Shifting integration variable when determing population densities

AI Thread Summary
The discussion centers on the integration variable shift in calculating fermion number density influenced by a space-time dependent field B_a. It is noted that this shift, where \(\vec{p}\) is replaced by \(\vec{p} + \vec{B}\), is valid only if B_a is treated as constant. If B_a is not constant, the momentum states of the fermions would fluctuate over time, complicating the integration process. The participants agree that without a specific form for B, further progress in the analysis is limited. The conversation highlights the challenges in handling variable fields in quantum statistical mechanics.
"Don't panic!"
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Hi,

I'm hoping someone can enlighten me on this as I'm a little bit fuzzy on the reasoning:

Say I have a space-time dependent field B_{a} that interacts with fermions such that it affects their energy dispersion. It appears in the energies in the form

E\sim\sqrt{\left(\vec{p}+\vec{B}\right)-m^{2}}+B_{0}

Why is it, that when I then calculate the number density of fermions in such a scenario, i.e.

n\sim\int^{+\infty}_{-\infty}\frac{d^{3}p}{\left(2\pi\right)^{3}}\frac{1}{\exp{\left(E/k_{_{B}}T\right)}+1}

(where in this case the chemical potential is negligible) that I can only shift the integration variable, such that \vec{p}\rightarrow \vec{p}+\vec{B} (thus "absorbing" the 3-vector components of B_{a}), if I consider B_{a} to be constant?

Thanks in advance!
 
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Apologies for the spelling mistake in the title of the thread by the way, should be "determining" , but don't know how to retroactively edit it!
 
What do you think would happen to d3p if B is not constant?
 
Would it be that it becomes time dependent and thus coupled to the fluctuations in B over time?
 
or more explicitly, that you would also introduce an additional integral over d^{3}B?
 
Slow down with the questions and answer my question in post #3
 
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sorry, they were my attempts at a possible answer (shouldn't have included the question marks)!

I assume that you would have d^{3}p\rightarrow d^{3}\left(p+B\right)=d^{3}p' and so, as B is not constant, one could not talk of set momentum states for the fermions as they would fluctuate in time depending on the fluctuations in B.
 
"Don't panic!" said:
sorry, they were my attempts at a possible answer (shouldn't have included the question marks)!

I assume that you would have d^{3}p\rightarrow d^{3}\left(p+B\right)=d^{3}p' and so, as B is not constant, one could not talk of set momentum states for the fermions as they would fluctuate in time depending on the fluctuations in B.

Correct. If you have a explicit form for B then you might attempt a solution. You can't go much further with the general expression, I don't think
 
ok, that's cleared things up a bit. Thanks for your time.
 
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