Normal ordering for bosons vs fermions

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SUMMARY

The discussion addresses the differences in normal ordering for bosons and fermions within quantum mechanics. It highlights that while normal ordering for bosons disregards commutation rules, fermions require consideration of anti-commutation rules, leading to a change in sign due to the nature of fermionic operators. The paper referenced, available at this link, clarifies that ignoring commutation rules for bosons results in a mere shift of energy eigenvalues, while for fermions, the implications are more significant than just energy shifts.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with bosonic and fermionic operators
  • Knowledge of Hamiltonian mechanics
  • Comprehension of commutation and anti-commutation relations
NEXT STEPS
  • Read the paper on normal ordering available at this link
  • Explore the implications of energy eigenvalue shifts in quantum harmonic oscillators
  • Investigate the role of anti-commutation in fermionic systems
  • Study the effects of normal ordering on quantum field theory
USEFUL FOR

Physicists, quantum mechanics students, and researchers focusing on quantum field theory and the behavior of bosons and fermions will benefit from this discussion.

planetology
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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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