Moore Joel E
Department of Physics, University of California, Berkeley, CA 94720, USA
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA.
Philos Trans A Math Phys Eng Sci. 2017 Dec 13;375(2108). doi: 10.1098/rsta.2016.0429.
Two of the most active areas in quantum many-particle dynamics involve systems with an unusually large number of conservation laws. Many-body-localized systems generalize ideas of Anderson localization by disorder to interacting systems. While localization still exists with interactions and inhibits thermalization, the interactions between conserved quantities lead to some dramatic differences from the Anderson case. Quantum integrable models such as the XXZ spin chain or Bose gas with delta-function interactions also have infinite sets of conservation laws, again leading to modifications of conventional thermalization. A practical way to treat the hydrodynamic evolution from local equilibrium to global equilibrium in such models is discussed. This paper expands upon a presentation at a discussion meeting of the Royal Society on 7 February 2017. The work described was carried out with a number of collaborators, including Jens Bardarson, Vir Bulchandani, Roni Ilan, Christoph Karrasch, Siddharth Parameswaran, Frank Pollmann and Romain Vasseur.This article is part of the themed issue 'Breakdown of ergodicity in quantum systems: from solids to synthetic matter'.
量子多粒子动力学中最活跃的两个领域涉及具有异常大量守恒定律的系统。多体局域化系统将由无序导致的安德森局域化概念推广到相互作用系统。虽然局域化在存在相互作用时仍然存在并抑制热化,但守恒量之间的相互作用导致了与安德森情形的一些显著差异。诸如具有δ函数相互作用的XXZ自旋链或玻色气体等量子可积模型也有无限组守恒定律,这同样导致了对传统热化的修正。本文讨论了在这类模型中处理从局部平衡到全局平衡的流体动力学演化的一种实用方法。本文是在2017年2月7日皇家学会的一次讨论会上的报告基础上扩展而成。所描述的工作是与包括延斯·巴尔达森、维尔·布尔钱达尼、罗尼·伊兰、克里斯托夫·卡拉斯克、西达尔特·帕拉梅斯瓦兰、弗兰克·波尔曼和罗曼·瓦瑟尔在内的多位合作者共同完成的。本文是主题为“量子系统中遍历性的崩溃:从固体到合成物质”的特刊的一部分。