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Non-hermitian quantum thermodynamics

Thermodynamics is the phenomenological theory of heat and work. Here we analyze to what extent quantum thermodynamic relations are immune to the underlying mathematical formulation of quantum mechanics. As a main result, we show that the Jarzynski equality holds true for all non-hermitian quantum sy...

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Autores principales: Gardas, Bartłomiej, Deffner, Sebastian, Saxena, Avadh
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4802220/
https://www.ncbi.nlm.nih.gov/pubmed/27003686
http://dx.doi.org/10.1038/srep23408
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author Gardas, Bartłomiej
Deffner, Sebastian
Saxena, Avadh
author_facet Gardas, Bartłomiej
Deffner, Sebastian
Saxena, Avadh
author_sort Gardas, Bartłomiej
collection PubMed
description Thermodynamics is the phenomenological theory of heat and work. Here we analyze to what extent quantum thermodynamic relations are immune to the underlying mathematical formulation of quantum mechanics. As a main result, we show that the Jarzynski equality holds true for all non-hermitian quantum systems with real spectrum. This equality expresses the second law of thermodynamics for isothermal processes arbitrarily far from equilibrium. In the quasistatic limit however, the second law leads to the Carnot bound which is fulfilled even if some eigenenergies are complex provided they appear in conjugate pairs. Furthermore, we propose two setups to test our predictions, namely with strongly interacting excitons and photons in a semiconductor microcavity and in the non-hermitian tight-binding model.
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spelling pubmed-48022202016-03-23 Non-hermitian quantum thermodynamics Gardas, Bartłomiej Deffner, Sebastian Saxena, Avadh Sci Rep Article Thermodynamics is the phenomenological theory of heat and work. Here we analyze to what extent quantum thermodynamic relations are immune to the underlying mathematical formulation of quantum mechanics. As a main result, we show that the Jarzynski equality holds true for all non-hermitian quantum systems with real spectrum. This equality expresses the second law of thermodynamics for isothermal processes arbitrarily far from equilibrium. In the quasistatic limit however, the second law leads to the Carnot bound which is fulfilled even if some eigenenergies are complex provided they appear in conjugate pairs. Furthermore, we propose two setups to test our predictions, namely with strongly interacting excitons and photons in a semiconductor microcavity and in the non-hermitian tight-binding model. Nature Publishing Group 2016-03-22 /pmc/articles/PMC4802220/ /pubmed/27003686 http://dx.doi.org/10.1038/srep23408 Text en Copyright © 2016, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Gardas, Bartłomiej
Deffner, Sebastian
Saxena, Avadh
Non-hermitian quantum thermodynamics
title Non-hermitian quantum thermodynamics
title_full Non-hermitian quantum thermodynamics
title_fullStr Non-hermitian quantum thermodynamics
title_full_unstemmed Non-hermitian quantum thermodynamics
title_short Non-hermitian quantum thermodynamics
title_sort non-hermitian quantum thermodynamics
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4802220/
https://www.ncbi.nlm.nih.gov/pubmed/27003686
http://dx.doi.org/10.1038/srep23408
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