By analyzing B→X u ℓ ν ℓ spectra with a model based on soft-gluon resummation and an analytic time-like QCD coupling, we obtain Vub=(376013022)10−3 where the first and the second error refer to experimental and theoretical error, respectively. This model successfully describes the accurate experimental data in beauty fragmentation, which has similar soft-gluon effects. The |V ub | value is obtained from the available measured semileptonic branching fractions in limited regions of the phase space. The distributions in the lepton energy E ℓ , the hadron invariant mass m X , the light-cone momentum P+EX−pX , together with the double distributions in (m X ,q 2) and (E ℓ ,s hmax ), are used to select the phase-space regions. q 2 is the dilepton squared momentum and s hmax is the maximal m X 2 at fixed q 2 and E ℓ . The |V ub | value obtained is in complete agreement with the value coming from exclusive B decays and from an over-all fit to the standard model parameters. We show that the slight disagreement (up to +2σ) with respect to previous inclusive measurements is not related to different choices for the b (and c) masses, but to a different modeling of the threshold (Sudakov) region.
Inclusive measure of |V(ub)| with the analytic coupling model / U. Aglietti, F. Di Lodovico, G. Ferrera, G. Ricciardi. - In: THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS. - ISSN 1434-6044. - 59:4(2009), pp. 831-840. [10.1140/epjc/s10052-008-0817-x]
Inclusive measure of |V(ub)| with the analytic coupling model
G. FerreraPenultimo
;
2009
Abstract
By analyzing B→X u ℓ ν ℓ spectra with a model based on soft-gluon resummation and an analytic time-like QCD coupling, we obtain Vub=(376013022)10−3 where the first and the second error refer to experimental and theoretical error, respectively. This model successfully describes the accurate experimental data in beauty fragmentation, which has similar soft-gluon effects. The |V ub | value is obtained from the available measured semileptonic branching fractions in limited regions of the phase space. The distributions in the lepton energy E ℓ , the hadron invariant mass m X , the light-cone momentum P+EX−pX , together with the double distributions in (m X ,q 2) and (E ℓ ,s hmax ), are used to select the phase-space regions. q 2 is the dilepton squared momentum and s hmax is the maximal m X 2 at fixed q 2 and E ℓ . The |V ub | value obtained is in complete agreement with the value coming from exclusive B decays and from an over-all fit to the standard model parameters. We show that the slight disagreement (up to +2σ) with respect to previous inclusive measurements is not related to different choices for the b (and c) masses, but to a different modeling of the threshold (Sudakov) region.File | Dimensione | Formato | |
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