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Exploring Interacting Topological Insulators with Ultracold Atoms: The Synthetic Creutz-Hubbard Model

J. Jünemann1,2, A. Piga3, S.-J. Ran3, M. Lewenstein3,4, M. Rizzi1, and A. Bermudez5

  • 1Johannes Gutenberg-Universität, Institut für Physik, Staudingerweg 7, 55099 Mainz, Germany
  • 2MAINZ–Graduate School Materials Science in Mainz, Staudingerweg 9, 55099 Mainz, Germany
  • 3ICFO-Institut de Ciencies Fotoniques, The Barcelona Institute of Science and Technology, 08860 Castelldefels (Barcelona), Spain
  • 4ICREA, Lluis Companys 23, 08010 Barcelona, Spain
  • 5Department of Physics, Swansea University, Singleton Park, Swansea SA2 8PP, United Kingdom and Instituto de Física Fundamental, IFF-CSIC, Madrid E-28006, Spain

Phys. Rev. X 7, 031057 – Published 27 September, 2017

DOI: https://doi.org/10.1103/PhysRevX.7.031057

Abstract

Understanding the robustness of topological phases of matter in the presence of strong interactions and synthesizing novel strongly correlated topological materials lie among the most important and difficult challenges of modern theoretical and experimental physics. In this work, we present a complete theoretical analysis of the synthetic Creutz-Hubbard ladder, which is a paradigmatic model that provides a neat playground to address these challenges. We give special attention to the competition of correlated topological phases and orbital quantum magnetism in the regime of strong interactions. These results are, furthermore, confirmed and extended by extensive numerical simulations. Moreover, we propose how to experimentally realize this model in a synthetic ladder made of two internal states of ultracold fermionic atoms in a one-dimensional optical lattice. Our work paves the way towards quantum simulators of interacting topological insulators with cold atoms.

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References (95)

  1. X. Wen, From the Origin of Sound to an Origin of Light and Electrons, Quantum Field Theory of Many-Body Systems(Oxford University Press, New York, 2004).
  2. A. Y. Kitaev, Fault-Tolerant Quantum Computation by Anyons, Ann. Phys. (Amsterdam) 303, 2 (2003); C. Nayak, A. Stern, M. Freedman, and S. Das Sarma, Non-Abelian Anyons and Topological Quantum Computation, Rev. Mod. Phys. 80, 1083 (2008).
  3. K. Klitzing, G. Dorda, and M. Pepper, New Method for High-Accuracy Determination of the Fine-Structure Constant Based on Quantized Hall Resistance, Phys. Rev. Lett. 45, 494 (1980).
  4. D. J. Thouless, M. Kohmoto, M. P. Nightingale, and M. den Nijs, Quantized Hall Conductance in a Two-Dimensional Periodic Potential, Phys. Rev. Lett. 49, 405 (1982).
  5. B. I. Halperin, Quantized Hall Conductance, Current-Carrying Edge States, and the Existence of Extended States in a Two-Dimensional Disordered Potential, Phys. Rev. B 25, 2185 (1982).
  6. C. L. Kane and M. P. A. Fisher, in Perspectives in Quantum Hall Effects: Novel Quantum Liquids in Low-Dimensional Semiconductor Structures, edited by S. Das Sarma and A. Pinczuk (Wiley-VCH Verlag, Weinheim, 2004).
  7. F. D. M. Haldane, Model for a Quantum Hall Effect without Landau Levels: Condensed-Matter Realization of the “Parity Anomaly”, Phys. Rev. Lett. 61, 2015 (1988).
  8. A. Y. Kitaev, Unpaired Majorana Fermions in Quantum Wires, Phys. Usp. 44, 131 (2001).
  9. C. L. Kane and E. J. Mele, Z2 Topological Order and the Quantum Spin Hall Effect, Phys. Rev. Lett. 95, 146802 (2005).
  10. A. Altland and M. R. Zirnbauer, Nonstandard Symmetry Classes in Mesoscopic Normal-Superconducting Hybrid Structures, Phys. Rev. B 55, 1142 (1997); A. P. Schnyder, S. Ryu S, A. Furusaki, and A. W. W. Ludwig, Classification of Topological Insulators and Superconductors in Three Spatial Dimensions, 78, 195125 (2008); A. Y. Kitaev, Periodic Table for Topological Insulators and Superconductors, AIP Conf. Proc. 1134, 22 (2009).
