Non-Uniqueness of Quantized Yang-Mills Theories

dc.creatorDuetsch, Michael
dc.date1996-06-17
dc.date.accessioned2026-07-07T10:58:44Z
dc.date.available2026-07-07T10:58:44Z
dc.descriptionWe consider quantized Yang-Mills theories in the framework of causal perturbation theory which goes back to Epstein and Glaser. In this approach gauge invariance is expressed by a simple commutator relation for the S-matrix. The most general coupling which is gauge invariant in first order contains a two-parametric ambiguity in the ghost sector - a divergence- and a coboundary-coupling may be added. We prove (not completely) that the higher orders with these two additional couplings are gauge invariant, too. Moreover we show that the ambiguities of the n-point distributions restricted to the physical subspace are only a sum of divergences (in the sense of vector analysis). It turns out that the theory without divergence- and coboundary-coupling is the most simple one in a quite technical sense. The proofs for the n-point distributions containing coboundary-couplings are given up to third or fourth order only, whereas the statements about the divergence-coupling are proven in all orders.
dc.description22 pages. The paper is written in TEX. The necessary macros are included
dc.identifierhttps://arxiv.org/abs/hep-th/9606100
dc.identifierhttp://arxiv.org/abs/hep-th/9606100
dc.identifierJ.Phys.A29:7597-7617,1996
dc.identifierdoi:10.1088/0305-4470/29/23/021
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/187209
dc.subjectHigh Energy Physics - Theory
dc.titleNon-Uniqueness of Quantized Yang-Mills Theories
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