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Measurement of |V cb | using the semileptonic decay \(\overline{\rm {B^{0}_{d}}} \rightarrow {\rm D}^* \ell^- \overline{\nu}_{\ell}\)

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Abstract.

Data from Z decays in DELPHI have been searched for \(\overline{\rm B^0_d}\rightarrow {\rm D}^{* + } \ell^- \overline{\nu}_{\ell}\) with the \({\rm D}^{* + }\) decaying to \({\rm D}^0 \pi^ + \) and \({\rm D}^0 \rightarrow {\rm K}^- \pi^ + \), \({\rm K}^- \pi^ + \pi^ + \pi^-\) or \({\rm K}^- \pi^ + (\pi^0)\). These events are used to measure the CKM matrix element \(\left\vert{\rm V}_{cb} \right\vert\) and the form factor slope, \(\rho_{A_1}^2\): \({\cal F}_{D^*}(1) \left\vert{\rm V}_{cb} \right\vert = 0.0392 \pm 0.0018 \pm 0.0023; \rho_{A_1}^2 = 1.32 \pm 0.15 \pm 0.33 \) corresponding to a branching fraction: \({\rm BR}(\overline{\rm B^0_d}\rightarrow {\rm D}^{* + } \ell^- \overline{\nu}_{\ell}) = (5.90 \pm 0.22 \pm 0.50)\%. \) Combining these and previous DELPHI measurements gives: \( {\cal F}_{D^*}(1)\left|{\rm V}_{cb} \right|= 0.0377 \pm 0.0011 \pm 0.0019,\quad \rho_{A_1}^2 = 1.39 \pm 0.10 \pm 0.33\) and \({\rm BR}(\overline{\rm B^0_d}\rightarrow {\rm D}^{* + } \ell^- \overline{\nu}_{\ell}) = (5.39 \pm 0.11 \pm 0.34)\% \) Using \({\cal F}_{D^*}(1) = 0.91 \pm 0.04\), yields: \( \left|{\rm V}_{cb} \right|= 0.0414 \pm 0.0012\textrm{(stat.)} \pm 0.0021\textrm{(syst.)} \pm 0.0018\textrm{(theory)}. \) The b-quark semileptonic branching fraction into a \({\rm D}^{* + }\) emitted from higher mass charmed excited states has also been measured to be: \({\rm BR}(b \rightarrow {\rm D}^{* + } {\rm X} \ell^- \overline{\nu}_{\ell}) = (0.67\pm 0.08\pm0.10)\% \)

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Received: 24 September 2003, Revised: 15 December 2003, Published online: 4 February 2004

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The DELPHI Collaboration. Measurement of |V cb | using the semileptonic decay \(\overline{\rm {B^{0}_{d}}} \rightarrow {\rm D}^* \ell^- \overline{\nu}_{\ell}\) . Eur. Phys. J. C 33, 213–232 (2004). https://doi.org/10.1140/epjc/s2004-01598-6

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