Retarded potentials in disspersive media
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A very nice description of classical dispersion theory can be found in
A. Sommerfeld, Lectures on Theoretical Physics IV (Optics)
A. Sommerfeld, Lectures on Theoretical Physics IV (Optics)
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The classical dispersion theory gives you the (complex-valued) dielectric function [itex]\epsilon(\omega)[/itex] from a simple damped harmonic oscillator ansatz for the electrons in the medium interacting with the incoming em. wave.
Quantum-field theoretically you find very similar results as the retarded in-medium Green's function of the em. field. Quantum mechanical dispersion theory on this linear-response level is not so different from the classical theory.
Quantum-field theoretically you find very similar results as the retarded in-medium Green's function of the em. field. Quantum mechanical dispersion theory on this linear-response level is not so different from the classical theory.
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hunt_mat said:Interesting. I am not that interested in complex mediums, just a simple multiplicative description.
You can't avoid it though. A dispersive media always implies a lossy media by virtue of the Kramers-Kronig relation. As vanhees states though, the simplest model for a dispersive media is a simple oscillator as modeled by the Debye relaxation (or its variants like the Cole-Cole, Cole-Davidson, etc.). I would use Debye relaxation as a basic start for modeling dielectric dispersion. As simple as it is, it's very useful in application as long as you realize that it is meant to be applied over a finite bandwidth.
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