The General Principle behind Magnetization-induced Second-Order Topological Corner States in the Kane-Mele Model

Fuente: arXiv
Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: Miao, Cheng-Ming, Liu, Lizhou, Wan, Yu-Hao, Sun, Qing-Feng, Zhang, Ying-Tao
Format: Preprint
Veröffentlicht: 2024
Schlagworte:
Online-Zugang:
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
_version_ 1866908347854225408
author Miao, Cheng-Ming
Liu, Lizhou
Wan, Yu-Hao
Sun, Qing-Feng
Zhang, Ying-Tao
author_facet Miao, Cheng-Ming
Liu, Lizhou
Wan, Yu-Hao
Sun, Qing-Feng
Zhang, Ying-Tao
contents We propose a general principle for realizing second-order topological corner states in the modified Kane-Mele model with magnetization. It is demonstrated that the sign of the edge Dirac mass depends on the magnetization of the edge sublattice termination. By adjusting the directions of magnetization according to the type of sublattice at the termination of two edges, a mass domain wall can be induced in the presence of topological corner states at an arbitrary position. All previous work on introducing magnetization in the Kane-Mele model to realize second-order topological corner states can be explained by the presence of the Dirac mass domain wall with opposite signs. Applying this principle, we design square-shaped and armchair-type hexagon-shaped graphene nanoflakes with edge magnetization, allowing for the emergence of second-order topological corner states. Our findings serve as a general theory, demonstrating that the realization of second-order topological corner states is not limited by boundary type or nanoflake shape.
format Preprint
id arxiv_https___arxiv_org_abs_2403_02017
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle The General Principle behind Magnetization-induced Second-Order Topological Corner States in the Kane-Mele Model
Miao, Cheng-Ming
Liu, Lizhou
Wan, Yu-Hao
Sun, Qing-Feng
Zhang, Ying-Tao
Mesoscale and Nanoscale Physics
We propose a general principle for realizing second-order topological corner states in the modified Kane-Mele model with magnetization. It is demonstrated that the sign of the edge Dirac mass depends on the magnetization of the edge sublattice termination. By adjusting the directions of magnetization according to the type of sublattice at the termination of two edges, a mass domain wall can be induced in the presence of topological corner states at an arbitrary position. All previous work on introducing magnetization in the Kane-Mele model to realize second-order topological corner states can be explained by the presence of the Dirac mass domain wall with opposite signs. Applying this principle, we design square-shaped and armchair-type hexagon-shaped graphene nanoflakes with edge magnetization, allowing for the emergence of second-order topological corner states. Our findings serve as a general theory, demonstrating that the realization of second-order topological corner states is not limited by boundary type or nanoflake shape.
title The General Principle behind Magnetization-induced Second-Order Topological Corner States in the Kane-Mele Model
topic Mesoscale and Nanoscale Physics
url https://arxiv.org/abs/2403.02017