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Particules Élémentaires, Gravitation et CosmologieAnnée 2004-2005Interactions fortes et chromodynamique quantique I:Aspects perturbatifsCours VIII: 19 avril 2005Symmetries & Anomalies1. Global vs. local symmetries2. Classical global symmetries, conserved currents3. Explicit breaking, accidental symmetries,anomalies4. Explicit vs. spontaneous symmetry breaking5. CP & U(1) problems in QCD19 avril 2005 1G. Veneziano, Cours no. 81. Global vs. local symmetries In QFT we have to make the important distinctionbetween global (rigid) and local symmetries Example of former is Lorentz(Poincaré) invariance Example of latter are the gauge symmetries(NB. General Relativity can be seen as a gaugetheory with G = local Poincaré-group: x -->x’(x)) Recall: local symmetries mean that some d.o.f. areunphysical => they are sacred (have to be broken«carefully» ) Global symmetries are not sacred: we are allowedto break them explicitly19 avril 2005 2G. Veneziano, Cours no. 8 Occasionally symmetries of S are broken at thecl quantum level (i.e. in S ). One talks about aneff«anomaly» We have seen an example all along: Classical-CDcontains no dimensionful parameter, but QCDcontains a scale, : one talks indeed about a scale-invariance (or trace) anomaly, anomalousdimensions etc. Anomalies are acceptable in global symmetries Anomalies unacceptable in local symmetries (animportant constraint on the standard model andits possible extensions)19 avril ...
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