Measurements of the branching fractions of the decays B0s→D∓sK± and B0s→D−sπ+
The decay mode \( B_s^0 \to D_s^{ \mp }{K^{\pm }} \) allows for one of the theoretically cleanest measurements of the CKM angle γ through the study of time-dependent CP violation. This paper reports a measurement of its branching fraction relative to the Cabibbo-favoured mode \( B_s^0 \to D_s^{ - }{...
| Autores: | , , , , , , , , , , , , , , , , , , , , |
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| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2012 |
| País: | España |
| Institución: | Universidad de Barcelona |
| Repositorio: | Dipòsit Digital de la UB |
| OAI Identifier: | oai:diposit.ub.edu:2445/57955 |
| Acceso en línea: | https://hdl.handle.net/2445/57955 |
| Access Level: | acceso abierto |
| Palabra clave: | Hadrons Teoria quàntica de camps Gravitació Relativitat (Física) Teoria quàntica Quantum field theory Gravitation Relativity (Physics) Quantum theory |
| Sumario: | The decay mode \( B_s^0 \to D_s^{ \mp }{K^{\pm }} \) allows for one of the theoretically cleanest measurements of the CKM angle γ through the study of time-dependent CP violation. This paper reports a measurement of its branching fraction relative to the Cabibbo-favoured mode \( B_s^0 \to D_s^{ - }{\pi^{ + }} \) based on a data sample corresponding to 0.37 fb−1 of proton-proton collisions at \( \sqrt {s} = 7\;{\text{TeV}} \) collected in 2011 with the LHCb detector. In addition, the ratio of B meson production fractions f s /f d , determined from semileptonic decays, together with the known branching fraction of the control channel B 0 → D −π+, is used to perform an absolute measurement of the branching fractions: $ \begin{gathered} \mathcal{B}\left( {B_s^0 \to D_s^{ - }{\pi^{ + }}} \right) = \left( {2.95\pm 0.05\pm 0.17_{{ - 0.22}}^{{ + 0.18}}} \right) \times {10^{{ - 3}}}, \hfill \\ \mathcal{B}\left( {B_s^0 \to D_s^{ \mp }{K^{\pm }}} \right) = \left( {1.90\pm 0.12\pm 0.13_{{ - 0.14}}^{{ + 0.12}}} \right) \times {10^{{ - 4}}}, \hfill \\ \end{gathered} $ where the first uncertainty is statistical, the second the experimental systematic uncertainty, and the third the uncertainty due to f s /f d . |
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