论文标题
来自弱的恐怖性破裂的均匀浮标时间晶体
Homogeneous Floquet time crystal from weak ergodicity breaking
论文作者
论文摘要
关于观察离散时晶体特征的最新著作引发了稳定这种平衡阶段的本地化的必要性。在这些研究的激励下,我们深入研究了一个干净的相互作用的浮子系统,其准谱符合奇异的wigner-dyson分布,但在没有混乱或精细调节的情况下具有出乎意料的稳健,长期寿命的时间晶状体动力学。我们将这种行为与具有远距离空间相关性的零值的非热浮子本征量相关联,该体系与近距离的空间相关性在近距离温度下与其他热状态共存,并与翻译不变的,对称性,交换性交换的初始条件相关。这类似于“动力疤痕”的概念,这些概念在整个浮力频谱中保持着牢固的位置,并具有破裂的结构。我们将这种长寿的离散时间晶体列为部分非连续系统形成,“疤痕分离的时间晶体”,本质上与被多体定位或预防机制稳定的晶体不同。
Recent works on observation of discrete time-crystalline signatures throw up major puzzles on the necessity of localization for stabilizing such out-of-equilibrium phases. Motivated by these studies, we delve into a clean interacting Floquet system, whose quasi-spectrum conforms to the ergodic Wigner-Dyson distribution, yet with an unexpectedly robust, long-lived time-crystalline dynamics in the absence of disorder or fine-tuning. We relate such behavior to a measure zero set of nonthermal Floquet eigenstates with long-range spatial correlations, which coexist with otherwise thermal states at near-infinite temperature and develop a high overlap with a family of translationally invariant, symmetry-broken initial conditions. This resembles the notion of "dynamical scars" that remain robustly localized throughout a thermalizing Floquet spectrum with fractured structure. We dub such a long-lived discrete time crystal formed in partially nonergodic systems, "scarred discrete time crystal" which is distinct by nature from those stabilized by either many-body localization or prethermalization mechanism.