2017
DOI: 10.1103/physreva.95.013616
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Artificial topological models based on a one-dimensional spin-dependent optical lattice

Abstract: Topological matter is a popular topic in both condensed matter and cold atom research. In the past decades, a variety of models have been identified with fascinating topological features. Some, but not all, of the models can be found in materials. As a fully controllable system, cold atoms trapped in optical lattices provide an ideal platform to simulate and realize these topological models. Here we present a proposal for synthesizing topological models in cold atoms based on a one-dimensional (1D) spin-depend… Show more

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Cited by 6 publications
(5 citation statements)
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“…Schemes for realizing quantum simulators for the standard Dirac-fermion systems, using cold-atomic gases in continuum and lattice systems, have been already proposed. Some of them are a Raman coupling scheme [19][20][21][22], a modulation method on a tilted lattice [23], and an effective model of two-component cold atoms in a 1D optical superlattice [24]. The above works focus on the standard Dirac fermions.…”
Section: Introductionmentioning
confidence: 99%
“…Schemes for realizing quantum simulators for the standard Dirac-fermion systems, using cold-atomic gases in continuum and lattice systems, have been already proposed. Some of them are a Raman coupling scheme [19][20][21][22], a modulation method on a tilted lattice [23], and an effective model of two-component cold atoms in a 1D optical superlattice [24]. The above works focus on the standard Dirac fermions.…”
Section: Introductionmentioning
confidence: 99%
“…Here d d d d , , . Therefore, the lattice system described by eff  shares the same topological properties from the eigenstates of 1  [43,44]. We can see that the Hamiltonian 1  respects the particle-hole symmetry: k k…”
Section: Phase Transition and Topological Featuresmentioning
confidence: 80%
“…Therefore, the lattice system described by H eff shares the same topological properties from the eigenstates of H 1 [43,44]. We can see that the Hamiltonian H 1 respects the particle-hole symmetry: ΞH 1 (k)Ξ † = −H 1 (−k), where Ξ = σ x K ⊗ I 2×2 and K is the complex conjugate operator.…”
mentioning
confidence: 79%
“…A similar proposal based on a 1D spin-dependent OL for synthesizing SSH/Rice-Mele models with fully tunable parameters in the absence of domains was also presented in Ref. [135].…”
Section: Su-schrieffer-heeger Model and Rice-mele Modelmentioning
confidence: 96%