The Gribov-Zwanziger action in the presence of the gauge invariant, nonlocal mass operator $Tr \int d^4x F_{μν} (D^2)^{-1} F_{μν}$ in the Landau gauge

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dc.creatorCapri, M. A. L.
dc.creatorDudal, D.
dc.creatorLemes, V. E. R.
dc.creatorSobreiro, R. F.
dc.creatorSorella, S. P.
dc.creatorThibes, R.
dc.creatorVerschelde, H.
dc.date2007-05-24
dc.date.accessioned2026-07-07T10:55:48Z
dc.date.available2026-07-07T10:55:48Z
dc.descriptionWe prove that the nonlocal gauge invariant mass dimension two operator $F_{μν} (D^2)^{-1} F_{μν}$ can be consistently added to the Gribov-Zwanziger action, which implements the restriction of the path integral's domain of integration to the first Gribov region when the Landau gauge is considered. We identify a local polynomial action and prove the renormalizability to all orders of perturbation theory by employing the algebraic renormalization formalism. Furthermore, we also pay attention to the breaking of the BRST invariance, and to the consequences that this has for the Slavnov-Taylor identity.
dc.description30 pages
dc.identifierhttps://arxiv.org/abs/0705.3591
dc.identifierhttp://arxiv.org/abs/0705.3591
dc.identifierEur.Phys.J.C52:459-476,2007
dc.identifierdoi:10.1140/epjc/s10052-007-0379-3
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/186200
dc.subjectHigh Energy Physics - Theory
dc.titleThe Gribov-Zwanziger action in the presence of the gauge invariant, nonlocal mass operator $Tr \int d^4x F_{μν} (D^2)^{-1} F_{μν}$ in the Landau gauge
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