Can Dispersive Media Be Modeled Effectively as Fields?

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SUMMARY

This discussion focuses on modeling dispersive media as fields, specifically examining the phase and group velocity in both dispersive and non-dispersive media. It highlights that traditional modeling relies on constitutive relationships between fields such as E and D, B and H, and stress and strain. The discussion emphasizes the potential of deriving these relationships from microscopic dynamics using methods ranging from classical transport models to quantum field theory, particularly through the Kadanoff-Baym equations. The use of linear-response approximation and Green-Kubo relations is also noted as a standard approach for deriving permittivity, permeability, and electric conductivity.

PREREQUISITES
  • Understanding of phase and group velocity in wave propagation
  • Familiarity with constitutive relationships in electromagnetism
  • Knowledge of quantum field theory and its applications in condensed matter physics
  • Proficiency in linear-response theory and Green-Kubo relations
NEXT STEPS
  • Explore the Kadanoff-Baym equations in quantum field theory
  • Study classical transport models for dispersive media
  • Research linear-response approximation techniques in electromagnetism
  • Investigate the derivation of permittivity and permeability using Green-Kubo relations
USEFUL FOR

Researchers and students in physics, particularly those focused on wave propagation, electromagnetism, and quantum field theory applications in condensed matter physics.

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I am studying phase and group velocity in non-dispersive and dispersive media. My question is the following: Is there any reason why a dispersive medium simply cannot be modeled as a type of field?
 
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redtree said:
I am studying phase and group velocity in non-dispersive and dispersive media. My question is the following: Is there any reason why a dispersive medium simply cannot be modeled as a type of field?

Typically, a medium is modeled in terms of a constitutive relationship between two fields (E and D, B and H, stress and strain, etc.) rather that a field itself. The downside is that there is a fundamentally phenomenological aspect to constitutive relationships, but the upside is that the modeling framework can be very general.
 
Well, a bit more ambitious is to calculate the constitutive relationships from the underlying microscopic dynamics of the matter interacting with the em. field. The methods reach from classical transport models to the full quantum theortical treatment. One flavor of the latter case is the use of the Kadanoff-Baym equations which entirely are based on quantum field theory (not necessarily relativistic; in condensed-matter physics you use non-relativistic QFT for that purpose) to derive them.

In the usual textbook case you use matter close to thermal equibrium to derive the permittivity, permeability, and electric conductivity in "linear-response approximation" making use of the Green-Kubo relations.
 

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