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  • Determination of heavy quar...
    Adam, W; Albrecht, T; Alemany-Fernandez, R; Allport, P; Amaldi, U; Andringa, S; Antilogus, P; Apel, WD; Asman, B; Baillon, P; Ballestrero, A; Barbier, R; Begalli, M; Benekos, N; Bloch, D; Blom, M; Bonesini, M; Botner, O; Boyko, I; Brenner, R; Brodet, E; Bruckman, P; Brunet, M; Camporesi, T; Canale, V; Carena, F; Chudoba, J; Collins, P; Cosme, G; De Angelis, A; De Clercq, C; Di Simone, A; Drees, J; Eigen, G; Feindt, M; Fernandez, J; Ferro, F; Gandelman, M; Gazis, E; Goncalves, P; Guy, J; Hallgren, A; Hamacher, K; Hauler, F; Herr, H; Houlden, A; Johansson, D; Jungermann, L; Katsoufis, E; Kerzel, U; Kokkinias, P; Krumstein, Z; Lemonne, J; Lesiak, T; Lopez, M; Lutz, P; MacNaughton, J; Malek, A; Marechal, B; Markou, A; Matorras, F; Mazzucato, M; Meroni, C; Moreno, S; Morettini, P; Mulders, M; Murray, W; Myklebust, T; Osterberg, K; Oyanguren, A; Parzefall, U; Perepelitsa, V; Piedra, J; Pieri, L; Pimenta, M; Podobnik, T; Pol, E; Rames, J; Rehn, J; Reinhardt, R; Romero, A; Roudeau, P; Strauss, J; Taffard, C; Timmermans, J; Tonazzo, A; Trochimczuk, M; Turluer, ML; Tzamarias, S; Uvarov, V; Valenti, G; Van Dam, P; van Remortel, N; Vegni, G; Veloso, F; Verzi, V; Vilanova, D; Yushchenko, O; Zalewska, A; Zimin, I

    European physical journal. C, Particles and fields, 01/2006, Letnik: 45, Številka: 1
    Journal Article

    Moments of the hadronic invariant mass and of the lepton energy spectra in semileptonic B decays have been determined with the data recorded by the DELPHI detector at LEP. From measurements of the inclusive b-hadron semileptonic decays, and imposing constraints from other measurements on b- and c-quark masses, the first three moments of the lepton energy distribution and of the hadronic mass distribution, have been used to determine parameters which enter into the extraction of |Vcb| from the measurement of the inclusive b-hadron semileptonic decay width. The values obtained in the kinetic scheme are:\(\begin{array}{*{20}l}{{m_{b} {\left( {1\;{\text{GeV}}} \right)}} \hfill} & { = \hfill} & {{4.591 \pm 0.062 \pm 0.039 \pm 0.005\;{\text{GeV/c}}^{2} ,} \hfill} \\{{m_{c} {\left( {1\;{\text{GeV}}} \right)}} \hfill} & { = \hfill} & {{1.170 \pm 0.093 \pm 0.055 \pm 0.005\;{\text{GeV/c}}^{{\text{2}}} {\text{,}}} \hfill} \\{{\mu ^{2}_{\pi } {\left( {1\;{\text{GeV}}} \right)}} \hfill} & { = \hfill} & {{0.399 \pm 0.048 \pm 0.034 \pm 0.087\;{\text{GeV}}^{{\text{2}}} {\text{,}}} \hfill} \\{{ \ifmmode\expandafter\tilde\else\expandafter\~\fi{\rho }^{3}_{D} } \hfill} & { = \hfill} & {{0.053 \pm 0.017 \pm 0.011 \pm 0.026\;{\text{GeV}}^{{\text{3}}} ,} \hfill} \\\end{array} \)and include corrections at order 1/mb3. Using these results, and present measurements of the inclusive semileptonic decay partial width of b-hadrons at LEP, an accurate determination of |Vcb| is obtained: \({\left| {V_{{cb}} } \right|} = 0.0421 \times {\left( {1 \pm 0.014_{{{\text{meas}}{\text{.}}} \pm 0.014_{{{\text{fit}}} \pm 0.015_{{{\text{th}}{\text{.}}} } \right)}\)