  11. See M. Z. Hasan and C. L. Kane, Colloquium: Topological Insulators, Rev. Mod. Phys. 82, 3045 (2010); X.-L. Qi and S.-C. Zhang, Topological Insulators and Superconductors, 83, 1057 (2011), and references therein.
  12. M. König, S.Wiedmann, C. Brüne, A. Roth, H. Buhmann, L. W. Molenkamp, X.-L. Qi, and S.-C. Zhang, Quantum Spin Hall Insulator State in HgTe Quantum Wells, Science 318, 766 (2007).
  13. D. Hsieh, Q. Dong, A. L. Wray, Y. Xia, Y. Hor, R. Cava, and M. Z. Hasan, A Topological Dirac Insulator in a Quantum Spin Hall Phase, Nature (London) 452, 970 (2008).
  14. V. Mourik, K. Zuo, S. M. Frolov, S. R. Plissard, E. P. A. M. Bakkers, and L. P. Kouwenhoven, Signatures of Majorana Fermions in Hybrid Superconductor-Semiconductor Nanowire Devices, Science 336, 1003 (2012).
  15. D. R. Hofstadter, Energy Levels and Wave Functions of Bloch Electrons in Rational and Irrational Magnetic Fields, Phys. Rev. B 14, 2239 (1976).
  16. See M. Hohenadler and F. F. Assaad, Correlation Effects in Two-Dimensional Topological Insulators, J. Phys. Condens. Matter 25, 143201 (2013), and references therein.
  17. R. B. Laughlin, Anomalous Quantum Hall Effect: An Incompressible Quantum Fluid with Fractionally Charged Excitations, Phys. Rev. Lett. 50, 1395 (1983).
  18. See I. Bloch, J. Dalibard, and W. Zwerger, Many-Body Physics with Ultracold Gases, Rev. Mod. Phys. 80, 885 (2008), and references therein.
  19. See M. Lewenstein, A. Sanpera, V. Ahufinger, B. Damski, A. Sen, and U. Sen, Ultracold Atomic Gases in Optical Lattices: Mimicking Condensed Matter Physics and Beyond, Adv. Phys. 56, 243 (2007), and references therein.
  20. See I. Bloch, J. Dalibard, and S. Nascimbène, Quantum Simulations with Ultracold Quantum Gases, Nat. Phys. 8, 267 (2012), and references therein.
  21. M. P. A. Fisher, P. B. Weichman, G. Grinstein, and D. S. Fisher, Boson Localization and the Superfluid-Insulator Transition, Phys. Rev. B 40, 546 (1989).
  22. D. Jaksch, C. Bruder, J. I. Cirac, C. W. Gardiner, and P. Zoller, Cold Bosonic Atoms in Optical Lattices, Phys. Rev. Lett. 81, 3108 (1998).
  23. M. Greiner, O. Mandel, T. Esslinger, T. W. Hänsch, and I. Bloch, Quantum Phase Transition from a Superfluid to a Mott Insulator in a Gas of Ultracold Atoms, Nature (London) 415, 39 (2002).
  24. J. Hubbard, Electron Correlations in Narrow Energy Bands, Proc. R. Soc. A 276, 238 (1963).
  25. W. Hofstetter, J. I. Cirac, P. Zoller, E. Demler, and M. D. Lukin, High-Temperature Superfluidity of Fermionic Atoms in Optical Lattices, Phys. Rev. Lett. 89, 220407 (2002).
  26. R. Jördens, N. Strohmaier, K. Günter, H. Moritz, and T. Esslinger, A Mott Insulator of Fermionic Atoms in an Optical Lattice, Nature (London) 455, 204 (2008); U. Schneider, L. Hackermüller, S. Will, Th. Best, I. Bloch, T. A. Costi, R. W. Helmes, D. Rasch, and A. Rosch, Metallic and Insulating Phases of Repulsively Interacting Fermions in a 3D Optical Lattice, Science 322, 1520 (2008).
  27. D. Jaksch and P. Zoller, Creation of Effective Magnetic Fields in Optical Lattices: The Hofstadter Butterfly for Cold Neutral Atoms, New J. Phys. 5, 56 (2003).
  28. N. Goldman, I. Satija, P. Nikolic, A. Bermudez, M. A. Martin-Delgado, M. Lewenstein, and I. B. Spielman, Realistic Time-Reversal Invariant Topological Insulators with Neutral Atoms, Phys. Rev. Lett. 105, 255302 (2010).
