Abstract
We report preliminary measurements of the branching fractions of the decays τ−→ K−nπ0 ντ (n = 0, 1, 2, 3) and τ−→ π−nπ0ντ (n = 3, 4), excluding the contributions that proceed through the decay of intermediate K0 and η mesons. The measurements are based on a data sample of 435 million τ pairs produced in e+e− collisions at and near the γ(4S) peak and collected with the BABAR detector in 1999–2008. The measured branching fractions are B(τ−→ K− ντ) = (7.174±0.033±0.213)×10−3, B(τ−→ K−π0ντ) = (5.054± 0.021 ± 0.148) × 10−3, B(τ−→ K−2π0ντ) = (6.151 ± 0.117 ± 0.338) × 10−4, B(τ−→ K−3π0ντ) = (1.246 ± 0.164 ± 0.238) × 10−4, B(τ−→ π−3π0ντ) = (1.168 ±0.006 ±0.038) ×10−2, B(τ−→ π−4π0ντ) = (9.020 ±0.400 ±0.652) × 10−4, where the ?rst uncertainty is statistical and the second one systematic.
Highlights
The branching fractions of the τ lepton into strange and non-strange final states, respectively B(τ → Xsν) and B(τ → Xdν), can be used to determine the Cabibbo-Kobayashi-Maskawa (CKM) quark mixing matrix element |Vus| [? ? ]
10.58 GeV, recorded by the BABAR detector [? ] at the PEP-II asymmetric-energy storage rings operated at the SLAC National Accelerator Laboratory
For the simulation of the particle identification (PID) efficiencies, we use the BABAR PID efficiencies measurements in all cases except for the efficiencies to identify a pion as a pion, a kaon as a kaon and a pion as a kaon
Summary
The branching fractions of the τ lepton into strange and non-strange final states, respectively B(τ → Xsν) and B(τ → Xdν), can be used to determine the Cabibbo-Kobayashi-Maskawa (CKM) quark mixing matrix element |Vus| [? ? ]. ] is more than 3σ lower than the value that is obtained from the the |Vud| and |Vub| measurements with the assumption that the CKM matrix is unitary [? The experimental uncertainty of this |Vus| determination is dominated by the uncertainties on the τ branching fractions into states with an odd number of kaons, which are summed to obtain B(τ → Xsν) [? All measurements exclude the decays that proceed through KS0 → 2π0 or η → 3π0 to the above final states. These measurements significantly improve some of the least precise experimental inputs that are involved in the above mentioned |Vus| determination
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.