Crossref journal-article
The Royal Society
Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences (175)
Abstract

The long-range dispersion forces in a non-uniform dielectric at finite temperature are deduced from the frequency-dependent susceptibility of the electric field and the dielectric constant at imaginary frequency by a method which gives the main results of Lifshitz’s treatment and does not use quantum field theory. The fluctuation-dissipation theorem allows one to express the dispersion free energy of an atom in terms of its electric polarizability, and to derive the image force on an atom near a metal surface, or the dispersion force between two atoms in vacuo at any temperature. By considering the relation between the force on an atom outside a dielectric and the state of the field inside the dielectric we derive an expression for the long-range dispersion part of the free energy of the medium , and find the force between two dissolved atom s in a dielectric fluid. The forces are equivalent to a system of Maxwell stresses which can be calculated from the field susceptibilities. A simple classical treatment of the susceptibility then gives the Lifshitz force between two parallel plates of dielectric at close distances.

Bibliography

Retarded dispersion forces in dielectrics at finite temperatures. (1963). Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 274(1356), 80–90.

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Dates
Type When
Created 18 years, 8 months ago (Dec. 18, 2006, 5:24 p.m.)
Deposited 4 years, 6 months ago (Feb. 20, 2021, 7:16 p.m.)
Indexed 3 days, 15 hours ago (Aug. 21, 2025, 12:36 p.m.)
Issued 62 years, 2 months ago (June 25, 1963)
Published 62 years, 2 months ago (June 25, 1963)
Published Online 28 years, 7 months ago (Jan. 1, 1997)
Published Print 62 years, 2 months ago (June 25, 1963)
Funders 0

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@article{1963, volume={274}, ISSN={2053-9169}, url={http://dx.doi.org/10.1098/rspa.1963.0115}, DOI={10.1098/rspa.1963.0115}, number={1356}, journal={Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences}, publisher={The Royal Society}, year={1963}, month=jun, pages={80–90} }