Kln theorem and initial-state singularities

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SUMMARY

The KLN theorem addresses infrared (IR) singularities in quantum field theory, specifically in the context of final-state emissions, where the singularities cancel when summing over degenerate states. However, for initial-state emissions, such as a parton radiating a gluon before interacting with a target, the IR divergence cannot be canceled in the same manner. This necessitates the renormalization of the parton distribution function (PDF) to account for the remnant IR divergences associated with soft and collinear gluons. The discussion highlights the limitations of the KLN theorem in addressing initial-state singularities and the reliance on PDFs to manage these divergences.

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  • Understanding of the KLN theorem in quantum field theory
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eoghan
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Hi!
If I have a pair q\bar q g in a final state, I know that the gluon has a IR singularity. But KLN theorem rescues me: if I sum over all degenerate states the IR singularity cancels away.
Otherwise, if the emission of the soft gluon is in an initial state, then the IR divergence cannot be canceled. Why KLN doesn't work for initial-state singularities?
I'm thinking of the hard scattering of a parton from an hadron with a target. If the parton radiates a gluon before it hits the target, then I can't cancel the IR singularity, unless I "renormalize" the parton distribution function. Why can't I sum over all initial degenerate states to cancel the singularity?
 
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This is a post from 2012 but I was wondering the same question ^^ - the remnant IR divergences coming from collinear/soft gluons in the initial state are 'put under the rug' into the PDF associated with the mother hadron from which the parton came from. This is the treatment I have seen everywhere but if I did an inclusive summation over all initial degenerate states would I get no IR divergences as the KLN theorem perhaps tells me and, if so, what would such initial states look like?
 

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