Large n-pt functions renormalized by small n-pt functions?

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SUMMARY

The discussion centers on the renormalization of n-point functions in λφ4 theory, specifically addressing whether counter-terms from 2-point and 4-point functions can effectively cancel divergences in 3-particle scattering processes. It is established that in a renormalizable theory, counter-terms introduced for basic n-point functions are sufficient to cancel divergences in all n-point functions. The reasoning is that additional propagators in loop diagrams lead to convergence, and divergences in small loops are managed by the same counter-terms used for smaller n-point functions. Key references include sections 10.4 and 10.5 of Peskin & Schroeder.

PREREQUISITES
  • Understanding of λφ4 theory
  • Familiarity with renormalization techniques
  • Knowledge of n-point functions in quantum field theory
  • Ability to analyze loop diagrams and propagators
NEXT STEPS
  • Study the renormalization process in λφ4 theory
  • Examine Peskin & Schroeder sections 10.4 and 10.5 for detailed insights
  • Learn about the convergence of loop integrals in quantum field theory
  • Investigate the implications of interlocking divergent loops in higher n-point functions
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Quantum field theorists, particle physicists, and advanced students seeking to deepen their understanding of renormalization and n-point function behavior in λφ4 theory.

geoduck
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Suppose you have a λφ4 theory. Books only seem to calculate counter-terms for 2-pt and 4-pt functions.

But what about 3 particles scattering into 3 particles? Do the counter-terms determined by renormalizing the 2-pt and 4-pt functions cancel divergences in 3x3 scattering?

For example, take the graph below:

Is it obvious that the counter-terms from 2x2 and scattering, along with counter-terms from the 2-pt function, can cancel this graph?
 

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In a renormalizable theory, the counterterms that you introduce to cancel the divergences in a few basic n-point functions suffice to cancel the divergences in all n-point functions.

I think the intuitive reason for this is: the more propagators you add to a loop, the more convergent the loop integral becomes. So large n-point functions generally aren't divergent unless they contain a divergent subdiagram with a small loop. But the divergences in those small loops will be canceled by the counterterms that you introduced to make the small n-point functions finite.

For example look at the attached diagram that contributes to the 6-point function in ##\phi^4## theory. The loop has three propagators, so the loop integral goes like ##\int d^4 p / p^6##, which is convergent. The second attached image shows a divergent diagram contributing to the 6-point function. However the divergent loop looks just like one of the divergent contributions to the 4-point function, so it should be canceled by the same counterterm that cancels the divergence in the 4-point function.

In your diagram, I think the only divergent loop is the topmost loop. This divergence should be canceled by the same counterterm that cancels the divergences in the 4-point function.

I think there are nontrivial cases where there are "interlocking" divergent loops and it's not totally obvious that these ideas go through without doing some careful work, but this is the general picture.

Peskin & Schroeder sections 10.4 and 10.5 discuss these issues.
 

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