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arXiv 1010.3732cond-mat.str-elquant-ph
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使用矩阵积态和PEPS对量子相进行分类

Classifying quantum phases using Matrix Product States and PEPS

Norbert Schuch, David Perez-Garcia, Ignacio Cirac

摘要:

在矩阵乘积态(MPS)及其相关的父哈密顿量的框架下,对具有唯一和简并基态的一维系统,在对称性存在和不存在的情况下,给出了带隙量子相位的分类.我们发现,没有对称性,所有的系统是在同一个阶段,直到偶然的基态简并。如果强加对称性,则没有对称性破坏的相位(即,具有唯一基态)按对称群的上同调类,即其射影表示的等价类进行分类,这是[X. Chen,Z. - C. Gu和X。- G. Wen,Phys.Rev.B83,035107(2011); arXiv:1008.3745]。对于具有对称性破坏的相位(即,简并基态),我们发现对称性由两部分组成,一部分作用于基态的置换作用,另一部分作用于单个基态,相位由前者的置换作用和后者的上同调类来标记.使用投影纠缠对状态(PEPS),我们随后扩展我们的框架,在一些重要的情况下,在特定的系统具有独特的基态,退化的基态与当地的序参量,和拓扑顺序的附近的二维相位的分类。我们还表明,在两个维度上,施加对称性并不约束的相图在一维的方式。作为一个中心工具,我们介绍了等距形式,规范形式的MPS和PEPS,这是一个重整化不动点。将一个状态变换为它的等距形式并不改变相位,因此,我们可以把重点放在等距形式的分类上。

英文摘要:

We give a classification of gapped quantum phases of one-dimensional systems in the framework of Matrix Product States (MPS) and their associated parent Hamiltonians, for systems with unique as well as degenerate ground states, and both in the absence and presence of symmetries. We find that without symmetries, all systems are in the same phase, up to accidental ground state degeneracies. If symmetries are imposed, phases without symmetry breaking (i.e., with unique ground states) are classified by the cohomology classes of the symmetry group, this is, the equivalence classes of its projective representations, a result first derived in [X. Chen, Z.-C. Gu, and X.-G. Wen, Phys. Rev. B 83, 035107 (2011); arXiv:1008.3745]. For phases with symmetry breaking (i.e., degenerate ground states), we find that the symmetry consists of two parts, one of which acts by permuting the ground states, while the other acts on individual ground states, and phases are labelled by both the permutation action of the former and the cohomology class of the latter. Using Projected Entangled Pair States (PEPS), we subsequently extend our framework to the classification of two-dimensional phases in the neighborhood of a number of important cases, in particular systems with unique ground states, degenerate ground states with a local order parameter, and topological order. We also show that in two dimensions, imposing symmetries does not constrain the phase diagram in the same way it does in one dimension. As a central tool, we introduce the isometric form, a normal form for MPS and PEPS which is a renormalization fixed point. Transforming a state to its isometric form does not change the phase, and thus, we can focus on to the classification of isometric forms.

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