How do I treat IR divergences in e+/e- to mu+/mu- scattering?

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SUMMARY

In e+/e- to mu+/mu- scattering, infrared (IR) divergences arise when initial particles radiate photons. To address these divergences, it is essential to include all relevant diagrams up to a given order. The leading order matrix element M_1 is of order O(e^2), while the photon-emission diagram M_2 is of order O(e^3). To resolve the IR divergence, one must also incorporate renormalization diagrams, leading to a comprehensive expression for the matrix element that accounts for all contributions, ultimately allowing for the photon mass to be set to zero after calculations.

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eoghan
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Hi!

In e+/e- to mu+/mu- scattering, if the initial electron/positron radiates a photon, then I have an IR divergence. How do I treat it?
 
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Usually when you find an IR divergence it means that you didn't considered all the diagrams to a given order. For example, in the ee->μμ scattering you have the tree level diagram that is of order M_1=O(e^2) (where M is the related matrix element). If you want to add the diagram in which the initial electron emits a photon then you are adding a diagram of order M_2=O(e^3). Then, considering that you will have to take the square of the matrix elements your leading order will be |M_2|^2=O(e^6).
To resolve the IR divergence you have to add, for example, the diagrams in which the one of the initial (or final) particles emits and then re-absorb this photon (that is a renormalization diagram). This new diagram lead to a matrix element M_3=O(e^4) and so it could seem to be of higer order. But, since they all compete to the same phenomenon you will have to take the square of the sum of the diagrams and thus you obtain:

$$|M_1+M_2+M_3|^2=|M_1|^2+|M_2|^2+|M_3|^2+2Re(M_1^*M_2)+2Re(M_1^*M_3)+2Re(M_2^*M_3)=O(e^4)+O(e^6)+O(e^8)+O(e^5)+O(e^2)+O(e^7)$$

so, as you can see you have to include also the second mixed term in order to consider all the diagrams to the same order.

What you usually do is to give a small mass to the photon (in order to avoid divergences during calculations) and consider all these contribution. And the end of the calculation you can set the photon mass to zero.
 

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