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Discrete truncated Wigner approach to dynamical phase transitions in Ising models after a quantum quench

机译:Quantum淬火后in Ising模型中的离散截短的Wigner方法

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摘要

By means of the discrete truncated Wigner approximation, we study dynamical phase transitions arising in the steady state of transverse-field Ising models after a quantum quench. Starting from a fully polarized ferromagnetic initial condition, these transitions separate a phase with nonvanishing magnetization along the ordering direction from a disordered symmetric phase upon increasing the transverse field. We consider two paradigmatic cases, a one-dimensional long-range model with power-law interactions ∝ 1/r~α decaying algebraically as a function of distance r and a two-dimensional system with short-range nearest-neighbor interactions. In the former case, we identify dynamical phase transitions for α approx< 2 and we extract the critical exponents from a data collapse of the steady-state magnetization for up to 1200 lattice sites. We find identical exponents for a approx< 0.5, suggesting that the dynamical transitions in this regime fall into the same universality class as the nonergodic mean-field limit. The two-dimensional Ising model is believed to be thermalizing, which we also confirm using exact diagonalization for small system sizes. Thus, the dynamical transition is expected to correspond to the thermal phase transition, which is consistent with our data upon comparing to equilibrium quantum Monte Carlo simulations. We further test the accuracy of the discrete truncated Wigner approximation by comparing against numerically exact methods such as exact diagonalization, tensor network, as well as artificial neural network states and we find good quantitative agreement on the accessible time scales. Finally, our work provides an additional contribution to the understanding of the range and the limitations of qualitative and quantitative applicability of the discrete truncated Wigner approximation.
机译:借助于离散截短的Wigner近似,我们在量子淬火之后研究在横向场均匀模型的稳定状态下产生的动态相变。从完全偏振的铁磁性初始条件开始,这些过渡在增加横向场时从无序对称相位与排序方向分离出具有非衰弱磁化的相位。我们考虑了两种范式的情况,具有电力 - 律相互作用α1/ R〜α的一维远程模型作为距离R和具有短程最近邻相互作用的距离R和二维系统的代数衰减。在前一种情况下,我们确定α的动态相变大约<2,我们从稳态磁化的数据崩溃中提取临界指数,最多1200个格子位点。我们发现相同的指数为约<0.5,表明该制度的动态转变落入与非精通均值场限制相同的普遍性课程。认为二维读取模型被认为是热化的,我们还通过对小型系统尺寸进行精确的对角确认。因此,预期动态转变将对应于热相转变,其在比较与均衡量子蒙特卡罗模拟时与我们的数据一致。我们进一步测试了离散截断的Wigner近似的准确性,通过与数值精确的方法(如精确的对角化,张量网络)以及人工神经网络状态进行比较,并且我们在可访问的时间尺度上找到良好的定量协议。最后,我们的工作为对离散截短的WIGNER近似的定性和定量适用性的理解提供了额外的贡献。

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  • 来源
    《Physical review》 |2020年第1期|014303.1-014303.14|共14页
  • 作者单位

    Abdus Salam ICTP Strada Costiera 11 1-34151 Trieste Italy Department of Physics Institute for Advanced Studies in Basic Sciences (IASBS) Zanjan 45137-66731 Iran;

    Max-Planck-Institut fuer Physik Komplexer Systeme Noethnitzer Strasse 38 D-01187 Dresden Germany;

    Department of Physics University of California at Berkeley Berkeley California 94720 USA;

    Max-Planck-Institut fuer Physik Komplexer Systeme Noethnitzer Strasse 38 D-01187 Dresden Germany;

    Abdus Salam ICTP Strada Costiera 11 1-34151 Trieste Italy Dipartimento di Fisica Universita di Napoli Federico Ⅱ Monte S. Angelo 1-80126 Napoli Italy;

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