PreprintCC BY 4.0arXiv
Temperature dependence of the Casimir force between plane-layered structures: an approach based on the principle of argument
Abstract
Based on the complex analysis theorem the principle of argument, a temperature-dependent formula for the Casimir-Lifshitz dispersion force of the interaction of two arbitrary plane-layered structures separated by either a vacuum gap of size d or a layer of size d consisting of an arbitrary dissipative dielectric with dispersion is derived. The formula consists of the temperature-dependent Lifshitz formula plus the temperature-dependent contour integral
Related
- Temperature dependence of the Casimir pressure on two graphene sheets placed on a substrate
- Higher-order generalized uncertainty principle corrections to Casimir-supported traversable wormholes
- Quantum corrections to the Casimir effect in a scalar Hořava-Lifshitz theory with rough plates at low temperature
- Zero- and Finite-Temperature Casimir Effect in a Fracton Gauge Field
- DUNE Beam-Energy Dependence of Sensitivity to the Violation of the Equivalence Principle
BibTeX
@misc{davidovich2026temperature,
title = {{Temperature dependence of the Casimir force between plane-layered structures: an approach based on the principle of argument}},
author = {Michael V. Davidovich},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.23354},
eprint = {2610.23354},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.23354},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Temperature dependence of the Casimir force between plane-layered structures: an approach based on the principle of argument
AU - Michael V. Davidovich
PY - 2026
DA - 2026/10/16
PB - arXiv
DO - 10.48550/arxiv.2610.23354
UR - https://arxiv.org/abs/2610.23354
AB - Based on the complex analysis theorem the principle of argument, a temperature-dependent formula for the Casimir-Lifshitz dispersion force of the interaction of two arbitrary plane-layered structures separated by either a vacuum gap of size d or a layer of size d consisting of an arbitrary dissipative dielectric with dispersion is derived. The formula consists of the temperature-dependent Lifshitz formula plus the temperature-dependent contour integral
ER -