Casimir Energies for Isorefractive or Diaphanous Balls
It is known that the Casimir self-energy of a homogeneous dielectric ball is divergent, although a finite self-energy can be extracted through second order in the deviation of the permittivity from the vacuum value. The exception occurs when the speed of light inside the spherical boundary is the sa...
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doaj-100423dde165428f9f584fb17d5acd952020-11-24T23:29:17ZengMDPI AGSymmetry2073-89942018-03-011036810.3390/sym10030068sym10030068Casimir Energies for Isorefractive or Diaphanous BallsKimball A. Milton0Iver Brevik1Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK 73019, USADepartment of Energy and Process Engineering, Norwegian University of Science and Technology, NO-7491 Trondheim, NorwayIt is known that the Casimir self-energy of a homogeneous dielectric ball is divergent, although a finite self-energy can be extracted through second order in the deviation of the permittivity from the vacuum value. The exception occurs when the speed of light inside the spherical boundary is the same as that outside, so the self-energy of a perfectly conducting spherical shell is finite, as is the energy of a dielectric-diamagnetic sphere with ε μ = 1 , a so-called isorefractive or diaphanous ball. Here we re-examine that example and attempt to extend it to an electromagnetic δ -function sphere, where the electric and magnetic couplings are equal and opposite. Unfortunately, although the energy expression is superficially ultraviolet finite, additional divergences appear that render it difficult to extract a meaningful result in general, but some limited results are presented.http://www.mdpi.com/2073-8994/10/3/68Casimir effectdispersionultraviolet divergencesinfrared divergences |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Kimball A. Milton Iver Brevik |
spellingShingle |
Kimball A. Milton Iver Brevik Casimir Energies for Isorefractive or Diaphanous Balls Symmetry Casimir effect dispersion ultraviolet divergences infrared divergences |
author_facet |
Kimball A. Milton Iver Brevik |
author_sort |
Kimball A. Milton |
title |
Casimir Energies for Isorefractive or Diaphanous Balls |
title_short |
Casimir Energies for Isorefractive or Diaphanous Balls |
title_full |
Casimir Energies for Isorefractive or Diaphanous Balls |
title_fullStr |
Casimir Energies for Isorefractive or Diaphanous Balls |
title_full_unstemmed |
Casimir Energies for Isorefractive or Diaphanous Balls |
title_sort |
casimir energies for isorefractive or diaphanous balls |
publisher |
MDPI AG |
series |
Symmetry |
issn |
2073-8994 |
publishDate |
2018-03-01 |
description |
It is known that the Casimir self-energy of a homogeneous dielectric ball is divergent, although a finite self-energy can be extracted through second order in the deviation of the permittivity from the vacuum value. The exception occurs when the speed of light inside the spherical boundary is the same as that outside, so the self-energy of a perfectly conducting spherical shell is finite, as is the energy of a dielectric-diamagnetic sphere with ε μ = 1 , a so-called isorefractive or diaphanous ball. Here we re-examine that example and attempt to extend it to an electromagnetic δ -function sphere, where the electric and magnetic couplings are equal and opposite. Unfortunately, although the energy expression is superficially ultraviolet finite, additional divergences appear that render it difficult to extract a meaningful result in general, but some limited results are presented. |
topic |
Casimir effect dispersion ultraviolet divergences infrared divergences |
url |
http://www.mdpi.com/2073-8994/10/3/68 |
work_keys_str_mv |
AT kimballamilton casimirenergiesforisorefractiveordiaphanousballs AT iverbrevik casimirenergiesforisorefractiveordiaphanousballs |
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1725546459163525120 |