Change of variables in the Density of States function

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SUMMARY

The discussion focuses on transforming the density of states function for a relativistic Fermion gas from momentum space, ##D(p)dp##, to energy space, ##D(\varepsilon)d\varepsilon##, using the relationship ##\varepsilon=cp##. The correct transformation yields ##\tilde{D}(\varepsilon) = \frac{1}{c} D(\varepsilon/c)##, confirming that the density transforms appropriately. The distinction between the functions ##D## and ##\tilde{D}## is crucial for clarity in notation and understanding the transformation process.

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AndersF
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TL;DR
Reexpress the density of states for a Fermion gas in terms of momentum in terms of the energy.
I have a problem where I am given the density of states for a Fermion gas in terms of momentum: ##D(p)dp##. I need to express it in terms of the energy of the energy levels, ##D(\varepsilon)d\varepsilon##, knowing that the gas is relativistic and thus ##\varepsilon=cp##.

Replacing ##p## by ##\varepsilon/c## and ##dp## by ##d\varepsilon/c##, I would get ##D(\varepsilon/c)d\varepsilon/c##, but I'm looking for ##D(\varepsilon)d\varepsilon## instead.

I'm missing something? I know this is basic stuff, but I am stuck and this issue has me clueless...
 
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You have
$$\tilde{D}(\epsilon) \mathrm{d} \epsilon=D(p) \mathrm{d} p$$
and
$$\mathrm{d} \epsilon=c \mathrm{d} p$$
So you get
$$\tilde{D}(\epsilon) c \mathrm{d} p = D(p) \mathrm{d} p=D(\epsilon/c) \mathrm{d} p,$$
from which finally
$$\tilde{D}(\epsilon)=\frac{1}{c} D(\epsilon/c),$$
which means that ##D## transforms as a density, as it must be.

You have to be careful with the notation. That's why I distinguished ##D## (function of ##p##) and ##\tilde{D}## (function of ##\epsilon##).
 
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Oh ok, I see, thank you very much!
 

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