论文标题

圆形摇动骰子晶格中的拓扑floquet波段

Topological Floquet-bands in a circularly shaken dice lattice

论文作者

Cheng, Shujie, Xianlong, Gao

论文摘要

光学骰子晶格中非相互作用颗粒的跳跃导致三个最低迷你班形成的条带结构中的无间隙分散体。在我们的研究中,我们发现,一旦将定期驱动力应用于此光学骰子晶格,就可以更改原始光谱特性,从而在准能源brillouin区域形成三个间隙的准能带。包含最低准能带的Chern数量的拓扑相图表明,当最近邻居的跳跃的跳跃强度是各向同性的时,该系统持续存在于拓扑非平凡的阶段,Chern数字$ C = 2 $在广泛的驱动强度之内。伴随着各向异性最近的跳跃强度,发生了拓扑相过渡,使Chern数字从$ C = 2 $变为$ C = 1 $。通过我们的分析方法进一步验证了这种过渡。我们的理论工作意味着,可以通过应用周期性的摇动来实现光学骰子晶格的非拓扑特征是可行的,并且可以通过独立调整一种近端静脉跳跃的强度来观察到拓扑相变。

The hoppings of non-interacting particles in the optical dice lattice result in the gapless dispersions in the band structure formed by the three lowest minibands. In our research, we find that once a periodic driving force is applied to this optical dice lattice, the original spectral characteristics could be changed, forming three gapped quasi-energy bands in the quasi-energy Brillouin zone. The topological phase diagram containing the Chern number of the lowest quasi-energy band shows that when the hopping strengths of the nearest-neighboring hoppings are isotropic, the system persists in the topologically non-trivial phases with Chern number $C=2$ within a wide range of the driving strength. Accompanied by the anisotropic nearest-neighboring hopping strengths, a topological phase transition occurs, making Chern number change from $C=2$ to $C=1$. This transition is further verified by our analytical method. Our theoretical work implies that it is feasible to realize the non-trivially topological characteristics of optical dice lattices by applying the periodic shaking, and that topological phase transition can be observed by independently tuning the strength of a type of nearest-neighbor hopping.

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