Gauge symmetry and renormalization

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Discussion Overview

The discussion revolves around the relationship between gauge symmetry and renormalization in theoretical physics. Participants explore whether gauge symmetry is necessary for the renormalizability of certain theories, referencing various theoretical frameworks and historical contributions to the topic.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about how gauge symmetry contributes to the renormalizability of theories and seeks clarification.
  • Another suggests that the Ward-Takahashi identities may play a role in understanding the connection between gauge symmetry and renormalization.
  • It is mentioned that some texts indicate renormalization does not destroy gauge invariance, but the exact mechanism by which gauge symmetry facilitates renormalization is unclear to some participants.
  • Noether's Theorem is referenced as a foundational explanation, though its implications are not fully elaborated upon.
  • A participant cites 't Hooft and Veltmann's work as a significant contribution to the understanding of renormalization in gauge theories.
  • There is a discussion about whether gauge symmetry is necessary for renormalizability, with examples of renormalizable theories that do not involve gauge symmetry, such as certain \(\phi^4\) theories.
  • Another participant notes that some non-renormalizable theories can be viewed as low-energy effective theories resulting from spontaneous gauge symmetry breaking, which may restore renormalizability.
  • It is pointed out that the construction of the Standard Model relies on gauge symmetry, and that introducing mass terms without the Higgs mechanism leads to non-renormalizable theories.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of gauge symmetry for renormalization, with some asserting that it is essential while others provide counterexamples of renormalizable theories that lack gauge symmetry. The discussion remains unresolved regarding the definitive role of gauge symmetry in renormalization.

Contextual Notes

Participants acknowledge the complexity of the topic, with references to historical works and theoretical constructs that may not be fully understood or agreed upon. There are indications of missing assumptions and the need for further clarification on specific points.

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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