Nonequilibrium density matrix for quantum transport: Hershfield approach as a McLennan-Zubarev form of the statistical operator

H. Ness
Phys. Rev. E 88, 022121 – Published 13 August 2013

Abstract

In this paper, we formally demonstrate that the nonequilibrium density matrix developed by Hershfield for the steady state has the form of a McLennan-Zubarev nonequilibrium ensemble. The correction term in this pseudoequilibrium Gibbs-like ensemble is directly related to the entropy production in the quantum open system. The fact that both methods state that a nonequilibrium steady state can be mapped onto a pseudoequilibrium, permits us to develop nonequilibrium quantities from formal expressions equivalent to the equilibrium case. We provide an example: the derivation of a nonequilibrium distribution function for the electron population in a scattering region in the context of quantum transport.

  • Received 18 March 2013

DOI:https://doi.org/10.1103/PhysRevE.88.022121

©2013 American Physical Society

Authors & Affiliations

H. Ness*

  • Department of Physics, University of York, Heslington, York YO10 5DD, United Kingdom

  • *Also at European Theoretical Spectroscopy Facility (ETSF), www.etsf.eu; herve.ness@york.ac.uk

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Issue

Vol. 88, Iss. 2 — August 2013

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