Abstract

LHCb has reported deviations from the Standard Model in b→sμ+μ−b\to sμ^+μ^- transitions for which a new neutral gauge boson is a prime candidate for an explanation. As this gauge boson has to couple in a flavour non-universal way to muons and electrons in order to explain RKR_K, it is interesting to examine the possibility that also lepton flavour is violated, especially in the light of the CMS excess in h→τ±μ∓h\toτ^\pmμ^\mp. In this article, we investigate the perspectives to discover the lepton-flavour violating modes B→K(∗)τ±μ∓B\to K^{(*)}τ^\pmμ^\mp, Bs→τ±μ∓B_s\to τ^\pmμ^\mp and B→K(∗)μ±e∓B\to K^{(*)} μ^\pm e^\mp, Bs→μ±e∓B_s\to μ^\pm e^\mp. For this purpose we consider a simplified model in which new-physics effects originate from an additional neutral gauge boson (Z′Z^\prime) with generic couplings to quarks and leptons. The constraints from τ→3μτ\to3μ, τ→μννˉτ\toμν\barν, μ→eγμ\to eγ, gμ−2g_μ-2, semi-leptonic b→sμ+μ−b\to sμ^+μ^- decays, B→K(∗)ννB\to K^{(*)}νν and BsB_s--B‾s\overline{B}_s mixing are examined. From these decays, we determine upper bounds on the decay rates of lepton flavour violating BB decays. Br(B→Kνν)Br(B\to Kνν) limits the branching ratios of LFV BB decays to be smaller than 8×10−5(2×10−5)8\times 10^{-5} (2\times 10^{-5}) for vectorial (left-handed) lepton couplings. However, much stronger bounds can be obtained by a combined analysis of BsB_s--B‾s\overline{B}_s, τ→3μτ\to3μ, τ→μννˉτ\toμν\barν and other rare decays. The bounds depend on the amount of fine-tuning among the contributions to BsB_s--B‾s\overline{B}_s mixing. Allowing for a fine-tuning at the percent level we find upper bounds of the order of 10−610^{-6} for branching ratios into τμτμ final states, while Bs→μ±e∓B_s\to μ^\pm e^\mp is strongly suppressed and only B→K(∗)μ±e∓B\to K^{(*)} μ^\pm e^\mp can be experimentally accessible (with a branching ratio of order 10−710^{-7}).

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