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Fundamental Limitation on Cooling under Classical Noise

We prove a general theorem that the action of arbitrary classical noise or random unitary channels can not increase the maximum population of any eigenstate of an open quantum system, assuming initial system-environment factorization. Such factorization is the conventional starting point for descrip...

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Autores principales: Jing, Jun, Chhajlany, Ravindra W., Wu, Lian-Ao
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5427912/
https://www.ncbi.nlm.nih.gov/pubmed/28282969
http://dx.doi.org/10.1038/s41598-017-00194-9
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author Jing, Jun
Chhajlany, Ravindra W.
Wu, Lian-Ao
author_facet Jing, Jun
Chhajlany, Ravindra W.
Wu, Lian-Ao
author_sort Jing, Jun
collection PubMed
description We prove a general theorem that the action of arbitrary classical noise or random unitary channels can not increase the maximum population of any eigenstate of an open quantum system, assuming initial system-environment factorization. Such factorization is the conventional starting point for descriptions of open system dynamics. In particular, our theorem implies that a system can not be ideally cooled down unless it is initially prepared as a pure state. The resultant inequality rigorously constrains the possibility of cooling the system solely through temporal manipulation, i.e., dynamical control over the system Hamiltonian without resorting to measurement based cooling methods. It is a substantial generalization of the no-go theorem claiming that the exact ground state cooling is forbidden given initial system-thermal bath factorization, while here we prove even cooling is impossible under classical noise.
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spelling pubmed-54279122017-05-12 Fundamental Limitation on Cooling under Classical Noise Jing, Jun Chhajlany, Ravindra W. Wu, Lian-Ao Sci Rep Article We prove a general theorem that the action of arbitrary classical noise or random unitary channels can not increase the maximum population of any eigenstate of an open quantum system, assuming initial system-environment factorization. Such factorization is the conventional starting point for descriptions of open system dynamics. In particular, our theorem implies that a system can not be ideally cooled down unless it is initially prepared as a pure state. The resultant inequality rigorously constrains the possibility of cooling the system solely through temporal manipulation, i.e., dynamical control over the system Hamiltonian without resorting to measurement based cooling methods. It is a substantial generalization of the no-go theorem claiming that the exact ground state cooling is forbidden given initial system-thermal bath factorization, while here we prove even cooling is impossible under classical noise. Nature Publishing Group UK 2017-03-14 /pmc/articles/PMC5427912/ /pubmed/28282969 http://dx.doi.org/10.1038/s41598-017-00194-9 Text en © The Author(s) 2017 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
Jing, Jun
Chhajlany, Ravindra W.
Wu, Lian-Ao
Fundamental Limitation on Cooling under Classical Noise
title Fundamental Limitation on Cooling under Classical Noise
title_full Fundamental Limitation on Cooling under Classical Noise
title_fullStr Fundamental Limitation on Cooling under Classical Noise
title_full_unstemmed Fundamental Limitation on Cooling under Classical Noise
title_short Fundamental Limitation on Cooling under Classical Noise
title_sort fundamental limitation on cooling under classical noise
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5427912/
https://www.ncbi.nlm.nih.gov/pubmed/28282969
http://dx.doi.org/10.1038/s41598-017-00194-9
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