Unveiling correlated two-dimensional topological insulators through fermionic tensor network states-classification, edge theories and variational wavefunctions.

Chao Xu, Yixin Ma, Shenghan Jiang
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Abstract

The study of topological band insulators has revealed fascinating phases characterized by band topology indices and anomalous boundary modes protected by global symmetries. In strongly correlated systems, where the traditional notion of electronic bands becomes obsolete, it has been established that topological insulator phases persist as stable phases, separate from the trivial insulators. However, due to the inability to express the ground states of such systems as Slater determinants, the formulation of generic variational wave functions for numerical simulations is highly desirable. In this paper, we tackle this challenge for two-dimensional topological insulators by developing a comprehensive framework for fermionic tensor network states. Starting from simple assumptions, we obtain possible sets of tensor equations for any given symmetry group, capturing consistent relations governing symmetry transformation rules on tensor legs. We then examine the connection between these tensor equations andnon-chiraltopological insulators by constructing edge theories and extracting quantum anomaly data from each set of tensor equations. By exhaustively exploring all possible sets of equations, we achieve a systematic classification of non-chiral topological insulator phases. Imposing the solutions of a given set of equations onto local tensors, we obtain generic variational wavefunctions for the corresponding topological insulator phases. Our methodology provides an important step toward simulating topological insulators in strongly correlated systems. We discuss the limitations and potential generalizations of our results, paving the way for further advancements in this field.

通过费米子张量网络状态揭示相关的二维拓扑绝缘体--分类、边缘理论和变异波函数。
对拓扑带绝缘体的研究揭示了以带拓扑指数和受全局对称性保护的反常边界模式为特征的迷人相位。在强相关系统中,传统的电子带概念已经过时,拓扑绝缘体相作为稳定相存在,与微带绝缘体分离。然而,由于无法用斯莱特行列式来表达这类系统的基态,因此非常有必要制定用于数值模拟的通用变分波函数 在本文中,我们通过开发费米张量网络态的综合框架来解决二维拓扑绝缘体的这一难题。从简单的假设出发,我们为任何给定的对称群获得了可能的张量方程组,捕捉了张量腿对称变换规则的一致关系。然后,我们通过解释边缘理论和从每组张量方程中提取量子反常数据,研究这些张量方程与非手性拓扑绝缘体之间的联系。通过详尽探索所有可能的方程组,我们实现了对非手性拓扑绝缘体相位的系统分类。将给定方程组的解施加到局部张量上,我们就能得到相应拓扑绝缘体相的通用变分波函数。我们的方法为模拟强相关系统中的拓扑绝缘体迈出了重要一步。我们讨论了我们结果的局限性和潜在的推广性,为这一领域的进一步发展铺平了道路。
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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