Gauge anomalies (and cancellations)

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SUMMARY

This discussion focuses on the complexities of gauge anomalies and cancellations, particularly in the context of chiral theories and their associated Lagrangian symmetries. Participants emphasize that gauge anomalies are not merely perturbative phenomena, as commonly depicted through Feynman diagrams, but rather stem from a fundamental symmetry discrepancy between classical and quantum models. The conversation highlights the importance of understanding these anomalies nonperturbatively, suggesting that in lattice studies, no symmetry would be broken at all.

PREREQUISITES
  • Understanding of gauge theories and anomalies
  • Familiarity with Lagrangian mechanics and symmetries
  • Knowledge of Feynman diagrams and perturbation theory
  • Concept of chiral theories in quantum field theory
NEXT STEPS
  • Research "nonperturbative gauge theories" for deeper insights
  • Explore "lattice gauge theory" to understand symmetry implications
  • Study "anomalies in quantum field theory" for comprehensive knowledge
  • Examine "chiral symmetry breaking" and its effects on gauge theories
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This discussion is beneficial for theoretical physicists, quantum field theorists, and advanced students seeking to deepen their understanding of gauge anomalies and their implications in quantum mechanics.

diegzumillo
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Hey all
As usual I can get through the specifics of calculations on books but the big picture escapes me. I'm having difficulty understanding gauge anomalies and cancellations. To be more specific, every book I read talks about Feynman diagrams, giving the impression that gauge anomalies are a perturbative phenomena. On the other hand, the anomaly seems to come from a symmetry of the lagrangian on chiral theories, and I don't see anything perturbation-specific there.

I'd appreciate any help, indlucing some interesting references on the subject.
 
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The point is that an "anomalous" symmetry is a symmetry which is a symmetry of the classical model but not of the quantum model. So nonperturbatively, you won't see any symmetry at all.
 
Just to be clear. When you say classical model and quantum you are referring to the Lagrangian symmetries and the usual quantization procedures, or equivalently tree-level and higher order diagrams, right? And in a hypothetical scenario, if we could study this system in, say, a lattice there would be no symmetry to be broken in the first place.
 

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