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Casimir self-entropy of nanoparticles with classical polarizabilities: Electromagnetic field fluctuations

Casimir self-entropy of nanoparticles with classical polarizabilities: Electromagnetic field fluctuations
Casimir self-entropy of nanoparticles with classical polarizabilities: Electromagnetic field fluctuations
Not only are Casimir interaction entropies not guaranteed to be positive, but also, more strikingly, Casimir self-entropies of bodies can be negative. Here, we attempt to interpret the physical origin and meaning of these negative self-entropies by investigating the Casimir self-entropy of a neutral spherical nanoparticle. After extracting the polarizabilities of such a particle by examining the asymptotic behavior of the scattering Green’s function, we compute the corresponding free energy and entropy. Two models for the nanoparticle, namely a spherical plasma δ-function shell and a homogeneous dielectric/diamagnetic ball, are considered at low temperature, because that is all that can be revealed from a nanoparticle perspective. The second model includes a contribution to the entropy from the bulk free energy, referring to the situation where the medium inside or outside the ball fills all space, which must be subtracted on physical grounds in order to maintain consistency with van der Waals interactions, corresponding to the self-entropy of each bulk. (The van der Waals calculation is described in Appendix A.) The entropies so calculated agree with known results in the low-temperature limit, appropriate for a small particle, and are negative. But we suggest that the negative self-entropy is simply an interaction entropy, the difference between the total entropy and the blackbody entropy of the two bulks, outside or inside of the nanosphere. The vacuum entropy is always positive and overwhelms the interaction entropy. Thus the interaction entropy can be negative, without contradicting the principles of statistical thermodynamics. Given the intrinsic electrical properties of the nanoparticle, the self-entropy arises from its interaction with the thermal vacuum permeating all space. Because the entropy of blackbody radiation by itself plays an important role, it is also discussed, including dispersive effects, in detail.
2470-0010
Li, Yang
4f067119-66c6-48c9-8da6-408037692d76
Milton, Kimball A.
32b2e838-92a4-4f2d-a33d-ab54ddaf8e08
Parashar, Prachi
d9529981-5e23-47b3-b76d-9354be4a1a91
Kennedy, Gerard
47b61664-2d2d-45fa-a73a-5af7a7c740cd
Pourtolami, Nima
b43c7cb9-06b9-4dde-ba1a-8936230f6d04
Guo, Xin
3f89f94f-15ae-4a6d-962a-4fbfdc099541
Li, Yang
4f067119-66c6-48c9-8da6-408037692d76
Milton, Kimball A.
32b2e838-92a4-4f2d-a33d-ab54ddaf8e08
Parashar, Prachi
d9529981-5e23-47b3-b76d-9354be4a1a91
Kennedy, Gerard
47b61664-2d2d-45fa-a73a-5af7a7c740cd
Pourtolami, Nima
b43c7cb9-06b9-4dde-ba1a-8936230f6d04
Guo, Xin
3f89f94f-15ae-4a6d-962a-4fbfdc099541

Li, Yang, Milton, Kimball A., Parashar, Prachi, Kennedy, Gerard, Pourtolami, Nima and Guo, Xin (2022) Casimir self-entropy of nanoparticles with classical polarizabilities: Electromagnetic field fluctuations. Physical Review D, 106 (3), [036002]. (doi:10.1103/PhysRevD.106.036002).

Record type: Article

Abstract

Not only are Casimir interaction entropies not guaranteed to be positive, but also, more strikingly, Casimir self-entropies of bodies can be negative. Here, we attempt to interpret the physical origin and meaning of these negative self-entropies by investigating the Casimir self-entropy of a neutral spherical nanoparticle. After extracting the polarizabilities of such a particle by examining the asymptotic behavior of the scattering Green’s function, we compute the corresponding free energy and entropy. Two models for the nanoparticle, namely a spherical plasma δ-function shell and a homogeneous dielectric/diamagnetic ball, are considered at low temperature, because that is all that can be revealed from a nanoparticle perspective. The second model includes a contribution to the entropy from the bulk free energy, referring to the situation where the medium inside or outside the ball fills all space, which must be subtracted on physical grounds in order to maintain consistency with van der Waals interactions, corresponding to the self-entropy of each bulk. (The van der Waals calculation is described in Appendix A.) The entropies so calculated agree with known results in the low-temperature limit, appropriate for a small particle, and are negative. But we suggest that the negative self-entropy is simply an interaction entropy, the difference between the total entropy and the blackbody entropy of the two bulks, outside or inside of the nanosphere. The vacuum entropy is always positive and overwhelms the interaction entropy. Thus the interaction entropy can be negative, without contradicting the principles of statistical thermodynamics. Given the intrinsic electrical properties of the nanoparticle, the self-entropy arises from its interaction with the thermal vacuum permeating all space. Because the entropy of blackbody radiation by itself plays an important role, it is also discussed, including dispersive effects, in detail.

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Accepted/In Press date: 11 July 2022
e-pub ahead of print date: 1 August 2022
Published date: 2 August 2022
Additional Information: Funding Information: The work of K. A. M. and X. G. was supported by a grant from the U.S. National Science Foundation, Grant No. 2008417. It is a pleasure to acknowledge the collaborative assistance of Stephen Fulling and Iver Brevik. This paper reflects solely the authors’ personal opinions and does not represent the opinions of the authors’ employers, present and past, in any way. Publisher Copyright: © 2022 authors. Published by the American Physical Society. Published by the American Physical Society under the terms of the "https://creativecommons.org/licenses/by/4.0/"Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Funded by SCOAP3.

Identifiers

Local EPrints ID: 468998
URI: http://eprints.soton.ac.uk/id/eprint/468998
ISSN: 2470-0010
PURE UUID: 9a168f84-340c-48df-b15f-fe70b98370e7
ORCID for Gerard Kennedy: ORCID iD orcid.org/0000-0003-4844-6231

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Date deposited: 05 Sep 2022 16:34
Last modified: 17 Mar 2024 02:59

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Contributors

Author: Yang Li
Author: Kimball A. Milton
Author: Prachi Parashar
Author: Gerard Kennedy ORCID iD
Author: Nima Pourtolami
Author: Xin Guo

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