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用于三维拓扑模型的各向异性缩放

Anisotropic scaling for 3D topological models.

作者信息

Rufo S, Griffith M A R, Lopes Nei, Continentino Mucio A

机构信息

Beijing Computational Science Research Center, Beijing, 100193, China.

CeFEMA, Instituto Superior Técnico, Universidade de Lisboa, Av. Rovisco Pais, 1049-001, Lisbon, Portugal.

出版信息

Sci Rep. 2021 Nov 18;11(1):22524. doi: 10.1038/s41598-021-01888-x.

DOI:10.1038/s41598-021-01888-x
PMID:34795344
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8602304/
Abstract

A proposal to study topological models beyond the standard topological classification and that exhibit breakdown of Lorentz invariance is presented. The focus of the investigation relies on their anisotropic quantum critical behavior. We study anisotropic effects on three-dimensional (3D) topological models, computing their anisotropic correlation length critical exponent [Formula: see text] obtained from numerical calculations of the penetration length of the zero-energy surface states as a function of the distance to the topological quantum critical point. A generalized Weyl semimetal model with broken time-reversal symmetry is introduced and studied using a modified Dirac equation. An approach to characterize topological surface states in topological insulators when applied to Fermi arcs allows to capture the anisotropic critical exponent [Formula: see text]. We also consider the Hopf insulator model, for which the study of the topological surface states yields unusual values for [Formula: see text] and for the dynamic critical exponent z. From an analysis of the energy dispersions, we propose a scaling relation [Formula: see text] and [Formula: see text] for [Formula: see text] and z that only depends on the Hopf insulator Hamiltonian parameters p and q and the axis direction [Formula: see text]. An anisotropic quantum hyperscaling relation is also obtained.

摘要

本文提出了一项研究超越标准拓扑分类且表现出洛伦兹不变性破缺的拓扑模型的提议。研究重点在于它们的各向异性量子临界行为。我们研究了三维(3D)拓扑模型中的各向异性效应,通过计算零能表面态穿透长度作为到拓扑量子临界点距离的函数的数值计算,得到其各向异性关联长度临界指数[公式:见原文]。引入了一个具有时间反演对称性破缺的广义外尔半金属模型,并使用修正的狄拉克方程对其进行研究。当应用于费米弧时,一种表征拓扑绝缘体中拓扑表面态的方法能够捕捉各向异性临界指数[公式:见原文]。我们还考虑了霍普夫绝缘体模型,对其拓扑表面态的研究得出了[公式:见原文]和动态临界指数z的异常值。通过对能量色散的分析,我们提出了一个仅依赖于霍普夫绝缘体哈密顿量参数p和q以及轴方向[公式:见原文]的[公式:见原文]和z的标度关系[公式:见原文]。还得到了一个各向异性量子超标度关系。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/26f449ed1a8e/41598_2021_1888_Fig10_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/82d7c5caaad7/41598_2021_1888_Fig2_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/b71721043051/41598_2021_1888_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/7e29e5ffa74c/41598_2021_1888_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/7347809009e3/41598_2021_1888_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/129d6429f449/41598_2021_1888_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/fe499533743d/41598_2021_1888_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e782/8602304/26f449ed1a8e/41598_2021_1888_Fig10_HTML.jpg

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