Solving Perplexing Commutator for Simplification

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SUMMARY

The discussion focuses on simplifying the integral involving the commutator of field operators in quantum field theory. Specifically, it addresses the simplification of the expression \(\int d^3x' [\pi(x), \frac{1}{2}\pi^2(x') + \frac{1}{2} \phi(x')( -\nabla^2 + m^2)\phi(x')]\) using the properties of commutators. The key conclusions are that the commutator \([\pi(x), \pi(x')] = 0\) and \([\phi(x), \pi(x')] = -i\delta(x-x')\) allow the integral to simplify to \(\int d^3x' \delta(x-x')( -\nabla^2 + m^2)\phi(x')\), with the Laplacian effectively factored out through integration by parts and the application of the commutation relations.

PREREQUISITES
  • Understanding of quantum field theory concepts, particularly commutation relations
  • Familiarity with functional derivatives in quantum mechanics
  • Knowledge of integration techniques in multiple dimensions
  • Proficiency in manipulating differential operators such as the Laplacian
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  • Study the properties of commutators in quantum mechanics and quantum field theory
  • Learn about integration by parts in the context of functional integrals
  • Explore the role of delta functions in quantum field theory
  • Investigate the relationship between commutators and functional derivatives
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Physicists, particularly those specializing in quantum field theory, graduate students studying advanced quantum mechanics, and researchers looking to deepen their understanding of operator algebra in field theory.

waht
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When simplifying this

\int d^3x' [\pi(x), \frac{1}{2}\pi^2(x') + \frac{1}{2} \phi(x')( -\nabla^2 + m^2)\phi(x')]

we know that

[\pi(x), \pi(x')] = 0

[\phi(x), \pi(x')] = -i\delta(x-x')

how does that simplify to

\int d^3x' \delta(x-x')( -\nabla^2 + m^2)\phi(x')

I know that

[\pi(x), \pi^2(x')] = 0

but not sure how does the laplacian gets factored out like that and one-half disappears?
 
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Have you tried to see what part integration brings you ?
 
By expanding the commutator we get,

<br /> \frac{1}{2} \int d^3x&#039; \pi(x)\phi(x&#039;)( -\nabla^2 + m^2)\phi(x&#039;) - \phi(x&#039;)( -\nabla^2 + m^2)\phi(x&#039;)\pi(x)<br />

the laplacian in the second term is sandwiched between two phis, integration by part doesn't seem to help to factor it out.
 
I think you're better off using [A,BC] = [A,B]C + B[A,C] and then integration by parts. Also, it's a good time in your life to realize that a commutator behaves very much like a functional derivative (recall QM 101).
 

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