Abstract

We study the direct CP violation in the $\tau^\pm\rightarrow K^\pm \rho^0 (\omega)\nu_\tau \rightarrow K^\pm \pi^+\pi^-\nu_\tau$ decay process in the Standard Model. An interesting mechanism involving the charge symmetry violating mixing between $\rho^0$ and $\omega$ is applied to enlarge the CP asymmetry. With this mechanism, the maximum differential and localized integrated CP asymmetries can reach $-(5.6^{+2.9}_{-1.7})\times10^{-12}$ and $6.3^{+2.4}_{-3.3}\times 10^{-11}$, respectively, which still leave plenty room for CP-violating New Physics to be discovered through this process.

Highlights

  • C experiment ceased data collection in March 2008, the BESIII experiment began to collect data, and the luminosity reached 1032 cm−2 s−1 in 2013 [7]

  • In the framework of the standard model (SM), CP violation in the τ lepton decay process arises from a nontrivial phase in the Cabibbo– Kobayashi–Maskawa (CKM) matrix and is predicted to be zero in the leading order in G F

  • Delepine pointed out that the CP-odd phase can arise from the second-order weak process in the τ ± → K ±π 0ντ decay mode [22]

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Summary

Introduction

C experiment ceased data collection in March 2008, the BESIII experiment began to collect data, and the luminosity reached 1032 cm−2 s−1 in 2013 [7]. In the framework of the SM, the direct CP asymmetries come about due to a relative weak (CP-odd) and a relative strong (CP-even) phase This mechanism is forbidden in τ decays in the leading order of the Fermi coupling constant G F [21]. One can expect that there could be a bigger CP-violating asymmetry in the τ ± → K ±ρ0(ω)ντ → K ±π +π −ντ process It will be shown from our explicit calculations that ρ–ω mixing leads to an additional strong phase and enlarges the differential CP-violating asymmetry by a maximum of four orders of magnitude and the localized integrated CP asymmetry by a maximum of three orders of magnitude. It will be shown below that the CP-odd phase difference arises from the second-order weak processes and the CP-even phase difference is determined by the decay widths of intermediate resonances and ρ–ω mixing in the τ − → K ±ρ0(ω)ντ → K ±π +π −ντ decay mode

General formalism for CP asymmetry
Derivation details of matrix elements
Hadronic rest frame
Numerical results
Models for form factors and meson wave functions
Numerical results for the CP asymmetries
Conclusion
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