无序SU(2)-对称Floquet系统的扩展非遍历区和自旋亚扩散

Zhi-Cheng Yang, Stuart Nicholls, M. Cheng
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引用次数: 4

摘要

我们研究了一维无序SU(2)对称Floquet模型中的热化和量子动力学,其中多体局域相被非阿贝尔对称所禁止。尽管缺乏局域化,我们发现在强无序状态下系统表现出非热行为的扩展非过能状态。在强无序状态下,能级间隔统计量既不表现Wigner-Dyson分布,也不表现泊松分布,谱形式因子也不表现随机矩阵理论的早期线性增长特征。Floquet本征态的平均纠缠熵是亚热的,尽管违反了与系统尺寸成比例的面积定律。我们进一步计算了局部观测值的期望值,并发现了与本征态热化假设的强烈偏差。无限温度自旋自相关函数在长时间衰减为$t^{-\beta}$且$\beta < 0.5$,表明在强失序下存在亚扩散输运。
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Extended nonergodic regime and spin subdiffusion in disordered SU(2)-symmetric Floquet systems
We explore thermalization and quantum dynamics in a one-dimensional disordered SU(2)-symmetric Floquet model, where a many-body localized phase is prohibited by the non-abelian symmetry. Despite the absence of localization, we find an extended nonergodic regime at strong disorder where the system exhibits nonthermal behaviors. In the strong disorder regime, the level spacing statistics exhibit neither a Wigner-Dyson nor a Poisson distribution, and the spectral form factor does not show a linear-in-time growth at early times characteristic of random matrix theory. The average entanglement entropy of the Floquet eigenstates is subthermal, although violating an area-law scaling with system sizes. We further compute the expectation value of local observables and find strong deviations from the eigenstate thermalization hypothesis. The infinite temperature spin autocorrelation function decays at long times as $t^{-\beta}$ with $\beta < 0.5$, indicating subdiffusive transport at strong disorders.
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