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Short-range quantum magnetism of ultracold fermions in an optical - - PowerPoint PPT Presentation
Short-range quantum magnetism of ultracold fermions in an optical - - PowerPoint PPT Presentation
Short-range quantum magnetism of ultracold fermions in an optical lattice Leticia Tarruell Experiments in Tilman Esslingers group, ETH Zurich Warsaw 26/06/2015 z y 50.000 40 K fermionic atoms T<0.1T F x The Fermi-Hubbard model t U
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The Fermi-Hubbard model
tunneling interaction
t U
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Quantum simulation
Strongly correlated material Fermi-Hubbard model
« with a suitable class of quantum machines you could imitate any quantum system »
- R. P. Feynman, 1981
Quantum simulator
t U
?
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2005: First experimental realization with cold atoms (non interacting fermions)
Metal – band insulator transition
The Fermi-Hubbard model
Metal Band insulator
filling
- M. Köhl, H. Moritz, T. Stöferle, K. Günter and T. Esslinger, Phys. Rev. Lett. 94, 080403 (2005)
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2008: Strongly correlated regime
The Fermi-Hubbard model
Metal – Mott insulator transition kinetic energy interaction energy
Delocalization vs. interactions
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The Fermi-Hubbard model
2008: Strongly correlated regime
Metal – Mott insulator transition
U/6t=4.8 U/6t=0
Non interacting Mott insulator
- R. Jördens et al., Nature 455, 204 (2008)
- U. Schneider et al.,
Science 322, 1520 (2008)
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Metal Mott insulator
The Fermi-Hubbard model
Next challenge:
Quantum magnetism
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Temperature scales
U>>t
energy T > U: metallic behavior T < U: Mott insulator
T
T < J: spin ordering
T
- R. Jördens et al., Phys. Rev. Lett. 104, 180401 (2010)
- P. Duarte et al., Phys. Rev. Lett. 114, 070403 (2015)
J=4t2/U
Superexchange J
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Approaches to magnetism
- S. Trotzky et al., Science 319, 295 (2008)
- S. Nascimbène et al., Phys. Rev. Lett. 108, 205301 (2012)
- S. Murmann et al., Phys. Rev. Lett. 114, 080402 (2015)
Isolated double-wells or plaquettes (Munich, Heidelberg)
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Approaches to magnetism
- J. Simon et al., Nature 472, 307 (2011)
Ising spin chains (Harvard)
- J. Struck et al., Science 333, 996 (2011)
- J. Struck et al., Nature Phys. 9, 738 (2013)
Classical magnetism, Ising XY (Hamburg)
Mappings
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Approaches to magnetism
Dipolar interactions (JILA, Paris)
- B. Yan et al., Nature 501, 521-525 (2013)
- A. de Paz et al., Phys. Rev. Lett. 111, 185305 (2013)
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- D. Greif et al., Science 340, 1307 (2013)
- R. A. Hart et al., Nature 519, 211 (2015)
Approaches to magnetism
Short-range quantum magnetism in the Fermi-Hubbard model (ETH, Rice)
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J < T < Jd,s
T J Jd
Jd > J
Dimerized lattice
energy
The energy trick
Magnetic correlations T < J
Js > J
Anisotropic cubic lattice
Jd,s
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Magnetic correlations in dimerized lattice
singlet triplet
Jd
Spin correlations on neighboring sites T < Jd : NS > NT
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Local spin correlations in cubic lattice
Nearest-neighbor spin correlations vs. temperature
antiferromagnetic transition DCA simulation 3D Fermi-Hubbard model
- S. Fuchs, E. Gull, L. Pollet, E. Burovski, E. Kozik, T. Pruschke, and M. Troyer,
- Phys. Rev. Lett. 106, 030401 (2011)
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Merging lattice sites
Chequerboard Dimer Square
Tool: tunable geometry optical lattice
- L. Tarruell et al., Nature 483, 302 (2012)
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Detecting magnetic correlations
singlet
- r
triplet t0 singlet triplet t0
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Dimerized lattice
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Singlet-Triplet Imbalance
