Abstract

While the LHC did not observe direct evidence for physics beyond the standard model, indirect hints for new physics were uncovered in the flavour sector in the decays B→K∗μ+μ−B\to K^*μ^+μ^-, B→Kμ+μ−/B→Ke+e−B\to Kμ^+μ^-/B\to Ke^+e^-, Bs→ϕμ+μ−B_s\toϕμ^+μ^-, B→D(∗)τνB\to D^{(*)}τν and h→τ±μ∓h\toτ^\pmμ^\mp. Each observable deviates from the SM predictions at the 2−3 σ2-3\,σ level only, but combining all b→sμ+μ−b\to sμ^+μ^- data via a global fit, one finds 4−5 σ4-5\,σ difference for NP compared to the SM and combining B→D∗τνB\to D^{*}τν with B→DτνB\to Dτν one obtains 3.9 σ3.9\,σ. While B→D(∗)τνB\to D^{(*)}τν and h→τμh\toτμ can be naturally explained by an extended Higgs sector, the b→sμ+μ−b\to sμ^+μ^- anomalies point at a Z′Z' gauge boson. However, it is also possible to explain B→D(∗)τνB\to D^{(*)}τν and b→sμ+μ−b\to sμ^+μ^- simultaneously with leptoquarks while their effect in h→τ±μ∓h\toτ^\pmμ^\mp is far too small to account for current data. Combining a 2HDM with a gauged Lμ−LτL_μ-L_τ symmetry allows for explaining the b→sμ+μ−b\to sμ^+μ^- anomalies in combination with h→τ±μ∓h\toτ^\pmμ^\mp, predicting interesting correlations with τ→3μτ\to3μ. In the light of these deviations from the SM we also discuss the possibilities of observing lepton flavour violating BB decays (e.g. B→K(∗)τ±μ∓B\to K^{(*)}τ^\pmμ^\mp and Bs→τ±μ∓B_s\toτ^\pmμ^\mp).

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