从 (2+1) D可逆费米子状态和霍夫斯塔德的蝶中部分旋转的完整晶体拓不变数
Yuxuan Zhang1, Naren Manjunath1, Ryohei Kobayashi1
1Department of Physics, Joint Quantum Institute, and Condensed Matter Theory Center, University of Maryland, College Park, Maryland 20742, USA.
Physical review letters
|November 13, 2023
概括
研究人员开发了一种方法,可以在 (2+1) D 费米子状态下从晶体对称中提取拓不变量,即使有磁场. 这提供了拓阶段的完整表征,适用于像霍夫斯塔德特这样的模型.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 关于物质的拓阶段
- 晶体对称性是指晶体对称性的
背景情况:
- 物质的拓相具有由晶体对称性保护的不变量.
- 从微观计算中提取这些不变量一直是具有挑战性的.
研究的目的:
- 开发一种从微观计算中提取多体拓不变量的一般方法.
- 在 (2+1) D可逆费米子系统中提供拓状态的完整表征.
主要方法:
- 在 (2+1) D Fermionic 状态中使用部分旋转提取多体不变量 {Θ_{o}^{±}} .
- 在存在磁场和非零的切尔恩数的情况下应用该方法.
- 在正方形格子霍夫斯塔德模型上的数值计算.
主要成果:
- 一组多体不变数{Θ_{o}^{±}}被成功提取出来.
- 这些不变数,以及切尔恩数 (C),奇拉中心电荷 (c_{-}) 和填充 (ν),完全描述了拓状态.
- 从单个散装基本状态中获得了不变量,没有额外的缺陷.
- 数值结果与合规和拓场理论计算一致.
结论:
- 开发的方法提供了一种强大的方法来识别和描述由晶体对称性保护的拓相.
- 这些发现扩大了对拓相的理解,特别是在具有磁场的系统中.
- 结果为霍夫斯塔德的蝶光谱和拓量子化学提供了新的见解.
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