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dc.contributor.author | Bodenstein, Sebastian | |
dc.contributor.author | Bordes Villagrasa, José M. | |
dc.contributor.author | Domínguez, Cesáreo A. | |
dc.contributor.author | Peñarrocha Gantes, José Antonio | |
dc.contributor.author | Schilcher, K. | |
dc.date.accessioned | 2015-03-12T13:53:39Z | |
dc.date.available | 2015-03-12T13:53:39Z | |
dc.date.issued | 2011 | |
dc.identifier.citation | Bodenstein, Sebastian Bordes Villagrasa, José M. Domínguez, Cesáreo A. Peñarrocha Gantes, José Antonio Schilcher, K. 2011 QCD sum rule determination of the charm-quark mass Physical Review D 83 7 074014 | |
dc.identifier.uri | http://hdl.handle.net/10550/42734 | |
dc.description.abstract | QCD sum rules involving mixed inverse moment integration kernels are used in order to determine the running charm-quark mass in the MS¯ scheme. Both the high and the low energy expansion of the vector current correlator are involved in this determination. The optimal integration kernel turns out to be of the form p(s)=1−(s0/s)2, where s0 is the onset of perturbative QCD. This kernel enhances the contribution of the well known narrow resonances, and reduces the impact of the data in the range s≃20−25GeV2. This feature leads to a substantial reduction in the sensitivity of the results to changes in s0, as well as to a much reduced impact of the experimental uncertainties in the higher resonance region. The value obtained for the charm-quark mass in the MS¯ scheme at a scale of 3 GeV is m¯c(3GeV)=987±9MeV, where the error includes all sources of uncertainties added in quadrature. | |
dc.language.iso | eng | |
dc.relation.ispartof | Physical Review D, 2011, vol. 83, num. 7, p. 074014 | |
dc.subject | Física | |
dc.title | QCD sum rule determination of the charm-quark mass | |
dc.type | journal article | es_ES |
dc.date.updated | 2015-03-12T13:53:39Z | |
dc.identifier.doi | 10.1103/PhysRevD.83.074014 | |
dc.identifier.idgrec | 069737 | |
dc.rights.accessRights | open access | es_ES |