Radiation from a dielectric body

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Discussion Overview

The discussion revolves around the derivation of radiation emitted by a dielectric body, specifically focusing on the spectral density of radiation from a semi-infinite dielectric material at a given temperature. Participants explore the theoretical underpinnings and seek references for a first-principles approach to this topic.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant seeks sources for the derivation of spectral density of radiation from a dielectric body, suggesting that it should be straightforward using Lorentzian harmonic oscillators.
  • Another participant argues that anharmonic terms in the Hamiltonian are necessary for a realistic model, as a purely harmonic Hamiltonian would result in negligible emissivity.
  • A third participant expresses surprise at the lack of first-principles treatments of radiated energy density from dielectric bodies, suggesting it should be of significant academic interest.
  • One participant questions whether damped harmonic oscillators could account for absorption in the dielectric, indicating a potential connection to the discussion of anharmonic terms.
  • Another participant mentions the relationship between emissivity and reflectivity for opaque materials, suggesting a similar relation for dielectrics that includes transmission, but notes a lack of specific references.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of anharmonic terms and the role of damped oscillators in modeling absorption. There is no consensus on the best approach or available references for the derivation sought.

Contextual Notes

Participants acknowledge the complexity of the topic, including the need for anharmonic terms and the implications of different models on emissivity and absorption, but do not resolve these issues.

Karthiksrao
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Dear all,

I needed help in finding a source where the derivation of radiation emitted by a dielectric body is laid out.

The derivation of spectral density of radiation emitted from a blackbody at a temperature ##T## is given in many books by populating the energy states using Bose-Einstein statistics. However, try as I might, I have not been able to find any source where the derivation of the spectral density of radiation emitted by a semi-infinite body with a dielectric function ##\varepsilon (\omega)## and at a temperature ##T## is derived from first-principles (populating the quantum states).

I'd assume it should be straightforward since the dielectric function can be approximated by Lorentzian harmonic oscillators. Is it not so ?

Do you know any book/paper which discusses this in detail ?

Many thanks!
 
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I think it takes more than a dielectric function and/or oscillators. It is necessary to have anharmonic terms (essentially non-linear in the restoring force or non-quadratic in the energy) in the Hamiltonian, which may give you a complex dielectric function (with imaginary components) and a complex index of refraction. A completely harmonic Hamiltonian would give you a completely transparent dielectric and thereby the emissivity would likely be near zero. I think the solid state physics book by Ashcroft and Mermin discusses the anharmonic Hamiltonian. I don't have any handy references that have the precise derivation you are looking for, but hopefully this is helpful.
 
I'm surprised why this topic of radiated energy density by a dielectric body is not commonly dealt with from first principles. I'd assume it to be of primary academic interest.
 
Regarding what you mentioned, won't damped harmonic oscillators account for absorption in the dielectric ?
 
Karthiksrao said:
Regarding what you mentioned, won't damped harmonic oscillators account for absorption in the dielectric ?
I think the two are mathematically quite similar, but you might find it written up in the solid state textbooks as an anharmonic term. Meanwhile, one other thing to consider would be a Kirckhoff's law type equation where for an opaque material the emissivity plus the reflectivity is equal to unity. For a dielectric, I think you have a similar relation with a transmission term included. I don't know of a good source that discusses this concept in depth, but hopefully you might find one.
 

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