Abstract

We investigate the possibility of searching the lepton-flavor-violating (LFV) $\tau\rightarrow \mu\gamma$ rare decay at the Super Charm-Tau Factory (CTF). By comparing the kinematic distributions of the LFV signal and the standard model (SM) background, we develop an optimized event selection criteria which can significantly reduce the background events. It is concluded that new $2 \sigma$ upper limit of about $1.9 \times 10^{-9}$ on $Br(\tau \rightarrow \mu \gamma)$ can be obtained at the CTF, which is beyond the capability of Super-B factory in searching $\tau$ lepton rare decay. Within the framework of the scalar leptoquark model, a joint constraint on $\lambda_1 \lambda_2$ and $M_{LQ}$ can be derived from the upper bound on $Br(\tau \rightarrow \mu \gamma)$. With $1000~ fb^{-1}$ data expected at the CTF, we get $\lambda_1\lambda_2 < 7.2 \times 10^{-2}~(M_{LQ} = 800~ {\rm GeV})$ and $M_{LQ} > 900~{\rm GeV}~(\lambda_1 \lambda_2 = 9 \times 10^{-2})$ at $95\%$ confidence level (C.L.).

Highlights

  • In this paper, we investigate the potential of searching the τ → μγ LFV decay at the Charm-Tau Factory (CTF) and demonstrate its better chance than the Super-B factory

  • Compared to the Super-B factory, τ leptons can be copiously produced in pairs at the CTF with center-of-mass (c.m.s.) energies Ee+e− not far above the 2mτ threshold, and the radiative background e+e− → τ +τ −γ is not significant

  • We investigate the potential of searching τ → μγ LFV decay at the CTF

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Summary

Introduction

We investigate the potential of searching the τ → μγ LFV decay at the CTF and demonstrate its better chance than the Super-B factory. The paper is organized as follows: The LFV signal and dominant background at the CTF are discussed. A strategy of experimental event selection to improve signal significance is developed, and an. J. C (2016) 76:421 expected upper limit on Br(τ → μγ ) is presented. The constraints on the leptoquark model parameters are given as an example of an interpretation of new physics

LFV signal and background at the CTF
Results and discussion
Constraints on new physics
Summary
Full Text
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