Normal ordering for bosons vs fermions

AI Thread Summary
The discussion centers on the differing treatment of boson and fermion operators in Hamiltonians, specifically regarding normal ordering and the application of commutation and anti-commutation rules. It highlights that for bosons, ignoring commutation rules leads only to a shift in energy eigenvalues, which does not affect measurable physics. In contrast, for fermions, the application of anti-commutation rules results in significant changes beyond mere energy shifts, justifying the need for careful consideration. A referenced paper provides insights but primarily addresses the harmonic oscillator case. Further investigation into the implications for fermions is suggested as the next step.
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Why is it that when normal ordering the terms in the Hamiltonian for bosons, the commutation rules are ignored, but when normal ordering fermion operators the anti-commutation rules are used to justify a change in sign?
 
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I remember thinking about this a few years ago, and I seem to remember the answer was in the fact that the negative sign canceled with another negative sign, giving the appearance that we ignore the rule.

Here is an easy-to-read document that will be of some assistance:

http://xxx.lanl.gov/pdf/physics/0212061

I will get back to this later with a more definitive post.
 
Originally posted by Tom


Here is an easy-to-read document that will be of some assistance:

http://xxx.lanl.gov/pdf/physics/0212061

I will get back to this later with a more definitive post.

Thanks, that paper is a really good one. I have not gotten all the way through it yet so don't know if it answers the main question, but very useful in any case.
 
OK, I re-read the paper, and it only states the reason for ignoring the commutation rules for the harmonic oscillator potential. The reason is that the only effect is to shift the energy eigenvalues by (1/2)hf. In other words, the physics is unchanged (because only energy differences are measurable).

So, I think that gives us a lead for why we don't ignore it for fermions: something more happens than a mere shift in the energies.

That would be the next thing to look into, I think.
 
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