Lower bounds for ballistic current and noise in non-equilibrium quantum steady states

Let an infinite, homogeneous, many-body quantum system be unitarily evolved for a long time from a state where two halves are independently thermalized. One says that a non-equilibrium steady state emerges if there are nonzero steady currents in the central region. In particular, their presence is a...

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Main Author: Benjamin Doyon
Format: Article
Language:English
Published: Elsevier 2015-03-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321315000103
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spelling doaj-0a0d3faf898e4054b9e503733ddd79882020-11-24T21:08:38ZengElsevierNuclear Physics B0550-32132015-03-01892190210Lower bounds for ballistic current and noise in non-equilibrium quantum steady statesBenjamin Doyon0Department of Mathematics, King's College London, Strand, London WC2R 2LS, UKLet an infinite, homogeneous, many-body quantum system be unitarily evolved for a long time from a state where two halves are independently thermalized. One says that a non-equilibrium steady state emerges if there are nonzero steady currents in the central region. In particular, their presence is a signature of ballistic transport. We analyze the consequences of the current observable being a conserved density; near equilibrium this is known to give rise to linear wave propagation and a nonzero Drude peak. Using the Lieb–Robinson bound, we derive, under a certain regularity condition, a lower bound for the non-equilibrium steady-state current determined by equilibrium averages. This shows and quantifies the presence of ballistic transport far from equilibrium. The inequality suggests the definition of “nonlinear sound velocities”, which specialize to the sound velocity near equilibrium in non-integrable models, and “generalized sound velocities”, which encode generalized Gibbs thermalization in integrable models. These are bounded by the Lieb–Robinson velocity. The inequality also gives rise to a bound on the energy current noise in the case of pure energy transport. We show that the inequality is satisfied in many models where exact results are available, and that it is saturated at one-dimensional criticality.http://www.sciencedirect.com/science/article/pii/S0550321315000103
collection DOAJ
language English
format Article
sources DOAJ
author Benjamin Doyon
spellingShingle Benjamin Doyon
Lower bounds for ballistic current and noise in non-equilibrium quantum steady states
Nuclear Physics B
author_facet Benjamin Doyon
author_sort Benjamin Doyon
title Lower bounds for ballistic current and noise in non-equilibrium quantum steady states
title_short Lower bounds for ballistic current and noise in non-equilibrium quantum steady states
title_full Lower bounds for ballistic current and noise in non-equilibrium quantum steady states
title_fullStr Lower bounds for ballistic current and noise in non-equilibrium quantum steady states
title_full_unstemmed Lower bounds for ballistic current and noise in non-equilibrium quantum steady states
title_sort lower bounds for ballistic current and noise in non-equilibrium quantum steady states
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2015-03-01
description Let an infinite, homogeneous, many-body quantum system be unitarily evolved for a long time from a state where two halves are independently thermalized. One says that a non-equilibrium steady state emerges if there are nonzero steady currents in the central region. In particular, their presence is a signature of ballistic transport. We analyze the consequences of the current observable being a conserved density; near equilibrium this is known to give rise to linear wave propagation and a nonzero Drude peak. Using the Lieb–Robinson bound, we derive, under a certain regularity condition, a lower bound for the non-equilibrium steady-state current determined by equilibrium averages. This shows and quantifies the presence of ballistic transport far from equilibrium. The inequality suggests the definition of “nonlinear sound velocities”, which specialize to the sound velocity near equilibrium in non-integrable models, and “generalized sound velocities”, which encode generalized Gibbs thermalization in integrable models. These are bounded by the Lieb–Robinson velocity. The inequality also gives rise to a bound on the energy current noise in the case of pure energy transport. We show that the inequality is satisfied in many models where exact results are available, and that it is saturated at one-dimensional criticality.
url http://www.sciencedirect.com/science/article/pii/S0550321315000103
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