Study of the lepton flavor-violating Z′→τμZ'\toτμ decay

preprint2012arXivOpen access

Abstract

The lepton flavor violating Z′→τμZ^{\prime}\toτμ decay is studied in the context of several extended models that predict the existence of the new gauge boson named Z′Z^\prime. A calculation of the strength of the lepton flavor violating Z′μτZ^\primeμτ coupling is presented by using the most general renormalizable Lagrangian that includes lepton flavor violation. We used the experimental value of the muon magnetic dipole moment to bound this coupling, from which the Re(ΩLμτΩRμτ∗)\mathrm{Re}(Ω_{Lμτ}Ω^\ast_{Rμτ}) parameter is constrained and it is found that Re(ΩLμτΩRμτ∗)∼10−2\mathrm{Re}(Ω_{Lμτ}Ω^\ast_{Rμτ})\sim 10^{-2} for a Z′Z^\prime boson mass of 2 TeV. Alongside, we employed the experimental restrictions over the τ→μγτ\toμγ and τ→μμ+μ−τ\toμμ^+μ^- processes in the context of several models that predict the existence of the Z′Z^\prime gauge boson to bound the mentioned coupling. The most restrictive bounds come from the calculation of the three-body decay. For this case, it was found that the most restrictive result is provided by a vector-like coupling, denoted as ∣Ωμτ∣2|Ω_{μτ}|^2, for the ZχZ_χ case, finding around 10−210^{-2} for a Z′Z^\prime boson mass of 2 TeV. We used this information to estimate the branching ratio for the Z′→τμZ^\prime\toτμ decay. According to the analyzed models the least optimistic result is provided by the Sequential ZZ model, which is of the order of 10−210^{-2} for a Z′Z^\prime boson mass around 2 TeV.

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