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遍历性破坏对任意扰动具有可证明的鲁棒性。

Ergodicity Breaking Provably Robust to Arbitrary Perturbations.

作者信息

Stephen David T, Hart Oliver, Nandkishore Rahul M

机构信息

Department of Physics and Center for Theory of Quantum Matter, University of Colorado Boulder, Boulder, Colorado 80309, USA.

Department of Physics, California Institute of Technology, Pasadena, California 91125, USA.

出版信息

Phys Rev Lett. 2024 Jan 26;132(4):040401. doi: 10.1103/PhysRevLett.132.040401.

Abstract

We present a new route to ergodicity breaking via Hilbert space fragmentation that displays an unprecedented level of robustness. Our construction relies on a single emergent (prethermal) conservation law. In the limit when the conservation law is exact, we prove the emergence of Hilbert space fragmentation with an exponential number of frozen configurations. These configurations are low-entanglement states in the middle of the energy spectrum and therefore constitute examples of quantum many-body scars. We further prove that every frozen configuration is absolutely stable to arbitrary perturbations, to all finite orders in perturbation theory. In contrast to previous constructions, our proof is not limited to symmetric perturbations, or to perturbations with compact support, but also applies to perturbations with long-range tails, and even to arbitrary geometrically nonlocal k-body perturbations, as long as k/L→0 in the thermodynamic limit, where L is linear system size. Additionally, we identify one-form U(1) charges characterizing some nonfrozen sectors, and discuss the dynamics starting from typical initial conditions, which we argue is best interpreted in terms of the magnetohydrodynamics of the emergent one-form symmetry.

摘要

我们提出了一种通过希尔伯特空间碎片化实现遍历性破缺的新途径,该途径展现出了前所未有的稳健性。我们的构建依赖于一个单一的涌现(预热)守恒定律。在守恒定律精确成立的极限情况下,我们证明了具有指数数量冻结构型的希尔伯特空间碎片化的出现。这些构型是能谱中间的低纠缠态,因此构成了量子多体伤疤的例子。我们进一步证明,在微扰理论的所有有限阶下,每个冻结构型对任意微扰都是绝对稳定的。与先前的构建不同,我们的证明不限于对称微扰或具有紧支集的微扰,还适用于具有长程尾部的微扰,甚至适用于任意几何非局域的k体微扰,只要在热力学极限下k/L→0,其中L是线性系统大小。此外,我们识别了表征一些非冻结扇区的一形式U(1)电荷,并讨论了从典型初始条件开始的动力学,我们认为这最好根据涌现的一形式对称性的磁流体动力学来解释。

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