Measuring singlets and triplets
𝑞𝑇 𝑞𝑢𝑢
Singlets Triplets
Merging neighboring sites Singlet-triplet oscillations
Singlet-triplet oscillations: S. Trotzky et al., Phys. Rev. Lett. 105, 265303 (2010)
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Theory: second order high-temperature series expansion of coupled dimers
Dependence on dimerization
s=1.7 kB
Jd T J
isotropic strongly dimerized
- D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, Science 340, 1307 (2013)
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Dependence on entropy
Theory: second order high-temperature series expansion
- f coupled dimers
U/t = 11.0(8) td/t = 22(2) t/h = 67(3) Hz
Jd T J
- D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, Science 340, 1307 (2013)
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Anisotropic simple cubic lattice
transverse spin correlator ⟺ population difference Redistribution of entropy: incoherent spin chains, entropy stored in between AFM correlations along x Effective 1D chains
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Dependence on anisotropy
isotropic strongly anisotropic VY,Z = 11.0(3) ER s = 1.8 kB normalized spin correlator
- D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, Science 340, 1307 (2013)
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- J. Imriška, M. Iazzi, L. Wang, E. Gull, D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell,
- T. Esslinger, and M. Troyer, Phys. Rev. Lett. 112, 115301 (2014)
Theory: DCA+LDA for anisotropic simple cubic lattice
Comparison with theory
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Dependence on entropy
tS /t=7.3
- D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, Science 340, 1307 (2013)
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Comparison with theory
Theory: DCA+LDA for anisotropic simple cubic lattice
- J. Imriška, M. Iazzi, L. Wang, E. Gull, D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell,
- T. Esslinger, and M. Troyer, Phys. Rev. Lett. 112, 115301 (2014)
Correlations over 2 sites
T<t
Analogous results with DMRG: B. Sciolla et al., Phys. Rev. A 88, 063629 (2013)
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Short range magnetic correlations
- D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, Science 340, 1307 (2013)
Nearest-neighbor magnetic correlations in thermalized ensembles
- J. Imriška, M. Iazzi, L. Wang, E. Gull, D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell,
- T. Esslinger, and M. Troyer, Phys. Rev. Lett. 112, 115301 (2014)
- B. Sciolla, A. Tokuno, S. Uchino, P. Bartmettler, T. Giamarchi, and C. Kollath,
- Phys. Rev. A 88, 063629 (2013)
Comparison with numerics: effective 1D systems with T<J
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The ETH quantum magnetism team
Gregor Jotzu Daniel Greif
- L. T. Thomas Uehlinger Tilman Esslinger
Theory: J. Imriška, M. Iazzi, L. Wang, E. Gull and M. Troyer Many discussions with C. Kollath and T. Giamarchi’s groups
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October 2013
Ultracold Quantum Gases group @
February 2014 September 2014 ICFO-The Institute of Photonic Sciences Barcelona, Spain June 2015
41K BEC 40K MOT
June 2015
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Ultracold Quantum Gases group @
- L. T.
Pierrick Cheiney César Cabrera
www.qge.icfo.es
Luca Tanzi Jordi Sastre Julio Sanz Manel Bosch (now at Laboratoire Kastler Brossel, Paris) Vincent Lienhard (now student at ENS Cachan) Lisa Saemisch (now at ICFO’s Molecular Nanophotonics group)
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Measuring double occupancy
- 2. Feshbach-induced energy shift
- 4. Expansion and Stern-Gerlach separation
- 1. Suppress tunneling
- 3. RF transfer
Doubly occupied sites
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Measuring double occupancy
mF=-9/2 mF=-5/2 mF=-7/2
Doubly occupied sites
Measure D for values as low as 1% !
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Exchange energy
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With a bit more cooling…
High-T phase diagram of cuprates
QCP Dimers AFM T/J J/Jd
Geometry-induced quantum phase transitions Frustration