arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2007.11585cond-mat.str-elcond-mat.dis-nn
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无序反对称链中的拓扑晶相

Topological Crystalline Phases in a Disordered Inversion-Symmetric Chain

Saavanth Velury, Barry Bradlyn, Taylor L. Hughes

摘要:

当平移对称性被体无序破坏时,拓扑晶体系统中状态的拓扑性质可能会根据所应用的无序类型而改变。在这项工作中,我们描述了一个一维链的相位反转和手征对称性,其中每个无序配置是反转对称的。通过使用一个独立的基础配方的反转拓扑不变量,手性绕组数,和体极化,我们能够构建这些数量的相图时,无序存在。我们发现,不同于手征缠绕数和体极化,反转拓扑不变量可以波动时,体光谱间隙关闭在强无序。利用位置空间重整化群,我们能够比较如何在低能量的强无序极限的反转拓扑不变量,手征缠绕数和体极化的行为。我们发现,与反转保序无序,反转拓扑不变量的值是由反转中心的状态的反转本征值,而数量,如手征绕组数和体极化仍然有贡献,从整个链的每个状态。我们还表明,它是可能的,以改变一个干净的系统中的反转拓扑不变量的值,通过占据额外的状态在反转中心,同时保持体极化固定。我们讨论了我们的研究结果的影响,在高维电子系统中的拓扑结晶相,并在超冷原子系统。

英文摘要:

When translational symmetry is broken by bulk disorder, the topological nature of states in topological crystalline systems may change depending on the type of disorder that is applied. In this work, we characterize the phases of a one-dimensional (1D) chain with inversion and chiral symmetries, where every disorder configuration is inversion-symmetric. By using a basis-independent formulation for the inversion topological invariant, chiral winding number, and bulk polarization, we are able to construct phase diagrams for these quantities when disorder is present. We show that unlike the chiral winding number and bulk polarization, the inversion topological invariant can fluctuate when the bulk spectral gap closes at strong disorder. Using the position-space renormalization group, we are able to compare how the inversion topological invariant, chiral winding number and bulk polarization behave at low energies in the strong disorder limit. We show that with inversion symmetry-preserving disorder, the value of the inversion topological invariant is determined by the inversion eigenvalues of the states at the inversion centers, while quantities such as the chiral winding number and the bulk polarization still have contributions from every state throughout the chain. We also show that it is possible to alter the value of the inversion topological invariant in a clean system by occupying additional states at the inversion centers while keeping the bulk polarization fixed. We discuss the implications of our results for topological crystalline phases in higher-dimensional electronic systems, and in ultra-cold atomic systems.

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