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二维中具有旋转拓扑不变量的反铁磁二阶能带拓扑设计

Design of Antiferromagnetic Second-Order Band Topology with Rotation Topological Invariants in Two Dimensions.

作者信息

Zhan Fangyang, Qin Zheng, Xu Dong-Hui, Zhou Xiaoyuan, Ma Da-Shuai, Wang Rui

机构信息

Institute for Structure and Function & Department of Physics & Chongqing Key Laboratory for Strongly Coupled Physics, Chongqing University, Chongqing 400044, People's Republic of China.

Center of Quantum materials and devices, Chongqing University, Chongqing 400044, People's Republic of China.

出版信息

Nano Lett. 2024 Jun 26;24(25):7741-7747. doi: 10.1021/acs.nanolett.4c01817. Epub 2024 Jun 13.

Abstract

The existence of fractionally quantized topological corner charge serves as a key indicator for two-dimensional (2D) second-order topological insulators (SOTIs), yet it has not been experimentally observed in realistic materials. Here, based on effective model analysis and symmetry arguments, we propose a strategy for achieving SOTI phases with in-gap corner states in 2D systems with antiferromagnetic (AFM) order. We discover that the band topology originates from the interplay between intrinsic spin-orbital coupling and interlayer AFM exchange interactions. Using first-principles calculations, we show that the 2D AFM SOTI phase can be realized in (MnBiTe)(BiTe) films. Moreover, we demonstrate that the SOTI states are linked to rotation topological invariants under 3-fold rotation symmetry , resulting in fractionally quantized corner charge, i.e., (mod ). Due to the great achievements in (MnBiTe)(BiTe) systems, our results providing reliable material candidates for experimentally accessible AFM SOTIs should draw intense attention.

摘要

分数化量子化拓扑角电荷的存在是二维(2D)二阶拓扑绝缘体(SOTIs)的关键指标,然而在实际材料中尚未通过实验观测到。在此,基于有效模型分析和对称性论证,我们提出了一种策略,用于在具有反铁磁(AFM)序的二维系统中实现具有能隙角态的SOTI相。我们发现能带拓扑起源于本征自旋 - 轨道耦合与层间AFM交换相互作用之间的相互作用。通过第一性原理计算,我们表明二维AFM SOTI相可以在(MnBiTe)(BiTe)薄膜中实现。此外,我们证明SOTI态与三重旋转对称性下的旋转拓扑不变量相关联,从而导致分数化量子化角电荷,即 (模 )。由于(MnBiTe)(BiTe)系统取得的重大进展,我们的结果为实验上可实现的AFM SOTIs提供了可靠的材料候选者,应引起广泛关注。

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