Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations

We consider non-equilibrium open statistical systems, subject to potentials and to external “heat baths” (hb) at thermal equilibrium at temperature T (either with ab initio dissipation or without it). Boltzmann’s classical equilibrium distributions generate, as Gaussian weight functions in momenta,...

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Main Author: Ramon F. Alvarez-Estrada
Format: Article
Language:English
Published: MDPI AG 2012-02-01
Series:Entropy
Subjects:
Online Access:http://www.mdpi.com/1099-4300/14/2/291/
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spelling doaj-7e11de82d224479a90ec79c0fa892ee42020-11-25T00:51:52ZengMDPI AGEntropy1099-43002012-02-0114229132210.3390/e14020291Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time ApproximationsRamon F. Alvarez-EstradaWe consider non-equilibrium open statistical systems, subject to potentials and to external “heat baths” (hb) at thermal equilibrium at temperature T (either with ab initio dissipation or without it). Boltzmann’s classical equilibrium distributions generate, as Gaussian weight functions in momenta, orthogonal polynomials in momenta (the position-independent Hermite polynomialsHn’s). The moments of non-equilibrium classical distributions, implied by the Hn’s, fulfill a hierarchy: for long times, the lowest moment dominates the evolution towards thermal equilibrium, either with dissipation or without it (but under certain approximation). We revisit that hierarchy, whose solution depends on operator continued fractions. We review our generalization of that moment method to classical closed many-particle interacting systems with neither a hb nor ab initio dissipation: with initial states describing thermal equilibrium at T at large distances but non-equilibrium at finite distances, the moment method yields, approximately, irreversible thermalization of the whole system at T, for long times. Generalizations to non-equilibrium quantum interacting systems meet additional difficulties. Three of them are: (i) equilibrium distributions (represented through Wigner functions) are neither Gaussian in momenta nor known in closed form; (ii) they may depend on dissipation; and (iii) the orthogonal polynomials in momenta generated by them depend also on positions. We generalize the moment method, dealing with (i), (ii) and (iii), to some non-equilibrium one-particle quantum interacting systems. Open problems are discussed briefly.http://www.mdpi.com/1099-4300/14/2/291/classical and quantum distributionsequilibrium solutions and orthogonal polynomialsnon-equilibrium momentslong-time approximationsapproximate irreversibility
collection DOAJ
language English
format Article
sources DOAJ
author Ramon F. Alvarez-Estrada
spellingShingle Ramon F. Alvarez-Estrada
Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations
Entropy
classical and quantum distributions
equilibrium solutions and orthogonal polynomials
non-equilibrium moments
long-time approximations
approximate irreversibility
author_facet Ramon F. Alvarez-Estrada
author_sort Ramon F. Alvarez-Estrada
title Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations
title_short Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations
title_full Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations
title_fullStr Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations
title_full_unstemmed Classical and Quantum Models in Non-Equilibrium Statistical Mechanics: Moment Methods and Long-Time Approximations
title_sort classical and quantum models in non-equilibrium statistical mechanics: moment methods and long-time approximations
publisher MDPI AG
series Entropy
issn 1099-4300
publishDate 2012-02-01
description We consider non-equilibrium open statistical systems, subject to potentials and to external “heat baths” (hb) at thermal equilibrium at temperature T (either with ab initio dissipation or without it). Boltzmann’s classical equilibrium distributions generate, as Gaussian weight functions in momenta, orthogonal polynomials in momenta (the position-independent Hermite polynomialsHn’s). The moments of non-equilibrium classical distributions, implied by the Hn’s, fulfill a hierarchy: for long times, the lowest moment dominates the evolution towards thermal equilibrium, either with dissipation or without it (but under certain approximation). We revisit that hierarchy, whose solution depends on operator continued fractions. We review our generalization of that moment method to classical closed many-particle interacting systems with neither a hb nor ab initio dissipation: with initial states describing thermal equilibrium at T at large distances but non-equilibrium at finite distances, the moment method yields, approximately, irreversible thermalization of the whole system at T, for long times. Generalizations to non-equilibrium quantum interacting systems meet additional difficulties. Three of them are: (i) equilibrium distributions (represented through Wigner functions) are neither Gaussian in momenta nor known in closed form; (ii) they may depend on dissipation; and (iii) the orthogonal polynomials in momenta generated by them depend also on positions. We generalize the moment method, dealing with (i), (ii) and (iii), to some non-equilibrium one-particle quantum interacting systems. Open problems are discussed briefly.
topic classical and quantum distributions
equilibrium solutions and orthogonal polynomials
non-equilibrium moments
long-time approximations
approximate irreversibility
url http://www.mdpi.com/1099-4300/14/2/291/
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