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  • Measurements of the branchi...
    Aaij, R.; de Bonis, I.; Decamp, D.; Ghez, Ph; Hopchev, P.; Lees, J.-P.; Machikhiliyan, I.V.; Minard, M.-N.; Pietrzyk, B.; t'Jampens, S.; Tisserand, V.; Tournefier, E.; Ajaltouni, Ziad Zj; Deschamps, O.; Henrard, Pierre; Jahjah-Hussein, Marwa; Lefèvre, R.; Li Gioi, L.; Monteil, S.; Niess, V.; Perret, Pascal; Roa Romero, Diego Alejandro; Sobczak, Krzysztof Grzegorz; Barsuk, S.; Callot, O.; He, J.; Jean-Marie, B.; Lefrançois, J.; Machefert, F.; Martin Sanchez, A.; Nicol, M.; Robbe, P.; Schune, M.-H.; Viaud, B.; Videau, I.; Adrover, C.; Aslanides, E.; Cogan, J.; Khanji, B.; Legac, R.; Leroy, O.; Mancinelli, G.; Maurice, E.; Perrin-Terrin, M.; Sapunov, M.; Serrano, J.; Tsaregorodtsev, A.

    The journal of high energy physics, 2012, Letnik: 6
    Journal Article

    The decay mode $\B^{0}_{s} \to D^{\mp}_{s} K^{\pm} $ allows for one of the theoretically cleanest measurements of the CKM angle $\gamma$ through the study of time-dependent $\ensuremath{CP}\xspace$ violation. This paper reports a measurement of its branching fraction relative to the Cabibbo-favoured mode $\B^{0}_{s} \to D^{-}_{s} \pi^{+}$ based on a data sample of 0.37 fb$^{-1}$ proton-proton collisions at $\sqrt{s} = 7$ TeV collected in 2011 with the LHCb detector. In addition, the ratio of $\ensuremath{\mathrm{B}}\xspace$ meson production fractions $\ensuremath{f_s/f_d}$, determined from semileptonic decays, together with the known branching fraction of the control channel $B^{0} \to D^{-} \pi^{+}$, is used to perform an absolute measurement of the branching fractions: $B (\B^0_s \to D^-_s \pi^+) \;= (2.95 \pm 0.05 \pm 0.17^{\,+\,0.18}_{\,-\,0.22}) \times 10^{-3}$, $B (\B^0_s \to D^\mp_s K^\pm) = (1.90 \pm 0.12 \pm 0.13^{\,+\,0.12}_{\,-\,0.14}) \times 10^{-4}\,$, where the first uncertainty is statistical, the second the experimental systematic uncertainty, and the third the uncertainty due to $f_s/f_d$.