Casimir Self-Entropy of a Spherical Electromagnetic -Function Shell
arXiv:1707.09840 · doi:10.1103/PhysRevD.96.085007
Abstract
In this paper we continue our program of computing Casimir self-entropies of idealized electrical bodies. Here we consider an electromagnetic -function sphere ("semitransparent sphere") whose electric susceptibility has a transverse polarization with arbitrary strength. Dispersion is incorporated by a plasma-like model. In the strong coupling limit, a perfectly conducting spherical shell is realized. We compute the entropy for both low and high temperatures. The TE self-entropy is negative as expected, but the TM self-entropy requires ultraviolet and infrared subtractions, and, surprisingly, is only positive for sufficiently strong coupling. Results are robust under different regularization schemes.
25 pages, 3 figures
References in corpus (10)
- Thermal corrections to the Casimir effect
- Thermal Casimir effect in ideal metal rectangular boxes
- Lifshitz theory of atom-wall interaction with applications to quantum reflection
- On Horizonless Temperature with an Accelerating Mirror
- On the vacuum energy of a spherical plasma shell
- On the Casimir entropy for a ball in front of a plane
- Geometric origin of negative Casimir entropies: A scattering-channel analysis
- Negative Casimir Entropies in Nanoparticle Interactions
- Casimir Self-Entropy of an Electromagnetic Thin Sheet
- Presence of negative entropies in Casimir interactions