Kramers Kronig transforms for refractive index

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Discussion Overview

The discussion centers on the application of Kramers-Kronig transforms to the refractive index and its relationship with the electric susceptibility. Participants explore the theoretical implications and definitions surrounding these concepts, particularly in the context of dispersion relations and response functions.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that the Kramers-Kronig transform relates the real and imaginary components of the electric susceptibility, \chi(\omega), and also applies to the refractive index.
  • Others argue that the refractive index is not a primary concept but is derived from the permittivity tensor, which is a response function that satisfies the Kramers-Kronig relations.
  • A participant emphasizes that the real and imaginary parts of the refractive index can be related through Kramers-Kronig transformations, suggesting a different perspective on the relationship between these quantities.
  • Another participant expresses skepticism about the refractive index satisfying Kramers-Kronig relations in general, arguing that the relations should apply to permittivity and that the refractive index is more about definitions than physics.
  • A later reply suggests that the Kramers-Kronig relations can indeed be applied to the index of refraction, referencing a monograph for further reading.

Areas of Agreement / Disagreement

Participants exhibit disagreement regarding the applicability of Kramers-Kronig relations to the refractive index, with some asserting its relevance while others challenge this view. The discussion remains unresolved, with multiple competing perspectives presented.

Contextual Notes

Participants highlight the dependence on definitions and the conceptual nature of the refractive index versus the permittivity tensor. There are unresolved questions regarding the implications of causality in electrodynamics and the specific conditions under which Kramers-Kronig relations apply.

christianjb
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I'm puzzled (as usual).

The Kramers Kronig transform is commonly used to relate real and imaginary components of the electric susceptibility- \chi(\omega)

It appears from reading papers that it also works for relating real and imaginary components of the refractive index.

But why? That means that the refractive index can be written as the FT of a response function. What is that response function?
 
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Well, there must be some misunderstanding.

The refractive index is not really a primary concepts, it related wavevector and frequency in a solution of a dispersion relation.

The primary concept is that of the permittivity tensor, and it is a response function.
The permittivity tensor satisfies indeed the Kramers Kronig relations.
This has consequence on the propagating modes, that are solutions of the dispersion relation, and therefore it has a consequence on the refractive index.

But, of course, it make no sense to say that the refractive index satisfies in any way the http://en.wikipedia.org/wiki/Kramers-Kronig_relations" .
 
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lalbatros said:
Well, there must be some misunderstanding.

The refractive index is not really a primary concepts, it related wavevector and frequency in a solution of a dispersion relation.

The primary concept is that of the permittivity tensor, and it is a response function.
The permittivity tensor satisfies indeed the Kramers Kronig relations.
This has consequence on the propagating modes, that are solutions of the dispersion relation, and therefore it has a consequence on the refractive index.

But, of course, it make no sense to say that the refractive index satisfies in any way the http://en.wikipedia.org/wiki/Kramers-Kronig_relations" .

The real and imaginary portions of the index of refraction are related by the Kramers-Kronig transformations, not jus the real and imaginary parts of \chi

Replace the real part by n - 1 and the imaginary part by k. More publications dealing with this topic work with n and k than with \chi.
 
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Dr Transport,

Since, in the simplest situations (waves in vacuum), the refractive index is the square root of the permitivity, I have difficulties to imagine that it could satisfy the KK relation in general. Moreover, I does not really matter since anyway the KK relation on the permitivity should cover the whole effect of causality in electrodynamics.

Moreover, my definition of the refractive index is associated with any particular solution of the dispersion relation. For example, for longitudinal oscillations in an unmagnetised plasma, the dispersion relation is simply

epslo(w,k)=0 (where epslo is the longitudinal part of the permitivity)​

Solving for w provides the dispersion curve of the longitudinal mode and the so-called refraction index
n = Re(k)/w​
for this mode.

I can imagine however that the KK relation on the permitivity implies some particular properties for the refractive index. But I would consider that as a freedom of language.

As the question assumed, the refractive index is in no way a transfer function and assuming the KK are a property of causal transfer functions, it may be a bit excessive to say that the KK applies to the refractive index.

So it seems more a question of definitions than really a question of physics.

Michel
 
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