A lattice formulation of Weyl fermions on a single curved surface

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
Shoto Aoki, Hidenori Fukaya, Naoto Kan
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引用次数: 0

Abstract

In the standard lattice domain-wall fermion formulation, one needs two flat domain-walls where both of the left- and right-handed massless modes appear. In this work we investigate a single domain-wall system with a nontrivial curved background. Specifically we consider a massive fermion on a three-dimensional square lattice, whose domain-wall is a two-dimensional sphere. In the free theory, we find that a single Weyl fermion is localized at the wall and it feels gravity through the induced spin connection. With a topologically nontrivial U(1) link gauge field, however, we find a zero mode with the opposite chirality localized at the center where the gauge field is singular. In the latter case, the low-energy effective theory is not chiral but vectorlike. We discuss how to circumvent this obstacle in formulating lattice chiral gauge theory in the single domain-wall fermion system.
单个弯曲表面上韦尔费米子的晶格模型
在标准晶格畴壁费米子公式中,需要两个平坦的畴壁,其中同时出现左手和右手无质量模式。在这项工作中,我们研究了一个具有非对称曲线背景的单域壁系统。具体来说,我们考虑了三维方格上的大质量费米子,其域壁是一个二维球体。在自由理论中,我们发现单个韦尔费米子被定位在壁面上,并通过诱导自旋连接感受引力。然而,当存在拓扑非琐碎的 U(1) 链接量规场时,我们会发现在量规场奇异的中心位置存在一个具有相反手性的零模。在后一种情况下,低能有效理论不是手性理论,而是矢量理论。我们将讨论如何在单域壁费米子系统中绕过这一障碍,提出晶格手性规理论。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
7.20
自引率
4.30%
发文量
567
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