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非厄米半狄拉克半金属

Non-Hermitian semi-Dirac semi-metals.

作者信息

Banerjee Ayan, Narayan Awadhesh

机构信息

Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560012, India.

出版信息

J Phys Condens Matter. 2021 May 5;33(22). doi: 10.1088/1361-648X/abe796.

Abstract

Recently, many novel and exotic phases have been proposed by considering the role of topology in non-Hermitian systems, and their emergent properties are of wide current interest. In this work we propose the non-Hermitian generalization of semi-Dirac semimetals, which feature a linear dispersion along one momentum direction and a quadratic one along the other. We study the topological phase transitions in such two-dimensional semi-Dirac semimetals in the presence of a particle gain-and-loss term. We show that such a non-Hermitian term creates exceptional points (EPs) originating out of each semi-Dirac point. We map out the topological phase diagram of our model, using winding number and vorticity as topological invariants of the system. By means of numerical and analytical calculations, we examine the nature of edge states for different types of semi-Dirac models and establish bulk-boundary correspondence and absence of the non-Hermitian skin effect, in one class. On the other hand, for other classes of semi-Dirac models with asymmetric hopping, we restore the non-Hermitian skin effect, an anomalous feature usually present in non-Hermitian topological systems.

摘要

最近,通过考虑拓扑结构在非厄米系统中的作用,人们提出了许多新奇且奇特的相,它们的涌现特性目前引起了广泛关注。在这项工作中,我们提出了半狄拉克半金属的非厄米推广,其特征是在一个动量方向上具有线性色散,而在另一个方向上具有二次色散。我们研究了在存在粒子增益和损耗项的情况下,这种二维半狄拉克半金属中的拓扑相变。我们表明,这样一个非厄米项会产生源自每个半狄拉克点的例外点(EPs)。我们使用缠绕数和涡度作为系统的拓扑不变量,绘制出了我们模型的拓扑相图。通过数值和解析计算,我们研究了不同类型半狄拉克模型的边缘态性质,并在一类模型中建立了体边对应关系以及不存在非厄米趋肤效应。另一方面,对于具有不对称跳跃的其他类半狄拉克模型,我们恢复了非厄米趋肤效应,这是通常存在于非厄米拓扑系统中的一种反常特征。

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