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滑移-Z 磁拓扑光子晶体的理论分析

Theoretical analysis of glide-Z magnetic topological photonic crystals.

作者信息

Kim Heejae, Cheng Hengbin, Lu Ling, Murakami Shuichi

出版信息

Opt Express. 2021 Sep 27;29(20):31164-31178. doi: 10.1364/OE.439590.

Abstract

Gapped systems with glide symmetry can be characterized by a Z topological invariant. We study the magnetic photonic crystal with a gap between the second and third lowest bands, which is characterized by the nontrivial glide-Z topological invariant that can be determined by symmetry-based indicators. We show that under the space group No. 230 ( 3¯), the topological invariant is equal to a half of the number of photonic bands below the gap. Therefore, the band gap between the second and third lowest bands is always topologically nontrivial, and to realize the topological phase, we need to open a gap for the Dirac point at the P point by breaking time-reversal symmetry. With staggered magnetization, the photonic bands are gapped and the photonic crystal becomes topological, whereas with uniform magnetization, a gap does not open, which can be attributed to the minimal band connectivity exceeding two in this case. By introducing the notion of Wyckoff positions, we show how the topological characteristics are determined from the structure of the photonic crystals.

摘要

具有滑移对称性的带隙系统可以用Z拓扑不变量来表征。我们研究了在第二和第三低能带之间存在带隙的磁光子晶体,其特征在于非平凡的滑移-Z拓扑不变量,该不变量可以由基于对称性的指标来确定。我们表明,在空间群No. 230(3¯)下,拓扑不变量等于带隙以下光子能带数量的一半。因此,第二和第三低能带之间的带隙总是拓扑非平凡的,并且为了实现拓扑相,我们需要通过打破时间反演对称性来为P点处的狄拉克点打开一个带隙。对于交错磁化,光子能带出现带隙,光子晶体变为拓扑结构,而对于均匀磁化,带隙不会打开,这可以归因于在这种情况下最小能带连通性超过了2。通过引入魏格纳位置的概念,我们展示了如何从光子晶体的结构确定拓扑特征。

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