What is the origin of infrared divergence?

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SUMMARY

The origin of infrared divergence in quantum electrodynamics (QED) arises from the improper use of asymptotic states when dealing with massless particles, such as photons. Specifically, infrared divergences manifest through two primary mechanisms: the infinite emission probability of soft photons and the divergence of radiative corrections from virtual photons as energy approaches zero. To address these divergences, it is essential to incorporate a small mass for massless particles and recognize the experimental limitations in measuring outgoing electron energy. A comprehensive treatment of this topic is presented in the paper by P. P. Kulish and L. D. Faddeev, which discusses asymptotic conditions and infrared divergences in detail.

PREREQUISITES
  • Understanding of quantum electrodynamics (QED)
  • Familiarity with Feynman diagrams
  • Knowledge of perturbation theory in quantum mechanics
  • Basic concepts of asymptotic states in quantum theory
NEXT STEPS
  • Read "Asymptotic conditions and IR divergences in quantum electrodynamics" by P. P. Kulish and L. D. Faddeev
  • Study the concept of soft photon emission and its implications in QED
  • Explore the role of mass in regulating infrared divergences
  • Investigate the experimental limits of energy measurement in particle physics
USEFUL FOR

This discussion is beneficial for theoretical physicists, quantum field theorists, and students studying quantum electrodynamics, particularly those interested in the intricacies of infrared divergences and their implications in particle interactions.

ndung200790
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Please teach me this:
It seem that the ultraviolet divergence has origin of we unknow the physics at very small distance(very large momentum,then very small distance).So we must cut off the very large momentum by renormalization procedure.But I do not understand the origin of infrared divergence in Feynman diagrams.By the way,it seem that in order to cut off infrared divergence,the general procedure is to put a small mass for the massless particles.
Thank you very much in advance.
 
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The infrared divergence originates from using the wrong "asymptotic states" when massless particles (field quanta) like photons are involved.

The most simple example for this deficiency of a naive use of asympotic states is well-known also in non-relativistic quantum theory: For non-relativistic Coulomb scattering the asymptotic states are not plane waves (momentum eigenstates) but the Coulomb-scattering states, which have additional non-trivial phase factors.

A very nice treatment of IR divergences from this point of view is given in the paper (including the Coulomb-scattering example)

P. P. Kulish, L. D. Faddeev, Asympototic conditions and IR divergences in quantum electrodynamics, Theo. Math. Phys. 4, 745 (1970)
DOI: 10.1007/BF01066485
 
Infrared divergences arise in two ways: (a) the emission probability of soft photons (bremsstrahlung) becomes infinite with increasing wavelength, and (b) the radiative correction from a virtual photon diverges when integrated down to zero energy. If we do perturbation theory in the simplest way, we keep (b) but not (a) and obtain an infinite result.

The solution is to realize that the energy of an outgoing electron can only be determined experimentally to within some limit ΔE, and that therefore the emission of soft photons with energy < ΔE must be included. When (a) and (b) are combined, the result is finite.
 

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