RPV SUSY effects in τ−→e−(μ−)KKˉτ^- \to e^-(μ^-) K\bar{K} Decays

preprint2014arXivOpen access

Abstract

In this paper, we investigate τ−→e−(μ−)KKˉ(KKˉ=K+K−,K0Kˉ0)τ^- \to e^-(μ^-) K\bar{K}(K\bar{K}=K ^+K^-,K^0\bar{K}^0) decays in the framework of the RPV SUSY model. We discuss the tree level contribution of the sparticles ν~\tildeν and u~\tilde{u} to these decay branching ratios. In the two channels, the ν~\tildeν-mediated channel is more sensitive to the parameter product ∣λi22′∗λi31(2)∣|λ^{'*}_{i22}λ_{i31(2)}| than the u~\tilde{u}-mediated channel to ∣λ1(2)j2′∗λ3j2′∣|λ^{'*}_{1(2)j2}λ'_{3j2}|. And the parameter product ∣λi22′∗λi31(2)∣|λ^{'*}_{i22}λ_{i31(2)}| is severely constrained to the order of O(10−5){\cal O}(10^{-5}) by the experiment data with mν~=100GeVm_{\tildeν}=100 GeV, which is one order of magnitude more stringent than before. In the calculation of hadronic matrix elements, the resonant effects are large than those of non-resonant terms. Especially, the resonant contribution of scalar meson f(980)f_{(980)} plays a dominate role in ν~\tildeν-mediated channel.

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