  29. K. Wilson, in New Phenomena in Subnuclear Physics, edited by A. Zichichi (Plenum, New York, 1977).
  30. See N. Goldman, G. Juzeliunas, P. Öhberg, and I. B. Spielman, Light-Induced Gauge Fields for Ultracold Atoms, Rep. Prog. Phys. 77, 126401 (2014), and references therein.
  31. See N. Goldman, J. C. Budich, and P. Zoller, Topological Quantum Matter with Ultracold Gases in Optical Lattices, Nat. Phys. 12, 639 (2016), and references therein.
  32. M. Aidelsburger, M. Atala, M. Lohse, J. T. Barreiro, B. Paredes, and I. Bloch, Realization of the Hofstadter Hamiltonian with Ultracold Atoms in Optical Lattices, Phys. Rev. Lett. 111, 185301 (2013); H. Miyake, G. A. Siviloglou, C. J. Kennedy, W. C. Burton, and W. Ketterle, Realizing the Harper Hamiltonian with Laser-Assisted Tunneling in Optical Lattices, 111, 185302 (2013); M. Atala, M. Aidelsburger, M. Lohse, J. T. Barreiro, B. Paredes, and I. Bloch, Observation of Chiral Currents with Ultracold Atoms in Bosonic Ladders, Nat. Phys. 10, 588 (2014); M. Aidelsburger, M. Lohse, C. Schweizer, M. Atala, J. T. Barreiro, S. Nascimbene, N. R. Cooper, I. Bloch, and N. Goldman, Measuring the Chern Number of Hofstadter Bands with Ultracold Bosonic Atoms, 11, 162 (2015).
  33. G. Jotzu, M. Messer, R. Desbuquois, M. Lebrat, T. Uehlinger, D. Greif, and T. Esslinger, Experimental Realization of the Topological Haldane Model with Ultracold Fermions, Nature (London) 515, 237 (2014); N. Fläschner, B. S. Rem, M. Tarnowski, D. Vogel, D.-S. Lühmann, K. Sengstock, and C. Weitenberg, Experimental Reconstruction of the Berry Curvature in a Floquet Bloch Band, Science 352, 1091 (2016).
  34. C. Chin, R. Grimm, P. Julienne, and E. Tiesinga, Feshbach Resonances in Ultracold Gases, Rev. Mod. Phys. 82, 1225 (2010).
  35. M. Creutz, End States, Ladder Compounds, and Domain-Wall Fermions, Phys. Rev. Lett. 83, 2636 (1999).
  36. See U. Schollwoeck, The Density-Matrix Renormalization Group in the Age of Matrix Product States, Ann. Phys. (Amsterdam) 326, 96 (2011), and references therein.
  37. W. P. Su, J. R. Schrieffer, and A. J. Heeger, Solitons in Polyacetylene, Phys. Rev. Lett. 42, 1698 (1979).
  38. M. Atala, M. Aidelsburger, J. T. Barreiro, D. Abanin, T. Kitagawa, E. Demler, and I. Bloch, Direct Measurement of the Zak Phase in Topological Bloch Bands, Nat. Phys. 9, 795 (2013).
  39. M. Creutz and I. Horváth, Surface States and Chiral Symmetry on the Lattice, Phys. Rev. D 50, 2297 (1994).
  40. D. B. Kaplan, A Method for Simulating Chiral Fermions on the Lattice, Phys. Lett. B 288, 342 (1992).
  41. H. B. Nielsen and M. Ninomiya, Absence of Neutrinos on a Lattice: (I). Proof by Homotopy Theory, Nucl. Phys. B185, 20 (1981); Absence of Neutrinos on a Lattice: (II). Intuitive Topological Proof, B193, 173 (1981).
  42. A. Bermudez, L. Mazza, M. Rizzi, N. Goldman, M. Lewenstein, and M. A. Martin-Delgado, Wilson Fermions and Axion Electrodynamics in Optical Lattices, Phys. Rev. Lett. 105, 190404 (2010).
  43. See D. Xiao, M.-C. Chang, and Q.Niu, Berry Phase Effects on Electronic Properties, Rev. Mod. Phys. 82, 1959 (2010), and references therein.
  44. J. Zak, Berry’s Phase for Energy Bands in Solids, Phys. Rev. Lett. 62, 2747 (1989).
  45. M. Tovmasyan, E. van Nieuwenburg, and S. D. Huber, Geometry-Induced Pair Condensation, Phys. Rev. B 88, 220510(R) (2013).
