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Tensor-entanglement Renormalization Group Approach As A Unified Method For Symmetrybreaking And Topological Phase Transitions

机译:张量纠缠重整化组方法作为对称性破缺和拓扑相变的统一方法

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摘要

Traditional mean-field theory is a generic variational approach for analyzing symmetry breaking phases. However, this simple approach only applies to symmetry breaking states with short-range entanglement. In this paper, we describe a generic approach for studying two-dimensional (2D) quantum phases with long-range entanglement (such as topological phases). The method is based on (a) a general class of trial wave functions known as tensor-product states and (b) a 2D real-space renormalization group algorithm for efficiently calculating expectation values for these states. We demonstrate our method by studying several simple 2D quantum spin models exhibiting both symmetry breaking phase transitions and topological phase transitions. Our approach can be viewed as a unified mean-field theory for both symmetry breaking phases and topological phases.
机译:传统的平均场理论是一种用于分析对称断裂相的通用变分方法。但是,此简单方法仅适用于具有短程纠缠的对称破坏状态。在本文中,我们描述了一种用于研究具有长距离纠缠的二维(2D)量子相(例如拓扑相)的通用方法。该方法基于(a)一类普通的试验波函数,即张量积状态;(b)一种2D实空间重归一化组算法,用于有效地计算这些状态的期望值。我们通过研究几个简单的2D量子自旋模型来展示我们的方法,该模型同时显示对称性破坏相变和拓扑相变。我们的方法可以看作是对称断裂阶段和拓扑阶段的统一平均场理论。

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