly correlated physics: inadequate single-particle description Phenomena caused by interactions Hidden identity of individual particles (emergent phenomena) Examples: Mott insulators, superfluidity Condensed matter physics The physics of many-body and strongly correlated systems 4/31
5 Recent breakthroughs in atomic physics 1995: Bose-Einstein condensate 1998: Feshbach resonance 1999: Degenerate Fermi gas 2000: Vortex lattice 2002: Optical lattice SF-Mott 2003: Fermion condensates 2004: Tonks-Girardeau gas 2004: BEC-BCS crossover 2006: Correlations (statistics, KT...) I.Bloch, J.Dalibard, W.Zwerger; Rev.Mod.Phys. 80, 885 (2008) Images from Greiner and Ketterle labs 5/31
6 Ultra-cold fermions Fermions Lithium 6Li, Potassium 40K Two lowest hyperfine-split states: spin up and down Trapping Magnetic (Zeeman effect), optical: N ~ Cooling Laser cooling (Doppler shift): T~100mK + Sisyphus: T~10mK Evaporative: T ~ nk... (Tf ~ μk) Probing Absorption images (density), spectroscopy, interference 6/31
7 Strongly correlated fermions Feshbach resonance Resonant two-body scattering Scattering length exceeds inter-particle distance Optical lattice Suppressed kinetic energy, interactions win Superfluid-insulator transition Fast rotation Quantum liquids, quantum Hall effect Vortex lattices, KT transition Images from Ketterle lab 7/31
8 Challenges ahead Help us understand condensed matter materials One dimensional physics Correlated insulators (Mott, antiferromagnets) Superconductivity in large magnetic fields (FFLO) Cuprates, frustrated magnets, quantum computing... Physics not accessible in condensed matter materials BEC-BCS crossover Pauli-Clogston limit & FFLO states Exotic phases of matter (topological phases) 8/31
9 Interacting fermions in the unitarity limit Universality: irrelevant microscopic details a many-body effect near a 2nd order phase transition unitary scattering,,, 9/31
10 Quantum field theory at unitarity Theoretical Approaches Mean-field approximation Perturbation theory Renormalization group P.N., S.Sachdev; Phys.Rev. A 75, (2007) 10/31
11 BCS-BEC crossover in uniform systems Attractive interactions & pairing correlations Weak => many-body bound state, BCS superconductor Strong => two-body bound state, BEC condensate of molecules Unitarity Feshbach resonance The strongest pairing correlations and quantum entanglement Novel state uniquely accessible in atomic physics Fundamental questions The evolution of states between BCS and BEC limits New quantum phases 11/31
12 Rice: polarized fermionic superfluids G.B.Partridge, W.Li, R.I.Kamar, Y.A.Liao, R.G.Hulet Science 311, 503 (2006) G.B.Partridge, W.Li, Y.A.Liao, R.G.Hulet, M.Haque, H.T.C.Stoof Phys.Rev.Lett. 97, (2006) 12/31
13 MIT: polarized fermionic superfluids M.Zwierlen, A.Schirotzek, C.H.Schunck, W.Ketterle; Science 311, 492 (2006) Y.Shin, M.W.Zwierlein, C.H.Schunck, A.Schirotzek, W.Ketterle; Phys.Rev.Lett. 97, (2006) 13/31
14 T=0 phase diagram with population imbalance 1st order superfluid-metal transitions: hc=0.807μ+o(1/n) 2nd order superfluid-insulator (vacuum) transition Smooth BEC-BCS crossover Uniform magnetized BEC superfluid phase for μ<0 Normal metallic phases with one or two Fermi seas P.N., S.Sachdev; Phys.Rev. A 75, (2007) 14/31
15 Pairing fluctuations in T=0 normal states Pairing fluctuations increase pressure Longer-lived pairs larger pressure No pressure increase in the fully polarized state 15/31
16 Superfluid critical temperature 2nd order superluid-normal phase transition at T=Tc N=1 MC Monte-Carlo: E.Burovski, N.Prokof'ev, B.Svistunov, M.Troyer; Phys.Rev.Lett. 96, (2006) 16/31
17 BCS-BEC crossover in lattice potentials 2nd order superfluid-insulator phase transition at T=0, h=0 Band-Mott insulator crossover at unitarity (s-wave) E.G.Moon, P.Nikolić, S.Sachdev; Phys.Rev.Lett. 99, (2007) M.P.A.Fisher, P.B.Weichman, G.Grinstein, D.S.Fisher; Phys.Rev.B 40, 546 (1989) 17/31
18 Critical lattice depth Saddle-point approximation Diagonalize in continuum space near unitarity Single-band Hubbard models: only deep in BCS or BEC limits... Fix density - completely filled bands At unitarity: Our result: VC~ 70 Er MIT experiment: VC~ 6 Er Finite temperature effects? 18/31
