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Measurements of the branching fractions of the decays $ B_s^0 \to D_s^{ \mp }{K^{\pm }} $ and $ B_s^0 \to D_s^{ - }{\pi^{ + }} $
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Abstract
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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Title: Measurements of the branching fractions of the decays $ B_s^0 \to D_s^{ \mp }{K^{\pm }} $ and $ B_s^0 \to D_s^{ - }{\pi^{ + }} $
Description:
Abstract
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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