TY - DATA T1 - (a) The spatial density for the Haldane-like optical lattice described by equation (16), for λ = 0 and λ = 1 PY - 2013/06/24 AU - N Goldman AU - F Gerbier AU - M Lewenstein UR - https://iop.figshare.com/articles/figure/_a_The_spatial_density_for_the_Haldane_like_optical_lattice_described_by_equation_a_href_http_iopsci/1012051 DO - 10.6084/m9.figshare.1012051.v1 L4 - https://ndownloader.figshare.com/files/1479873 KW - Chern insulators KW - lattice sites KW - 3 J KW - value EF KW - ground state g KW - lattice size KW - quantum number KW - 8 J KW - r 0 KW - square lattice KW - Haldane quantum Hall model KW - chequerboard structure KW - tunnelling KW - topological insulators KW - Fermi energy KW - Haldane model KW - e states KW - bulk band KW - quantum Hall phases KW - metastable state e KW - V 0 KW - Atomic Physics KW - Molecular Physics N2 - Figure 4. (a) The spatial density for the Haldane-like optical lattice described by equation (16), for λ = 0 and λ = 1. The atoms are trapped by a harmonic potential V(r) = V0(r/r0)2, with V0 = 8J and r0 = 17a, and the lattice size is 40 × 40. The density was obtained by setting the Fermi energy to the value EF = 3J (corresponding to the maximum of the highest bulk band for λ = 0). The n coordinate is chosen to be fixed at the centre of the trap. (b) Same as (a) for λ = 1, but represented in the 2D plane x'–y'. Note the clear plateau for λ = 1, which indicates the opening of a spectral gap [44]. Abstract We describe a scheme to engineer non-Abelian gauge potentials on a square optical lattice using laser-induced transitions. We emphasize the case of two-electron atoms, where the electronic ground state g is laser-coupled to a metastable state e within a state-dependent optical lattice. In this scheme, the alternating pattern of lattice sites hosting g and e states depicts a chequerboard structure, allowing for laser-assisted tunnelling along both spatial directions. In this configuration, the nuclear spin of the atoms can be viewed as a 'flavour' quantum number undergoing non-Abelian tunnelling along nearest-neighbour links. We show that this technique can be useful to simulate the equivalent of the Haldane quantum Hall model using cold atoms trapped in square optical lattices, offering an interesting route to realize Chern insulators. The emblematic Haldane model is particularly suited to investigate the physics of topological insulators, but requires, in its original form, complex hopping terms beyond nearest-neighbouring sites. In general, this drawback inhibits a direct realization with cold atoms, using standard laser-induced tunnelling techniques. We demonstrate that a simple mapping allows us to express this model in terms of matrix hopping operators that are defined on a standard square lattice. This mapping is investigated for two models that lead to anomalous quantum Hall phases. We discuss the practical implementation of such models, exploiting laser-induced tunnelling methods applied to the chequerboard optical lattice. ER -