Debye model and dispersion relation

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SUMMARY

The discussion focuses on the application of the Debye model to analyze the heat capacity of bosons with a specific dispersion relation. It establishes that for bosons with a dispersion relation of the form \(\omega \sim A\sqrt{k}\), the heat capacity at constant volume \(C_V\) behaves as \(C_V \sim T^4\) when the temperature \(T\) is much less than the Debye temperature \(T_{Debye}\). The participants emphasize the importance of the density of states and the ultraviolet cutoff frequency \(\omega_{max}\) in deriving the heat capacity, linking these concepts to the dispersion relation.

PREREQUISITES
  • Understanding of the Debye model and its application to solid-state physics.
  • Familiarity with dispersion relations and their implications for vibrational modes.
  • Knowledge of statistical mechanics, particularly the concepts of heat capacity and energy distributions.
  • Basic calculus for evaluating integrals related to density of states.
NEXT STEPS
  • Study the derivation of the density of states for different dispersion relations.
  • Research the implications of the ultraviolet cutoff frequency \(\omega_{max}\) in thermal physics.
  • Learn about the relationship between energy \(E\), momentum \(p\), and frequency \(\omega\) in various contexts.
  • Explore the mathematical techniques for evaluating integrals in statistical mechanics.
USEFUL FOR

Students and researchers in condensed matter physics, particularly those studying thermal properties of materials and the behavior of bosonic systems at low temperatures.

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Homework Statement



I have seen case studies of the 3D Debye model where the vibrational modes of a solid is taken to be harmonic with dispersion relation \omega = c_sk. It is said that for temperatures much less than the Debye temperature, the heat capacity at constant volume C_V\sim T^3.

Now I want to show that for bosons with dispersion relation \omega\sim A\sqrt k has heat capacity C_V\sim T^4 for T\ll T_{Debye}.

In the case studies I have read, I can't find where the dispersion relation comes into play. I have no idea how to see this. Please help!

Homework Equations



Debye Temperature is given by T_{Debye}k_B=\hbar \omega_{max}



The Attempt at a Solution



Generally, I know I need to get the density of modes -- I have a suspicion that here is where the dispersion relation kicks in, but I don't know how.

After that, I should find the ultraviolet cutoff frequency \omega_{max}.

Then I should find the energy $$E=\int_0^\omega{max}d\omega {E(\omega)g(\omega)\over \exp(\beta(E-\mu))-1}$$ But what form does $E$ in the integrand take? I know that for photons with dispersion relation \omega = c_s k we have E=\hbar \omega.

After that, it's just a matter of taking limits and C_V=\left({\partial E\over \partial T}\right)_V (should) give the required result...
 
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Please, somebody?

OK, so I know that the density of state depends on the dispersion relation. What are the general definitions of E, p in terms of \omega, k? E.g. for the first case E=\hbar \omega and p=\hbar k. So the question is: what are the respective values for E,p in general?
 

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