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Corrections to the SU(3 x SU(3) Gell-Mann-Oakes-Renner relation and chiral couplings Lr8 and Hr2

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Corrections to the SU(3 x SU(3) Gell-Mann-Oakes-Renner relation and chiral couplings Lr8 and Hr2

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dc.contributor.author	Bordes Villagrasa, José M.
dc.contributor.author	Domínguez, Cesáreo A.
dc.contributor.author	Moodley, Preshin
dc.contributor.author	Peñarrocha Gantes, José Antonio
dc.contributor.author	Schilcher, K.
dc.date.accessioned	2015-03-12T12:04:52Z
dc.date.available	2015-03-12T12:04:52Z
dc.date.issued	2012
dc.identifier.citation	Bordes Villagrasa, José M. Domínguez, Cesáreo A. Moodley, Preshin Peñarrocha Gantes, José Antonio Schilcher, K. 2012 Corrections to the SU(3 x SU(3) Gell-Mann-Oakes-Renner relation and chiral couplings Lr8 and Hr2 Journal of High Energy Physics 2012 10 102-1 102-11
dc.identifier.uri	http://hdl.handle.net/10550/42701
dc.description.abstract	Next to leading order corrections to the SU(3) × SU(3) Gell-Mann-Oakes-Renner relation (GMOR) are obtained using weighted QCD Finite Energy Sum Rules (FESR) involving the pseudoscalar current correlator. Two types of integration kernels in the FESR are used to suppress the contribution of the kaon radial excitations to the hadronic spectral function, one with local and the other with global constraints. The result for the pseudoscalar current correlator at zero momentum is psi 5(0) = (2.8 ± 0.3) ×10-3 GeV4, leading to the chiral corrections to GMOR: delta K = (55 ± 5)%. The resulting uncertainties are mostly due to variations in the upper limit of integration in the FESR, within the stability regions, and to a much lesser extent due to the uncertainties in the strong coupling and the strange quark mass. Higher order quark mass corrections, vacuum condensates, and the hadronic resonance sector play a negligible role in this determination. These results confirm an independent determination from chiral perturbation theory giving also very large corrections, i.e. roughly an order of magnitude larger than the corresponding corrections in chiral SU(2) × SU(2). Combining these results with our previous determination of the corrections to GMOR in chiral SU(2) × SU(2), delta pi , we are able to determine two low energy constants of chiral perturbation theory, i.e. L_8^r=( {1.0± 0.3} )× {10^{-3 }} , and H_2^r=-( {4.7± 0.6} )× {10^{-3 }} , both atthe scaleof the rho-meson mass.
dc.language.iso	eng
dc.relation.ispartof	Journal of High Energy Physics, 2012, vol. 2012, num. 10, p. 102-1-102-11
dc.subject	Física
dc.title	Corrections to the SU(3 x SU(3) Gell-Mann-Oakes-Renner relation and chiral couplings Lr8 and Hr2
dc.type	journal article	es_ES
dc.date.updated	2015-03-12T12:04:52Z
dc.identifier.doi	10.1007/JHEP10(2012)102
dc.identifier.idgrec	080404
dc.rights.accessRights	open access	es_ES