哈珀-霍夫斯塔特模型中的量化场诱导拓扑特征

Xue Han, Fude Li, De-Xiu Qiu, Kang Xue, X. X. Yi
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引用次数: 0

摘要

经典磁场可能会改变拓扑绝缘体的特性,如时间反转对称性保护拓扑边缘态。这就提出了一个问题:相对于经典磁场,量子化磁场是否会改变拓扑材料的不同特性。在本文中,我们提出了一个模型来描述与可调谐单模量子化场耦合的拓扑绝缘体(带磁场的方形光学晶格中的超冷原子),并讨论了该系统的拓扑特征。我们发现,量子化场能以不同的方式诱导拓扑量子相变。具体来说,对于固定的规磁通量比,我们计算了在开放和周期边界条件下系统与磁场之间不同耦合常数的能带。我们发现,在连续规磁通量比下,霍夫斯塔德蝴蝶图被分成一对,这与没有单模量化磁场时的情况不同。此外,我们还绘制了以切尔数为特征的拓扑相图,它是单模量子化场动量的函数,并得到了一个具有非零填充因子的量子化结构。
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Quantized fields induced topological features in Harper-Hofstadter model

Classical magnetic fields might change the properties of topological insulators such as the time reversal symmetry protected topological edge states. This poses a question that whether quantized fields would change differently the feature of topological materials with respect to the classical one. In this paper, we propose a model to describe topological insulators (ultracold atoms in square optical lattices with magnetic field) coupled to a tunable single-mode quantized field, and discuss the topological features of the system. We find that the quantized field can induce topological quantum phase transitions in a different way. To be specific, for fixed gauge magnetic flux ratio, we calculate the energy bands for different coupling constants between the systems and the fields in both open and periodic boundary conditions. We find that the Hofstadter butterfly graph is divided into a pair for continuous gauge magnetic flux ratio, which is different from the one without single-mode quantized field. In addition, we plot topological phase diagrams characterized by Chern number as a function of the momentum of the single-mode quantized field and obtain a quantized structure with non-zero filling factor.

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