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二维q态量子Potts模型中的简并基态与多重分岔

Degenerate ground states and multiple bifurcations in a two-dimensional q-state quantum Potts model.

作者信息

Dai Yan-Wei, Cho Sam Young, Batchelor Murray T, Zhou Huan-Qiang

机构信息

Centre for Modern Physics and Department of Physics, Chongqing University, Chongqing 400044, People's Republic of China.

Centre for Modern Physics and Department of Physics, Chongqing University, Chongqing 400044, People's Republic of China and Department of Theoretical Physics and Mathematical Science Institute, Australian National University, Canberra, ACT 0200, Australia.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2014 Jun;89(6):062142. doi: 10.1103/PhysRevE.89.062142. Epub 2014 Jun 30.

Abstract

We numerically investigate the two-dimensional q-state quantum Potts model on the infinite square lattice by using the infinite projected entangled-pair state (iPEPS) algorithm. We show that the quantum fidelity, defined as an overlap measurement between an arbitrary reference state and the iPEPS ground state of the system, can detect q-fold degenerate ground states for the Z_{q} broken-symmetry phase. Accordingly, a multiple bifurcation of the quantum ground-state fidelity is shown to occur as the transverse magnetic field varies from the symmetry phase to the broken-symmetry phase, which means that a multiple-bifurcation point corresponds to a critical point. A (dis)continuous behavior of quantum fidelity at phase transition points characterizes a (dis)continuous phase transition. Similar to the characteristic behavior of the quantum fidelity, the magnetizations, as order parameters, obtained from the degenerate ground states exhibit multiple bifurcation at critical points. Each order parameter is also explicitly demonstrated to transform under the Z_{q} subgroup of the symmetry group of the Hamiltonian. We find that the q-state quantum Potts model on the square lattice undergoes a discontinuous (first-order) phase transition for q=3 and q=4 and a continuous phase transition for q=2 (the two-dimensional quantum transverse Ising model).

摘要

我们使用无限投影纠缠对态(iPEPS)算法对无限方形晶格上的二维q态量子Potts模型进行了数值研究。我们表明,量子保真度被定义为任意参考态与系统的iPEPS基态之间的重叠测量,可以检测Z_q破缺对称相的q重简并基态。因此,随着横向磁场从对称相变化到破缺对称相,量子基态保真度会出现多重分岔,这意味着多重分岔点对应于一个临界点。量子保真度在相变点的(不)连续行为表征了(不)连续相变。与量子保真度的特征行为类似,作为序参量的磁化强度,从简并基态获得,在临界点处表现出多重分岔。每个序参量也被明确证明在哈密顿量对称群的Z_q子群下发生变换。我们发现,方形晶格上的q态量子Potts模型在q = 3和q = 4时经历不连续(一阶)相变,在q = 2时(二维量子横向Ising模型)经历连续相变。

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