Cross-section for elastic scattering?

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SUMMARY

The discussion centers on the elastic scattering of two charged fermions, specifically addressing the divergence encountered when calculating the cross-section using the tree-level approximation, which varies as ##\sim 1/t##. The divergence arises from integrating the square modulus over the Mandelstam variable t, particularly at t=0, leading to a collinear singularity. This issue is acknowledged in quantum field theory, particularly in theories involving massless particles exchanged in the t and u channels, and is resolved through resummation techniques. For further understanding, the participants recommend consulting Weinberg's "Quantum Theory of Fields, Vol. I," which covers infrared problems extensively.

PREREQUISITES
  • Understanding of tree-level approximations in quantum field theory
  • Familiarity with the Mandelstam variables, particularly t
  • Knowledge of collinear singularities and their implications in scattering theory
  • Basic grasp of resummation techniques in quantum field theory
NEXT STEPS
  • Study the concept of collinear singularities in quantum field theory
  • Learn about resummation techniques for handling divergences
  • Examine Weinberg's "Quantum Theory of Fields, Vol. I" for insights on infrared problems
  • Explore the implications of massless particle exchanges in scattering processes
USEFUL FOR

Physicists, particularly those specializing in quantum field theory, particle physicists, and students seeking to understand the intricacies of scattering processes and the associated divergences in theoretical frameworks.

muppet
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Hi All,

Following on from the last dumb question I asked...

Suppose you calculate the tree-level approximation to the elastic scattering of two charged fermions
to find that the result varies as ##\sim 1/t##, where t is the Mandelstam variable describing the squared momentum transfer in the centre of mass frame.

To work out the corresponding cross-section, you integrate the square modulus of this over t with t=0 as one of your limits of integration, so that the result diverges. Why is this not regarded as a problem?
 
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This is regarded as a problem, a socalled collinear singularity. It always occurs for theories with massless particles exchanged in the t and u channels. The cure is a resummation in this channel. Look at Weinberg, Quantum Theory of Fields, Vol. I. There's a whole chapter is devoted to infrared problems.
 
Thanks for your reply. I've heard of collinear singularities, but I'd always had the impression that such singularities canceled other divergences from the same order in perturbation theory- e.g. infrared divergences in loop integrals being canceled by those from bremstrahlung, so I couldn't see how such higher-order terms would cancel a tree-level effect. Guess I need to look into Weinberg, thanks.
 

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