arXiv Analytics

Sign in

arXiv:1811.03114 [cond-mat.stat-mech]AbstractReferencesReviewsResources

An Extension of ETH to Non-Equilibrium Steady States

Sanjay Moudgalya, Trithep Devakul, D. P. Arovas, S. L. Sondhi

Published 2018-11-07Version 1

We extend the notion of the Eigenstate Thermalization Hypothesis (ETH) to Open Quantum Systems governed by the Gorini-Kossakowski-Lindblad-Sudarshan (GKLS) Master Equation. We present evidence that the eigenstates of non-equilibrium steady state (NESS) density matrices obey a generalization of ETH in boundary-driven systems when the bulk Hamiltonian is non-integrable, just as eigenstates of Gibbs density matrices do in equilibrium. This generalized ETH, which we call NESS-ETH, can be used to obtain representative pure states that reproduce the expectation values of few-body operators in the NESS. The density matrices of these representative pure states can be further interpreted as weak solutions of the GKLS Master Equation. Additionally, we explore the validity and breakdown of NESS-ETH in the presence of symmetries, integrability and many-body localization in the bulk Hamiltonian.

Related articles: Most relevant | Search more
Eigenstate thermalization hypothesis and integrals of motion
Eigenstate thermalization hypothesis through the lens of autocorrelation functions
arXiv:2110.04085 [cond-mat.stat-mech] (Published 2021-10-08, updated 2022-05-09)
Eigenstate thermalization hypothesis and its deviations from random-matrix theory beyond the thermalization time