  46. S. Takayoshi, H. Katsura, N. Watanabe, and H. Aoki, Phase Diagram and Pair Tomonaga-Luttinger Liquid in a Bose-Hubbard Model with Flat Bands, Phys. Rev. A 88, 063613 (2013).
  47. S. D. Huber and E. Altman, Bose Condensation in Flat Bands, Phys. Rev. B 82, 184502 (2010).
  48. M. Tovmasyan, S. Peotta, P. Törmä, and S. D. Huber, Effective Theory and Emergent SU(2) Symmetry in the Flat Bands of Attractive Hubbard Models, Phys. Rev. B 94, 245149 (2016).
  49. D. Sticlet, L. Seabra, F. Pollmann, and J. Cayssol, From Fractionally Charged Solitons to Majorana Bound States in a One-Dimensional Interacting Model, Phys. Rev. B 89, 115430 (2014).
  50. L. Mazza, M. Aidelsburger, H.-H. Tu, N. Goldman, and M. Burrello, Methods for Detecting Charge Fractionalization and Winding Numbers in an Interacting Fermionic Ladder, New J. Phys. 17, 105001 (2015).
  51. See S. A. Parameswaran, R. Roy, and S. L. Sondhi, Fractional Quantum Hall Physics in Topological Flat, C.R. Phys. 14, 816 (2013), and references therein.
  52. D. A. Abanin, T. Kitagawa, I. Bloch, and E. Demler, Interferometric Approach to Measuring Band Topology in 2D Optical Lattices, Phys. Rev. Lett. 110, 165304 (2013); F. Grusdt, D. Abanin, and E. Demler, Measuring Z2 Topological Invariants in Optical Lattices Using Interferometry, Phys. Rev. A 89, 043621 (2014).
  53. J. Vidal, R. Mosseri, and B. Doucot, Aharonov-Bohm Cages in Two-Dimensional Structures, Phys. Rev. Lett. 81, 5888 (1998).
  54. M. Mancini, G. Pagano, G. Cappellini, L. Livi, M. Rider, J. Catani, C. Sias, P. Zoller, M. Inguscio, M. Dalmonte, and L. Fallani, Observation of Chiral Edge States with Neutral Fermions in Synthetic Hall Ribbons, Science 349, 1510 (2015).
  55. B. K. Stuhl, H.-I. Lu, L. M. Aycock, D. Genkina, and I. B. Spielman, Visualizing Edge States with an Atomic Bose Gas in the Quantum Hall Regime, Science 349, 1514 (2015).
  56. A. L. Gaunt, T. F. Schmidutz, I. Gotlibovych, R. P. Smith, and Z. Hadzibabic, Bose-Einstein Condensation of Atoms in a Uniform Potential, Phys. Rev. Lett. 110, 200406 (2013); A. L. Navon, A. L. Gaunt, R. P. Smith, and Z. Hadzibabic, Critical Dynamics of Spontaneous Symmetry Breaking in a Homogeneous Bose Gas, Science 347, 167 (2015); L. Corman, L. Chomaz, T. Bienaimé, R. Desbuquois, C. Weitenberg, S. Nascimbene, J. Dalibard, and J. Beugnon, Quench-Induced Supercurrents in an Annular Bose Gas, Phys. Rev. Lett. 113, 135302 (2014).
  57. N. Goldman, J. Beugnon, and F. Gerbier, Detecting Chiral Edge States in the Hofstadter Optical Lattice, Phys. Rev. Lett. 108, 255303 (2012).
  58. T. D. Stanescu, V. Galitski, and S. Das Sarma, Topological States in Two-Dimensional Optical Lattices, Phys. Rev. A 82, 013608 (2010).
  59. E. Fradkin and L. Susskind, Order and Disorder in Gauge Systems and Magnets, Phys. Rev. D 17, 2637 (1978); J. B. Kogut, An Introduction to Lattice Gauge Theory and Spin Systems, Rev. Mod. Phys. 51, 659 (1979).
  60. P. Jordan and E. Wigner, Über das Paulische Äquivalenzverbot, Z. Phys. 47, 631 (1928).
  61. J. H. Taylor and G. Müller, Magnetic Field Effects in the Dynamics of Alternating or Anisotropic Quantum Spin Chains, Physica (Amsterdam) 130A, 1 (1985).
  62. F. Grusdt, N. Y. Yao, D. Abanin, M. Fleischhauer, and E. Demler, Interferometric Measurements of Many-Body Topological Invariants Using Mobile Impurities, Nat. Commun. 7, 11994 (2016).
  63. I. Carusotto, Bragg Scattering and the Spin Structure Factor of Two-Component Atomic Gases, J. Phys. B 39, S211 (2006).
