Thermodynamics of the Ramsey Zone

We studied the thermodynamic properties such as the entropy, heat (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>Q</mi></msub></semantics></math>&l...

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Main Authors: Rogério Jorge de Assis, Ciro Micheletti Diniz, Norton Gomes de Almeida, Celso Jorge Villas-Bôas
Format: Article
Language:English
Published: MDPI AG 2023-10-01
Series:Entropy
Subjects:
Online Access:https://www.mdpi.com/1099-4300/25/10/1430
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author Rogério Jorge de Assis
Ciro Micheletti Diniz
Norton Gomes de Almeida
Celso Jorge Villas-Bôas
author_facet Rogério Jorge de Assis
Ciro Micheletti Diniz
Norton Gomes de Almeida
Celso Jorge Villas-Bôas
author_sort Rogério Jorge de Assis
collection DOAJ
description We studied the thermodynamic properties such as the entropy, heat (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>Q</mi></msub></semantics></math></inline-formula>), and work (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>W</mi></msub></semantics></math></inline-formula>) rates involved when an atom passes through a Ramsey zone, which consists of a mode field inside a low-quality factor cavity that behaves classically, promoting rotations on the atomic state. Focusing on the atom, we show that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>W</mi></msub></semantics></math></inline-formula> predominates when the atomic rotations are successful, maintaining its maximum purity as computed by the von Neumann entropy. Conversely, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>Q</mi></msub></semantics></math></inline-formula> stands out when the atomic state ceases to be pure due to its entanglement with the cavity mode. With this, we interpret the quantum-to-classical transition in light of the heat and work rates. Besides, we show that, for the cavity mode to work as a Ramsey zone (classical field), several photons (of the order of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mn>10</mn><mn>6</mn></msup></semantics></math></inline-formula>) need to cross the cavity, which explains its classical behavior, even when the inside average number of photons is of the order of unity.
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spelling doaj.art-d0b71051d4ca4dea8cadd5684304ac742023-11-19T16:24:47ZengMDPI AGEntropy1099-43002023-10-012510143010.3390/e25101430Thermodynamics of the Ramsey ZoneRogério Jorge de Assis0Ciro Micheletti Diniz1Norton Gomes de Almeida2Celso Jorge Villas-Bôas3Instituto de Física, Universidade Federal de Goiás, Goiânia 74690-900, GO, BrazilDepartamento de Física, Universidade Federal de São Carlos, São Carlos 13565-905, SP, BrazilInstituto de Física, Universidade Federal de Goiás, Goiânia 74690-900, GO, BrazilDepartamento de Física, Universidade Federal de São Carlos, São Carlos 13565-905, SP, BrazilWe studied the thermodynamic properties such as the entropy, heat (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>Q</mi></msub></semantics></math></inline-formula>), and work (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>W</mi></msub></semantics></math></inline-formula>) rates involved when an atom passes through a Ramsey zone, which consists of a mode field inside a low-quality factor cavity that behaves classically, promoting rotations on the atomic state. Focusing on the atom, we show that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>W</mi></msub></semantics></math></inline-formula> predominates when the atomic rotations are successful, maintaining its maximum purity as computed by the von Neumann entropy. Conversely, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>J</mi><mi>Q</mi></msub></semantics></math></inline-formula> stands out when the atomic state ceases to be pure due to its entanglement with the cavity mode. With this, we interpret the quantum-to-classical transition in light of the heat and work rates. Besides, we show that, for the cavity mode to work as a Ramsey zone (classical field), several photons (of the order of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mn>10</mn><mn>6</mn></msup></semantics></math></inline-formula>) need to cross the cavity, which explains its classical behavior, even when the inside average number of photons is of the order of unity.https://www.mdpi.com/1099-4300/25/10/1430quantum thermodynamicscavity quantum electrodynamicsRamsey zone
spellingShingle Rogério Jorge de Assis
Ciro Micheletti Diniz
Norton Gomes de Almeida
Celso Jorge Villas-Bôas
Thermodynamics of the Ramsey Zone
Entropy
quantum thermodynamics
cavity quantum electrodynamics
Ramsey zone
title Thermodynamics of the Ramsey Zone
title_full Thermodynamics of the Ramsey Zone
title_fullStr Thermodynamics of the Ramsey Zone
title_full_unstemmed Thermodynamics of the Ramsey Zone
title_short Thermodynamics of the Ramsey Zone
title_sort thermodynamics of the ramsey zone
topic quantum thermodynamics
cavity quantum electrodynamics
Ramsey zone
url https://www.mdpi.com/1099-4300/25/10/1430
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AT ciromichelettidiniz thermodynamicsoftheramseyzone
AT nortongomesdealmeida thermodynamicsoftheramseyzone
AT celsojorgevillasboas thermodynamicsoftheramseyzone