Physics – High Energy Physics – High Energy Physics - Experiment
Scientific paper
2010-03-16
Physics
High Energy Physics
High Energy Physics - Experiment
submitted to Phys. Rev. D (Rapid Communications)
Scientific paper
The branching fraction for the decay $D^+_s\to\tau^{+}\nu_{\tau}$, with $\tau^{+}\to e^{+} \nu_{e}\bar{\nu}_{\tau}$, is measured using a data sample corresponding to an integrated luminosity of 427 fb^{-1} collected at center of mass energies near 10.58 GeV with the \slshape B\kern-0.1em{\smaller A}\kern-0.1em B\kern-0.1em{\smaller A\kern-0.2em R} detector at the PEP-II asymmetric-energy $e^{+}e^{-}$ collider at SLAC. In the process $e^{+}e^{-}\to c\bar c\to D^{*+}_s \kern 0.2em\bar{\kern -0.2em D}{}_{\mathrm{TAG}} \kern 0.2em\bar{\kern -0.2em K}{} X$, the $D^{*+}_s$ meson is reconstructed as a missing particle, and the subsequent decay $D^{*+}_s\to D^+_s\gamma$ yields an inclusive $D^+_s$ data sample. Here $_{\mathrm{TAG}}$ refers to a fully reconstructed hadronic $\kern 0.2em\bar{\kern -0.2em D}{}$ decay, $\kern 0.2em\bar{\kern -0.2em K}{}$ is a $K^-$ or $\kern 0.2em\bar{\kern -0.2em K}{}^0$, and $X$ stands for any number of charged or neutral pions. The decay $D^+_s\to K^0_{\scriptscriptstyle S} K^{+}$ is isolated also, and from ratio of event yields and known branching fractions, ${\cal B} (D^+_s\to\tau^{+}\nu_{\tau})$ = (4.5\pm0.5\pm0.4\pm0.3% is determined. The pseudoscalar decay constant is extracted to be $f_{D_s}$ = (233\pm13\pm10\pm7) MeV, where the first uncertainty is statistical, the second is systematic, and the third results from the uncertainties on the external measurements used as input to the calculation.
"The BABAR Collaboration
Lee Jong-Phil
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