Gauge anomalies (and cancellations)

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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.