  64. J. H. Drewes, L. A. Miller, E. Cocchi, C. F. Chan, N. Wurz, M. Gall, D. Pertot, F. Brennecke, and M. Köhl, Antiferromagnetic Correlations in Two-Dimensional Fermionic Mott-Insulating and Metallic Phases, Phys. Rev. Lett. 118, 170401 (2017).
  65. K. Eckert, O. Romero-Isart, M. Rodriguez, M. Lewenstein, E. S. Polzik, and A. Sanpera, Quantum Non-Demolition Detection of Strongly Correlated Systems, Nat. Phys. 4, 50 (2008).
  66. D. Greif, M. F. Parsons, A. Mazurenko, C. S. Chiu, S. Blatt, F. Huber, G. Ji, and M. Greiner, Site-Resolved Imaging of a Fermionic Mott Insulator, Science 351, 953 (2016); M. Boll, T. A. Hilker, G. Salomon, A. Omran, J. Nespolo, L. Pollet, I. Bloch, and C. Gross, Spin- and Density-Resolved Microscopy of Antiferromagnetic Correlations in Fermi-Hubbard Chains, 353, 1257 (2016).
  67. P. W. Anderson, New Approach to the Theory of Superexchange Interactions, Phys. Rev. 115, 2 (1959).
  68. L.-M. Duan, E. Demler, and M. D. Lukin, Controlling Spin Exchange Interactions of Ultracold Atoms in Optical Lattices, Phys. Rev. Lett. 91, 090402 (2003).
  69. S. Trotzky, P. Cheinet, S. Fölling, M. Feld, U. Schnorrberger, A. M. Rey, A. Polkovnikov, E. A. Demler, M. D. Lukin, and I. Bloch, Time-Resolved Observation and Control of Superexchange Interactions with Ultracold Atoms in Optical Lattices, Science 319, 295 (2008).
  70. D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, Short-Range Quantum Magnetism of Ultracold Fermions in an Optical Lattice, Science 340, 1307 (2013); R. A. Hart, P. M. Duarte, T.-L. Yang, X. Liu, T. Paiva, E. Khatami, R. T. Scalettar, N. Trivedi, D. A. Huse, and R. G. Hulet, Observation of Antiferromagnetic Correlations in the Hubbard Model with Ultracold Atoms, Nature (London) 519, 211 (2015).
  71. A. H. MacDonald, S. M. Girvin, and D. Yoshioka, t/U Expansion for the Hubbard Model, Phys. Rev. B 37, 9753 (1988).
  72. P. Pfeuty, The One-Dimensional Ising Model with a Transverse Field, Ann. Phys. (N.Y.) 57, 79 (1970).
  73. N. N. Bogoliubov, On a New Method in the Theory of Superconductivity, Sov. Phys. JETP, 7, 41 (1958) [Nuovo Cimento Soc. Ital. Fis. 6, 794 (1958)].
  74. See O. Dutta, M. Gajda, P. Hauke, M. Lewenstein, D.-S. Lhmann, B. A. Malomed, T. Sowiski, and J. Zakrzewski, Non-Standard Hubbard Models in Optical Lattices: A Review, Rep. Prog. Phys. 78, 066001 (2015), and references therein.
  75. The energies of the bulk bands for the finite chain can differ from those of the periodic chain by an intensive quantity related to the missing bond timb connecting the edges. In the thermodynamic limit N, this difference will be irrelevant for any extensive observable, or any quantity that depends on a sum over all possible bulk energies.

  76. P. W. Anderson, Localized Magnetic States in Metals, Phys. Rev. 124, 41 (1961); U. Fano, Effects of Configuration Interaction on Intensities and Phase Shifts, 124, 1866 (1961).
  77. N. N. Bogoliubov, On a New Method in the Theory of Superconductivity, Sov. Phys. JETP, 7, 41 (1958) [Nuovo Cimento Soc. Ital. Fis. 6, 794 (1958)].
  78. See L. Amico, R. Fazio, A. Osterloh, and V. Vedral, Entanglement in Many-Body Systems, Rev. Mod. Phys. 80, 517 (2008), and references therein.
  79. T. Osborne and M. Nielsen, Entanglement in a Simple Quantum Phase Transition, Phys. Rev. A 66, 032110 (2002); A. Osterloh, L. Amico, G. Falci, and R. Fazio, Scaling of Entanglement Close to a Quantum Phase Transition, Nature (London) 416, 608 (2002).
