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A Wigner Quasiprobability Distribution of Work

In this article, we introduce a quasiprobability distribution of work that is based on the Wigner function. This proposal rests on the idea that the work conducted on an isolated system can be coherently measured by coupling the system to a quantum measurement apparatus. In this way, a quasiprobabil...

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Detalles Bibliográficos
Autores principales: Cerisola, Federico, Mayo, Franco, Roncaglia, Augusto J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10606729/
https://www.ncbi.nlm.nih.gov/pubmed/37895560
http://dx.doi.org/10.3390/e25101439
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author Cerisola, Federico
Mayo, Franco
Roncaglia, Augusto J.
author_facet Cerisola, Federico
Mayo, Franco
Roncaglia, Augusto J.
author_sort Cerisola, Federico
collection PubMed
description In this article, we introduce a quasiprobability distribution of work that is based on the Wigner function. This proposal rests on the idea that the work conducted on an isolated system can be coherently measured by coupling the system to a quantum measurement apparatus. In this way, a quasiprobability distribution of work can be defined in terms of the Wigner function of the apparatus. This quasidistribution contains the information of the work statistics and also holds a clear operational definition that can be directly measured in a real experiment. Moreover, it is shown that the presence of quantum coherence in the energy eigenbasis is related with the appearance of features related to non-classicality in the Wigner function such as negativity and interference fringes. On the other hand, from this quasiprobability distribution, it is straightforward to obtain the standard two-point measurement probability distribution of work and also the difference in average energy for initial states with coherences.
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spelling pubmed-106067292023-10-28 A Wigner Quasiprobability Distribution of Work Cerisola, Federico Mayo, Franco Roncaglia, Augusto J. Entropy (Basel) Article In this article, we introduce a quasiprobability distribution of work that is based on the Wigner function. This proposal rests on the idea that the work conducted on an isolated system can be coherently measured by coupling the system to a quantum measurement apparatus. In this way, a quasiprobability distribution of work can be defined in terms of the Wigner function of the apparatus. This quasidistribution contains the information of the work statistics and also holds a clear operational definition that can be directly measured in a real experiment. Moreover, it is shown that the presence of quantum coherence in the energy eigenbasis is related with the appearance of features related to non-classicality in the Wigner function such as negativity and interference fringes. On the other hand, from this quasiprobability distribution, it is straightforward to obtain the standard two-point measurement probability distribution of work and also the difference in average energy for initial states with coherences. MDPI 2023-10-11 /pmc/articles/PMC10606729/ /pubmed/37895560 http://dx.doi.org/10.3390/e25101439 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Cerisola, Federico
Mayo, Franco
Roncaglia, Augusto J.
A Wigner Quasiprobability Distribution of Work
title A Wigner Quasiprobability Distribution of Work
title_full A Wigner Quasiprobability Distribution of Work
title_fullStr A Wigner Quasiprobability Distribution of Work
title_full_unstemmed A Wigner Quasiprobability Distribution of Work
title_short A Wigner Quasiprobability Distribution of Work
title_sort wigner quasiprobability distribution of work
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10606729/
https://www.ncbi.nlm.nih.gov/pubmed/37895560
http://dx.doi.org/10.3390/e25101439
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