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

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In summary, the counterterms introduced to cancel the divergences in 2-point and 4-point functions in a renormalizable theory are also sufficient to cancel the divergences in all n-point functions. This is because the more propagators added to a loop, the more convergent the loop integral becomes, making large n-point functions generally non-divergent. The attached diagram in the conversation shows an example of a divergent loop that can be cancelled by the same counterterm used to cancel the divergences in the 4-point function. Nontrivial cases may require further analysis, but this is the general idea discussed in Peskin & Schroeder sections 10.4 and 10.5.
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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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What is the purpose of renormalizing large n-pt functions with small n-pt functions?

The purpose of renormalizing large n-pt functions with small n-pt functions is to account for the effects of quantum corrections on the behavior of these functions. As the number of particles involved in a system increases, the effects of quantum fluctuations become more prominent and must be taken into consideration for accurate predictions.

How are small n-pt functions used in the renormalization process?

Small n-pt functions are used to calculate the contributions of virtual particles and interactions to the large n-pt functions. By subtracting these contributions, the large n-pt functions can be renormalized and made more accurate.

What is the significance of large n-pt functions in quantum field theory?

Large n-pt functions are important in quantum field theory because they describe the behavior of a system with a high number of particles. These functions can be used to calculate important quantities such as scattering amplitudes and correlation functions.

Can renormalization be applied to any type of n-pt function?

Yes, renormalization can be applied to any type of n-pt function. It is a general technique used in quantum field theory to account for the effects of quantum corrections on the behavior of these functions.

How does renormalization affect the predictions of n-pt functions?

Renormalization can significantly improve the predictions of n-pt functions by accounting for the effects of quantum corrections. This results in more accurate and reliable calculations, especially in systems with a high number of particles.

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