Axial Casimir force

Quantum fluctuations in vacuum can exert a dissipative force on moving objects, which is known as Casimir friction. Especially, a rotating particle in the vacuum will eventually slow down due to the dissipative Casimir friction. Here, we identify a dissipationless force by examining a rotating parti...

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Main Authors: Jiang, Qing-Dong, Wilczek, Frank
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics
Format: Article
Language:English
Published: American Physical Society 2020
Online Access:https://hdl.handle.net/1721.1/125067
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author Jiang, Qing-Dong
Wilczek, Frank
author2 Massachusetts Institute of Technology. Center for Theoretical Physics
author_facet Massachusetts Institute of Technology. Center for Theoretical Physics
Jiang, Qing-Dong
Wilczek, Frank
author_sort Jiang, Qing-Dong
collection MIT
description Quantum fluctuations in vacuum can exert a dissipative force on moving objects, which is known as Casimir friction. Especially, a rotating particle in the vacuum will eventually slow down due to the dissipative Casimir friction. Here, we identify a dissipationless force by examining a rotating particle near a bi-isotropic media that generally breaks parity symmetry or/and time-reversal symmetry. The direction of the dissipationless vacuum force is always parallel with the rotating axis of the particle. We therefore call this dissipationless vacuum force the axial Casimir force.
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spelling mit-1721.1/1250672022-09-27T16:00:06Z Axial Casimir force Jiang, Qing-Dong Wilczek, Frank Massachusetts Institute of Technology. Center for Theoretical Physics Massachusetts Institute of Technology. Department of Physics Quantum fluctuations in vacuum can exert a dissipative force on moving objects, which is known as Casimir friction. Especially, a rotating particle in the vacuum will eventually slow down due to the dissipative Casimir friction. Here, we identify a dissipationless force by examining a rotating particle near a bi-isotropic media that generally breaks parity symmetry or/and time-reversal symmetry. The direction of the dissipationless vacuum force is always parallel with the rotating axis of the particle. We therefore call this dissipationless vacuum force the axial Casimir force. Swedish Research Council (Contract 335-2014-7424) United States. Department of Energy (Grant DE-SC0012567) European Research Council (Grant 742104) 2020-05-06T18:31:02Z 2020-05-06T18:31:02Z 2019-04 2019-03 2019-04-01T18:00:28Z Article http://purl.org/eprint/type/JournalArticle 2469-9950 2469-9969 https://hdl.handle.net/1721.1/125067 Jiang, Qing-Dong, and Frank Wilczek. “Axial Casimir Force.” Physical Review B 99, 16 (April 2019): 165402. © 2019 American Physical Society en http://dx.doi.org/10.1103/PhysRevB.99.165402 Physical Review B Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. American Physical Society application/pdf American Physical Society American Physical Society
spellingShingle Jiang, Qing-Dong
Wilczek, Frank
Axial Casimir force
title Axial Casimir force
title_full Axial Casimir force
title_fullStr Axial Casimir force
title_full_unstemmed Axial Casimir force
title_short Axial Casimir force
title_sort axial casimir force
url https://hdl.handle.net/1721.1/125067
work_keys_str_mv AT jiangqingdong axialcasimirforce
AT wilczekfrank axialcasimirforce