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Takagi topological insulator with oddPTpairs of corner states
Physical Review B ( IF 3.2 ) Pub Date : 2021-10-25 , DOI: 10.1103/physrevb.104.165142
Jia-Xiao Dai 1 , Kai Wang 1 , Shengyuan A. Yang 2 , Y. X. Zhao 1, 3
Affiliation  

We present a novel class of topological insulators, termed the Takagi topological insulators (TTIs), which is protected by the sublattice symmetry and space-time inversion (PT) symmetry. The required symmetries for the TTIs can be realized on any bipartite lattice where the inversion exchanges sublattices. The protecting symmetries lead to the classifying space of Hamiltonians being unitary symmetric matrices, and therefore Takagi's factorization can be performed. Particularly, the global Takagi's factorization can (cannot) be done on a 3D (2D) sphere. In 3D, there is a Z2 topological invariant corresponding to the parity of the winding number of Takagi's unitary-matrix factor over the entire Brillouin zone, where the Z2 nature comes from the O(N) gauge degrees of freedom in Takagi's factorization. In 2D, the obstruction for a global Takagi's factorization is characterized by another Z2 topological invariant, equivalent to the second Stiefel-Whitney number. For the third-order topological phases, the 3D TTIs feature a parity condition for corner zero modes, i.e., there always exist odd PT pairs of corners with zero modes. Moreover, for any PT invariant sample geometry, all configurations of corner zero modes satisfying the parity condition can exist with the same nontrivial bulk topological invariant. Actually, without closing the bulk gap, the boundary phase diagram has a cellular structure, where each topological boundary phase associated with a particular (cross-order) boundary-mode pattern corresponds to a contractible cell with a certain dimension in the parameter space.

中文翻译:

具有奇数PT对角态的高木拓扑绝缘体

我们提出了一类新的拓扑绝缘体,称为高木拓扑绝缘体(TTI),它受到亚晶格对称性和时空反转的保护。) 对称性。TTI 所需的对称性可以在反演交换亚格的任何二分格上实现。保护对称性导致哈密顿量的分类空间是酉对称矩阵,因此可以进行高木因式分解。特别是,全局 Takagi 的分解可以(不能)在一个3D (2D) 球体。在 3D 中,有一个Z2 对应于整个布里渊区的高木酉矩阵因子的绕数奇偶性的拓扑不变量,其中 Z2 大自然来自 (N)Takagi 分解中的规范自由度。在 2D 中,全局 Takagi 分解的障碍的特征在于另一个Z2拓扑不变量,相当于第二个 Stiefel-Whitney 数。对于三阶拓扑相,3D TTI 具有角零模式的奇偶校验条件,即始终存在奇数 具有零模式的角对。此外,对于任何不变的样本几何,满足奇偶性条件的所有角零模式配置都可以以相同的非平凡体拓扑不变量存在。实际上,在没有关闭体间隙的情况下,边界相图具有细胞结构,其中与特定(跨阶)边界模式模式相关的每个拓扑边界相对应于参数空间中具有特定维度的可收缩单元。
更新日期:2021-10-26
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