Abstract
The LHCb Collaboration reported anomalies in B→K^{*}μ^{+}μ^{-}, B_{s}→ϕμ^{+}μ^{-}, and R(K)=B→Kμ^{+}μ^{-}/B→Ke^{+}e^{-}. Furthermore, BABAR, BELLE, and LHCb Collaborations found hints for the violation of lepton-flavor universality violation in R(D^{(*)})=B→D^{(*)}τν/B→D^{(*)}ℓν. In this Letter we reexamine these decays and their correlations to B→K^{(*)}νν[over ¯] using gauge invariant dim-6 operators. For the numerical analysis we focus on scenarios in which new physics couples, in the interaction eigenbasis, to third generation quarks and lepton only. We conclude that such a setup can explain the b→sμ^{+}μ^{-} data simultaneously with R(D^{(*)}) for small mixing angles in the lepton sector (of the order of π/16) and very small mixing angles in the quark sector (smaller than V_{cb}). In these regions of parameter space, B→K^{(*)}τμ and B_{s}→τμ can be order 10^{-6}. Possible UV completions are briefly discussed.
Highlights
Effective Field Theory Approach to b → sllð0Þ, B → KðÃÞννand B → DðÃÞτν with Third Generation Couplings
For the numerical analysis we focus on scenarios in which new physics couples, in the interaction eigenbasis, to third generation quarks and lepton only
We conclude that such a setup can explain the b → sμþμ− data simultaneously with RðDðÃÞÞ for small mixing angles in the lepton sector and very small mixing angles in the quark sector
Summary
[56,57,58,59,60,61,62] It has been claimed than a simultaneous explanation of RðKÞ, RðDÞ, and RðDÃÞ using gauge invariant operators with left-handed fermions is possible [58,61]. For this purpose, it was assumed that in the interaction eigenbasis only couplings to the third generation exist [51,58] (or are enhanced by m2τ =m2μ compared to the second one [61]), while all other couplings are generated by the misalignment between the mass and the interaction basis (or are suppressed by small lepton-mass ratios [61]). Flavor observables: b → sμþμ− transitions.—b → slilj transitions are defined via the effective Hamiltonian
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