From a study of the kinematic properties of the final state produced in the semileptonic decays b --> Xlv(l), the inclusive charmless semileptonic branching ratio of b hadrons is measured. With a sample of 3.6 million hadronic Z decays recorded between 1992 and 1995 with the ALEPH detector at LEP, the value Br(b --> X(u)lv(l)) is determined to be (1.73 +/- 0.55(stat) +/- 0.55(syst)) x 10(-3), where X(u) represents any charmless hadronic state and b is a mixture of b hadrons weighted by their production rates. This measurement yields the result |V-ub|(2) = (18.68 +/- 5.94(stat) +/- 5.94(syst) +/- 1.45(HQE)) x 10(-6) where the last error comes from the conversion of the branching ratio to the CKM matrix element squared.

Determination of |V-ub| from the measurement of the inclusive charmless semileptonic branching ratio of b hadrons

G. Batignani;CIOCCI, MARIA AGNESE;FERRANTE, ISIDORO;FORTI, FRANCESCO;MESSINEO, ALBERTO MARIA;G. Rizzo;TONELLI, GUIDO EMILIO;
1999-01-01

Abstract

From a study of the kinematic properties of the final state produced in the semileptonic decays b --> Xlv(l), the inclusive charmless semileptonic branching ratio of b hadrons is measured. With a sample of 3.6 million hadronic Z decays recorded between 1992 and 1995 with the ALEPH detector at LEP, the value Br(b --> X(u)lv(l)) is determined to be (1.73 +/- 0.55(stat) +/- 0.55(syst)) x 10(-3), where X(u) represents any charmless hadronic state and b is a mixture of b hadrons weighted by their production rates. This measurement yields the result |V-ub|(2) = (18.68 +/- 5.94(stat) +/- 5.94(syst) +/- 1.45(HQE)) x 10(-6) where the last error comes from the conversion of the branching ratio to the CKM matrix element squared.
1999
Barate, R.; Buskulic, D.; Decamp, D.; Ghez, P.; Goy, C.; Lees, J. P.; Lucotte, A.; Merle, E.; Minard, M. N.; Nief, J. Y.; Pietrzyk, B.; Alemany, R.; B...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/828789
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