Prove Van Leeuwen's Theorem: Diamagnetism Does Not Exist in Classical Physics

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Van Leeuwen's theorem states that diamagnetism does not exist in classical physics, which is the focus of the discussion. The Hamiltonian changes in the presence of an external magnetic field, affecting the calculation of the partition function QN. The induced magnetization M is derived from the partition function, but challenges arise when integrating due to the magnetic field's influence. A solution was found by changing variables in the momentum integral, simplifying the calculation. This approach successfully demonstrates the theorem's implications in statistical mechanics.
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For a statistical mechanics course we have to prove Van Leeuwen's theorem: Diamagnetism does not exist in classical physics.

I know that in an external magnetic field H the Hamiltonian Ha goes from Ha(p1,p2,--------,pN ,q1,q2,-------qN) to Ha(p1-(e/c)A1, p2-(e/c)A2, ------- pN-(e/c)AN, q1,q2,------.qN)

I also know that the induced magnetization M = kT*d(log QN)/dH

So the problem is finding QN. I know how to calculate it for a perfect gas without the magnetic field but I can't seem to solve the integral when Ha changes.
 
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Try shifting integration variables.
 
Ah I found bij changing p - (e/c)A to p' and then integrating. Thanks a lot.
 
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