Gauge symmetry and renormalization

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SUMMARY

Gauge symmetry plays a crucial role in the renormalization of quantum field theories, as established by 't Hooft and Veltman in their 1972 paper on the regularization and renormalization of gauge fields. The Ward-Takahashi identities illustrate how gauge invariance is preserved during renormalization, allowing for perturbative calculations across all orders in the coupling constant. The discussion highlights that while gauge theories are often associated with renormalizability, there exist non-gauge theories, such as the \(\phi^4\) theory, that are also renormalizable. However, theories that violate gauge symmetry, like Fermi's theory of weak interactions, are inherently non-renormalizable.

PREREQUISITES
  • Understanding of gauge symmetry in quantum field theory
  • Familiarity with renormalization techniques and concepts
  • Knowledge of Noether's Theorem and its implications
  • Basic comprehension of the Standard Model of particle physics
NEXT STEPS
  • Study the implications of Noether's Theorem in gauge theories
  • Explore the regularization and renormalization techniques used in quantum field theories
  • Investigate the differences between gauge and non-gauge theories, particularly in the context of renormalization
  • Read 't Hooft and Veltman's paper on the regularization and renormalization of gauge fields for in-depth understanding
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Physicists, particularly theoretical physicists and particle physicists, who are interested in the foundations of quantum field theory, gauge theories, and the renormalization process.

Lapidus
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Here and then I read gauge symmetry makes theories renormalizable. Unfortunately I could not find a satisfactory explanation why that so is. Could someone shed some light?

thanks
 
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It must have something to do with the Ward-Takahashi identities, I believe.

Anybody here who knows a little about gauge symmetry and renormalization and could help?

Note: some texts show how renormalization does not destroy gauge invariance, a fact that at first, of course, is not obvious. But then I read sometimes that gauge symmetry makes renormalization possible, like for example here in Perkins "Particle Astrophysics":

Why do we stress the concept of gauge invariance? The point of a gaugeinvariant theory is that it introduces a symmetry in the calculations, which
makes the theory renormalizable. This means that it is possible, at least in
principle, to make calculations in the form of a perturbation series to all orders
in the coupling constant, that is, for a sum over all possible Feynman diagrams,
including those involving an arbitrary number of exchanged photons.

Unfortunately, he fails to explain how exactly gauge symmetry makes theories renormalizable.thanks again
 
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Well, the base explanation is Noether's Theorem of course. Dunno what exactly explanation you looking for
 
Yes, proving this is nontrivial but it was done (and the authors won a Nobel prize for it). The reference is

'T Hooft and Veltman, regularization and renormalization of gauge fields. Nucl. Phys. B44: 189-213, 1972
 
A rather good overview of the subject by 't Hooft can be found http://www.staff.science.uu.nl/~hooft101/gthpub/GtH_Yukawa_06.pdf" .
 
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Bill_K said:
A rather good overview of the subject by 't Hooft can be found http://www.staff.science.uu.nl/~hooft101/gthpub/GtH_Yukawa_06.pdf" .

Very good overview, indeed.

But as I understand t'Hooft and Veltmann showed that renormalizing a gauge invariant theory does not spoil the gauge invariance of the theory.

My question: is gauge symmetry even necessary to make some theories renormalisable (as it is claimed sometimes)?
 
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Lapidus said:
Very good overview, indeed.

But as I understand t'Hooft and Veltmann showed that renormalizing a gauge invariant theory does not spoil the gauge invariance of the theory.

My question: is gauge symmetry even necessary to make some theories renormalisable (as it is claimed sometimes)?

There are certainly renormalizable theories which are not gauge theories (\phi^4 theories with real \phi come to mind). What you may be thinking of is that certain types of non-renormalizable theories can be seen to be low-energy effective theories arising from the spontaneous breaking of a gauge symmetry; and, casting them in this light restores renormalizability.
 
Parlyne said:
There are certainly renormalizable theories which are not gauge theories (\phi^4 theories with real \phi come to mind). What you may be thinking of is that certain types of non-renormalizable theories can be seen to be low-energy effective theories arising from the spontaneous breaking of a gauge symmetry; and, casting them in this light restores renormalizability.

Well, I was not thinking of much! But I think you correctly sumed up what people mean when they say that gauge symmetry makes some theories renormalizable. Like that Fermi's theory for the weak force is not renormalisable, but the gauge-invariant Weinberg-Salam theory is.

thanks everybody
 
Another reason one usually say that gauge symmetry is required for renormalization is related to the construction of the Standard Model.

In fact if you start from the Yang-Mills Lagrangian and add an arbitrary mass term without the Higgs mechanism, thus spoiling gauge symmetry, you end up with a non renormalizable theory.
 

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