Are energy levels in a Debye solid equivalent to particles?

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    Debye Solid
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SUMMARY

The discussion centers on the relationship between energy levels and particles in a Debye solid, specifically regarding the density of states at a given frequency ν. Participants clarify that while the density of states represents the number of available modes at frequency ν, it does not equate to the total number of photons. Instead, each energy level at frequency ν can be populated by multiple photons, leading to a misunderstanding of the relationship between energy levels and particle count. The key takeaway is that the density of states reflects the number of modes, not the total photon count.

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  • Understanding of the Debye model in solid-state physics
  • Familiarity with concepts of density of states and phonons
  • Knowledge of quantum mechanics, particularly photon energy levels
  • Basic grasp of statistical mechanics and particle distributions
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Physicists, materials scientists, and students studying solid-state physics who seek to deepen their understanding of the Debye model and the behavior of phonons and photons in solids.

Karthiksrao
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Dear all,

In the wiki article about Debye solid :
https://en.wikipedia.org/wiki/Debye_model , in the section 'Another derivation', below Eq. 6, the following statement is provided:
382bf6a9a1564fd0f9e1ea0af7e89d19.png


Here, I understand the right hand side, which is nothing but the density of states/modes at the frequency \nu.

I fail to understand how this can be equated to the total number of photons (particles) Sigma n_i

Is each mode/state equivalent to a particle ?

Thanks!
 
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It's not the total number of phonons but just the total number of phonons with frequency ## \nu ##. For a given frequency you can have different energies associated (Ei) and for each energy level you have some number of phonons (ni).
 
oh yes, I did actually have in mind total number of photons with frequency \nu.

So just to clear things up, at every frequency \nu, there are many energy levels corresponding to 1 h \nu, 2 h \nu, 3 h \nu, etc.
Each of these energy levels is populated by photons. If you add up the number of photons distributed in all these energy levels, I am unable to visualize why this sum comes out to be just equal to the number of energy levels at frequency \nu (or the density of states at frequency \nu) represented by dN(\nu) in the expression. Can't each energy level hold more than one photon ? That doesn't seem right.
 

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