Completing Continuum Coulomb Gauge in the Functional Formalism

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dc.creatorWatson, P.
dc.creatorReinhardt, H.
dc.date2007-11-19
dc.date.accessioned2026-07-07T08:43:48Z
dc.date.available2026-07-07T08:43:48Z
dc.descriptionIt is argued that within the continuum functional formalism, there is no need to supply a further (spatially independent) gauge constraint to complete the Coulomb gauge of Yang-Mills theory. It is shown explicitly that a natural completion of the gauge-fixing leads to a contradiction with the perturbative renormalizability of the theory.
dc.description4 pages, no figures
dc.identifierhttps://arxiv.org/abs/0711.2997
dc.identifierhttp://arxiv.org/abs/0711.2997
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/142442
dc.subjectHigh Energy Physics - Theory
dc.subjectHigh Energy Physics - Lattice
dc.subjectHigh Energy Physics - Phenomenology
dc.titleCompleting Continuum Coulomb Gauge in the Functional Formalism
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