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.
References
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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) |
@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} }