What about small momentum divergences?

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Discussion Overview

The discussion revolves around the topic of momentum divergences in integrals related to quantum field theory, particularly focusing on small momentum divergences in the context of dimensional regularization and their implications in theories such as QED and QCD.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant notes that integrals of the form \int\, \frac{d^{d}l}{l^4} diverge at large l for d>=4, questioning why small l divergences are not similarly concerning when d<4.
  • Another participant explains that in the case of a massive field, small l divergences are less of a concern due to the presence of a nonzero mass term in the denominator.
  • It is mentioned that in QED, involving massless photons, infrared divergences do occur and require special handling.
  • A different viewpoint suggests that small momentum divergences are significant, highlighting the existence of an infinite number of zero angle, zero energy photons along an electron's line, which necessitates integrating over finite angles and energies to obtain finite results.

Areas of Agreement / Disagreement

Participants express differing views on the significance of small momentum divergences, with some arguing they are not a concern in certain contexts while others assert their relevance, particularly in QED and QCD.

Contextual Notes

The discussion highlights the dependence on the mass of the field and the specific context of the theory being considered, indicating that assumptions about mass and dimensionality play a crucial role in the treatment of divergences.

LAHLH
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In Srednicki (ch14 say), he looks at integrals of the form [tex]\int\, \frac{d^{d}l}{l^4}...[/tex]. This is of course diveregent at large l if d>=4, which is easily seen by looking at the integrals measure in hyperspherical coords.

However, what about small l divergences, surely these occur if d<4, e.g. if d=3 we have something that goes as [tex]\frac{1}{l^2}[/tex], which diverges for small l. Why are we not concerned about this and only large l divergences?

Thanks
 
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LAHLH said:
Why are we not concerned about this and only large l divergences?
Because in the example you mentioned, Srednicki is dealing with a massive field.
I.e., there's a nonzero mass term in the denominator.

However, for QED involving the massless photon field, one does indeed encounter
so-called infrared divergences, which require special handling.
 
ah I see, thanks a lot.
 
Those small momentum divergences may be real : for instance, there is really an infinity of zero angle zero energy photons along an electron's line. One has to integrate the cross section over finite angle and finite energy to get a finite result. This kind of divergence is also at the root of the concept of "jet" in QCD.
 

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