10.6084/m9.figshare.1012051.v1
N Goldman
F Gerbier
M Lewenstein
(a) The spatial density for the Haldane-like optical lattice described by equation (16), for λ = 0 and λ = 1
2013
IOP Publishing
Chern insulators
lattice sites
3 J
value EF
ground state g
lattice size
quantum number
8 J
r 0
square lattice
Haldane quantum Hall model
chequerboard structure
tunnelling
topological insulators
Fermi energy
Haldane model
e states
bulk band
quantum Hall phases
metastable state e
V 0
2013-06-24 00:00:00
article
https://iop.figshare.com/articles/_a_The_spatial_density_for_the_Haldane_like_optical_lattice_described_by_equation_a_href_http_iopsci/1012051
<p><strong>Figure 4.</strong> (a) The spatial density for the Haldane-like optical lattice described by equation (<a href="http://iopscience.iop.org/0953-4075/46/13/134010/article#jpb460847eqn16" target="_blank">16</a>), for λ = 0 and λ = 1. The atoms are trapped by a harmonic potential <em>V</em>(<em>r</em>) = <em>V</em><sub>0</sub>(<em>r</em>/<em>r</em><sub>0</sub>)<sup>2</sup>, with <em>V</em><sub>0</sub> = 8<em>J</em> and <em>r</em><sub>0</sub> = 17<em>a</em>, and the lattice size is 40 <b>×</b> 40. The density was obtained by setting the Fermi energy to the value <em>E</em><sub>F</sub> = 3<em>J</em> (corresponding to the maximum of the highest bulk band for λ = 0). The <em>n</em> 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 <em>x</em>'–<em>y</em>'. Note the clear plateau for λ = 1, which indicates the opening of a spectral gap [<a href="http://iopscience.iop.org/0953-4075/46/13/134010/article#jpb460847bib44" target="_blank">44</a>].</p> <p><strong>Abstract</strong></p> <p>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 <em>g</em> is laser-coupled to a metastable state <em>e</em> within a state-dependent optical lattice. In this scheme, the alternating pattern of lattice sites hosting <em>g</em> and <em>e</em> 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 <em>matrix</em> 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.</p>