19 Critical velocity and band -supersolids Uniform system Superfluid-metal: pairing at q=0 Universal critical velocity Lattice system Superfluid - band-insulator: pairing instability at q 0 P.Nikolić, A.Burkov, A.Paramekanti; (unpublished) 19/31
20 Strongly correlated insulators and superfluids Band -supersolid The effect of pairing between different bands Lattice symmetry breaking in the insulator due to pairing fluctuations? Unconventional Mott insulators Extended repulsive interactions (Coulomb, unitarity?) Fractional number of Cooper pairs per site Spontaneous lattice symmetry breaking Transition to superfluid Conventional (Landau-Ginzburg) supersolid Unconventional: deconfined critical point 20/31
21 Rotating fermion liquids near unitarity No time-reversal symmetry: quantum limit Superfluid vortex lattice Fermi liquid fermionic quantum Hall state Correlated insulators many possibilities Strongly correlated quantum insulators Quantum Hall liquid of Cooper pairs Density wave (Wigner crystal) of Cooper pairs Finite temperature, disorder Phase transitions or crossovers between different normal states? Critical fluctuations 21/31
22 Insulators and superfluids Normal state quantum Hall insulator Localized particles (cyclotron orbitals) Discrete Landau levels Macroscopic degeneracy: two particles per flux quantum Superfluid 22/31
23 Pairing instability Quantum Hall superfluid 2nd order (saddle-point) P.Nikolić; arxiv: (2008) P.Nikolić; arxiv: (2009) 23/31
24 Superfluids & Vortex lattice FFLO states Competing forces Pairing, orbital, Zeeman FFLO-metals and FFLO-insulators P.Nikolić; (unpublished) 24/31
25 Experimental signatures Trapped gasses Sharp shell boundaries FFLO: ρs 0 & p 0 FFLO-insulator: quantized p FFLO-metal: variable p Features Polarized outer shells FFLO rings, abrupt appearance 25/31
26 Vortex liquid Genuine phase at T=0 Vortex lattice potential energy: Δ04 Melting kinetic energy gain: log-1(δ0) 1st order vortex lattice melting as Δ0 0 Low energy spectrum inconsistent with fermionic quantum Hall states Δ0 Non-universal properties (by RG) strong (BEC) pairing weak (BCS) P.Nikolić; arxiv: (2009) 26/31
27 Unification with condensed matter Unification Particle physics truth is at high energies Condensed matter truth is at low energies Universal collective many-body phenomena cold atoms exhibit similar phenomena as electronic systems cold atoms are ideal and exceptionally tunable solvable theories which can be compared with experiments much to learn about probing Some unresolved problems Hubbard model Pseudogap in cuprates Frustrated magnets & exotic phases 27/31
28 Pseudogap in cuprates Fluctuating superconductivity Massless Dirac fermions Lattice + Coulomb repulsion + pairing d-wave no vortex core states Light, friction-free vortices Quantum vortex dynamics Competing orders Due to vortex quantum motion T.Hanaguri, et.al.; Nature 430, 1001 (2004) L.Balents, et.al.; Phys.Rev. B 71, (2005) L.Bartosch, L.Balents, S.Sachdev; Ann.Phys. 321, 1528 (2006). 28/31
29 Quantum motion of vortices B.W.Hoogenboom, et.al.; Phys.Rev.Lett. 87, (2001) Theory of vortices and quasiparticles P.N., S.Sachdev; Phys.Rev.B 73, (2006) P.N., S.Sachdev, L.Bartosch; Phys.Rev. B 74, (2006) P.N., S.Sachdev; Physica C 460, 256 (2007) Y.Wang, et.al.; Phys.Rev.B 73, (2006) 29/31
30 Unconventional phases Search for unconventional phases of matter Engineering custom quantum systems Ideal lattices, very little relaxation... Tunability Measurement techniques? Unconventional physics Valence-bond solids, spin liquids Topological phases Quantum computing P.N., T. Senthil; Phys.Rev.B 68, (2003) P.N., T. Senthil; Phys.Rev.B 71, (2005) P.N.; Phys.Rev.B 72, (2005) 30/31
31 Conclusions Unitarity Novel strongly correlated physics, universality BCS-BEC crossover with population imbalance Interacting fermions in lattice potentials Band-Mott insulator crossover at unitarity Supersolids & novel Mott insulators Fast-rotating interacting fermions Vortex lattices & FFLO states Vortex liquids 31/31
32 New phases due to Zeeman effect Breakdown of superconductivity Pauli-Clogston limit: μ -μ ~Δ FFLO: non-uniform magnetized superfluid Q=kF -kf Breached pair (Sarma) phase Q=0 extra
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