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The origin of three-cocycles in quantum field theory

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When quantising a classical field theory it is not automatic that a group of symmetries of the classical system is preserved as a symmetry of the quantum system. Apart from the phenomenon of symmetry breaking it can also happen (as in Faddeev's Gauss law anomaly) that only an extension of the classical group acts as a symmetry group of the quantum system. We show here that rather than signalling a failure of the associative law as has been suggested in the literature, the occurrence of a non-trivial three-cocycle on the local gauge group is an "anomaly" or obstruction to the existence of an extension of the local gauge group acting as a symmetry group of the quantum system.

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Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics

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