The density matrix in the non-Hermitian approach to open quantum system dynamics

In this paper we review an approach to the dynamics of open quantum systems based of non-Hermitian Hamiltonians. Non-Hermitian Hamiltonians arise naturally when one wish to study a subsystem interacting with a continuum of states. Moreover, quantum subsystems with probability sinks or sources are na...

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Main Author: Alessandro Sergi
Format: Article
Language:English
Published: Accademia Peloritana dei Pericolanti 2019-12-01
Series:Atti della Accademia Peloritana dei Pericolanti : Classe di Scienze Fisiche, Matematiche e Naturali
Online Access: http://dx.doi.org/10.1478/AAPP.97S2A11
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spelling doaj-1b50990b1eef4a699b80cc6b20efbce12020-11-25T01:34:55ZengAccademia Peloritana dei PericolantiAtti della Accademia Peloritana dei Pericolanti : Classe di Scienze Fisiche, Matematiche e Naturali0365-03591825-12422019-12-0197S2A1110.1478/AAPP.97S2A11AAPP.97S2A11The density matrix in the non-Hermitian approach to open quantum system dynamicsAlessandro SergiIn this paper we review an approach to the dynamics of open quantum systems based of non-Hermitian Hamiltonians. Non-Hermitian Hamiltonians arise naturally when one wish to study a subsystem interacting with a continuum of states. Moreover, quantum subsystems with probability sinks or sources are naturally described by non-Hermitian Hamiltonians. Herein, we discuss a non-Hermitian formalism based on the density matrix. We show both how to derive the equations of motion of the density matrix and how to define statistical averages properly. It turns out that the laws of evolution of the normalized density matrix are intrinsically non-linear. We also show how to define correlation functions and a non-Hermitian entropy with a non zero production rate. The formalism has been generalized to the case of hybrid quantum-classical systems using a partial Wigner representation. The equations of motion and the statistical averages are defined analogously to the pure quantum case. However, the definition of the entropy requires to introduce a non-Hermitian linear entropy functional. http://dx.doi.org/10.1478/AAPP.97S2A11
collection DOAJ
language English
format Article
sources DOAJ
author Alessandro Sergi
spellingShingle Alessandro Sergi
The density matrix in the non-Hermitian approach to open quantum system dynamics
Atti della Accademia Peloritana dei Pericolanti : Classe di Scienze Fisiche, Matematiche e Naturali
author_facet Alessandro Sergi
author_sort Alessandro Sergi
title The density matrix in the non-Hermitian approach to open quantum system dynamics
title_short The density matrix in the non-Hermitian approach to open quantum system dynamics
title_full The density matrix in the non-Hermitian approach to open quantum system dynamics
title_fullStr The density matrix in the non-Hermitian approach to open quantum system dynamics
title_full_unstemmed The density matrix in the non-Hermitian approach to open quantum system dynamics
title_sort density matrix in the non-hermitian approach to open quantum system dynamics
publisher Accademia Peloritana dei Pericolanti
series Atti della Accademia Peloritana dei Pericolanti : Classe di Scienze Fisiche, Matematiche e Naturali
issn 0365-0359
1825-1242
publishDate 2019-12-01
description In this paper we review an approach to the dynamics of open quantum systems based of non-Hermitian Hamiltonians. Non-Hermitian Hamiltonians arise naturally when one wish to study a subsystem interacting with a continuum of states. Moreover, quantum subsystems with probability sinks or sources are naturally described by non-Hermitian Hamiltonians. Herein, we discuss a non-Hermitian formalism based on the density matrix. We show both how to derive the equations of motion of the density matrix and how to define statistical averages properly. It turns out that the laws of evolution of the normalized density matrix are intrinsically non-linear. We also show how to define correlation functions and a non-Hermitian entropy with a non zero production rate. The formalism has been generalized to the case of hybrid quantum-classical systems using a partial Wigner representation. The equations of motion and the statistical averages are defined analogously to the pure quantum case. However, the definition of the entropy requires to introduce a non-Hermitian linear entropy functional.
url http://dx.doi.org/10.1478/AAPP.97S2A11
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