Renormalizable Sectors in Resonance Chiral Theory: S -> pi pi Decay Amplitude

dc.creatorXiao, L. Y.
dc.creatorSanz-Cillero, J. J.
dc.date2007-05-26
dc.date.accessioned2026-07-07T11:16:23Z
dc.date.available2026-07-07T11:16:23Z
dc.descriptionWe develop a resonance chiral theory without any a priori limitation on the number of derivatives in the hadronic operators. Through an exhaustive analysis of the resonance lagrangian and by means of field redefinitions, we find that the number of independent operator contributing to the S -> pi pi decay amplitude is finite: there is only one single-trace operator (the cd term) and three multi-trace terms. The deep implication of this fact is that the ultraviolet divergences that appear in this amplitude at the loop level can only appear through these chiral invariant structures. Hence, a renormalization of these couplings renders the amplitude finite.
dc.description4 pages
dc.identifierhttps://arxiv.org/abs/0705.3899
dc.identifierhttp://arxiv.org/abs/0705.3899
dc.identifierPhys.Lett.B659:452-456,2008
dc.identifierdoi:10.1016/j.physletb.2007.10.080
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/192657
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Theory
dc.titleRenormalizable Sectors in Resonance Chiral Theory: S -> pi pi Decay Amplitude
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