  80. G. Vidal, J. Latorre, E. Rico, and A. Kitaev, Entanglement in Quantum Critical Phenomena, Phys. Rev. Lett. 90, 227902 (2003); P. Calabrese and J. Cardy, Entanglement Entropy and Quantum Field Theory, J. Stat. Mech. (2004) P06002.
  81. See P. Calabrese and J. Cardy, Entanglement Entropy and Conformal Field Theory, J. Phys. A 42, 504005 (2009), and references therein.
  82. H. Li and F. D. M. Haldane, Entanglement Spectrum as a Generalization of Entanglement Entropy: Identification of Topological Order in Non-Abelian Fractional Quantum Hall Effect States, Phys. Rev. Lett. 101, 010504 (2008).
  83. F. Pollmann, A. M. Turner, E. Berg, and M. Oshikawa, Entanglement Spectrum of a Topological Phase in One Dimension, Phys. Rev. B 81, 064439 (2010).
  84. A. Bermudez, D. Patane, L. Amico, and M. A. Martin-Delgado, Topology-Induced Anomalous Defect Production by Crossing a Quantum Critical Point, Phys. Rev. Lett. 102, 135702 (2009).
  85. L. Mazza, A. Bermudez, N. Goldman, M. Rizzi, M. A. Martin-Delgado, and M. Lewenstein, An Optical-Lattice-Based Quantum Simulator for Relativistic Field Theories and Topological Insulators, New J. Phys. 14, 015007 (2012).
  86. O. Boada, A. Celi, M. Lewenstein, and J. I. Latorre, Quantum Simulation of an Extra Dimension, Phys. Rev. Lett. 108, 133001 (2012).
  87. A. Celi, P. Massignan, J. Ruseckas, N. Goldman, I. B. Spielman, G. Juzeliunas, and M. Lewenstein, Synthetic Gauge Fields in Synthetic Dimensions, Phys. Rev. Lett. 112, 043001 (2014).
  88. See A. Eckardt, Colloquium: Atomic Quantum Gases in Periodically Driven Optical Lattices, Rev. Mod. Phys. 89, 011004 (2017), and references therein.
  89. A. Bermudez, T. Schätz, and D. Porras, Synthetic Gauge Fields for Vibrational Excitations of Trapped Ions, Phys. Rev. Lett. 107, 150501 (2011); P. Hauke, O. Tieleman, A. Celi, C. Ölschläger, J. Simonet, J. Struck, M. Weinberg, P. Windpassinger, K. Sengstock, M. Lewenstein, and A. Eckardt, Non-Abelian Gauge Fields and Topological Insulators in Shaken Optical Lattices, 109, 145301 (2012).
  90. F. Gerbier and J. Dalibard, Gauge Fields for Ultracold Atoms in Optical Superlattices, New J. Phys. 12, 033007 (2010).
  91. G. Jotzu, M. Messer, F. Görg, D. Greif, R. Desbuquois, and T. Esslinger, Creating State-Dependent Lattices for Ultracold Fermions by Magnetic Gradient Modulation, Phys. Rev. Lett. 115, 073002 (2015).
  92. K. Drese and M. Holthaus, Ultracold Atoms in Modulated Standing Light Waves, Chem. Phys. 217, 201 (1997); C. Sias, H. Lignier, Y. P. Singh, A. Zenesini, D. Ciampini, O. Morsch, and E. Arimondo, Observation of Photon-Assisted Tunneling in Optical Lattices, Phys. Rev. Lett. 100, 040404 (2008).
  93. R. Ma, M. E. Tai, P. M. Preiss, W. S. Bakr, J. Simon, and M. Greiner, Photon-Assisted Tunneling in a Biased Strongly Correlated Bose Gas, Phys. Rev. Lett. 107, 095301 (2011); Y.-A. Chen, S. Nascimbene, M. Aidelsburger, M. Atala, S. Trotzky, and I. Bloch, Controlling Correlated Tunneling and Superexchange Interactions with ac-Driven Optical Lattices, 107, 210405 (2011).
  94. A. J. Daley and J. Simon, Effective Three-Body Interactions via Photon-Assisted Tunneling in an Optical Lattice, Phys. Rev. A 89, 053619 (2014).
  95. A. Bermudez and D. Porras, Interaction-Dependent Photon-Assisted Tunneling in Optical Lattices: A Quantum Simulator of Strongly-Correlated Electrons and Dynamical Gauge Fields, New J. Phys. 17, 103021 (2015).

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