Abstract

Recent LHCb results on R_{K^*}, the ratio of the branching fractions of B rightarrow K^* mu ^+ mu ^- to that of B rightarrow K^* e^+ e^-, for the dilepton invariant mass bins q^2 equiv m_{ell ell }^2 = [0.045–1.1] GeV^2 and [1.1–6] GeV^2 show approximately 2.5 sigma deviations from the corresponding Standard Model prediction in each of the bins. This, when combined with the measurement of R_K , (q^2=[1-6], mathrm GeV^2), a similar ratio for the decay to a pseudo-scalar meson, highly suggests lepton non-universal new physics in semi-leptonic B meson decays. In this work, we perform a model independent analysis of these potential new physics signals and identify the operators that do the best job in satisfying all these measurements. We show that heavy new physics, giving rise to q^2 independent local 4-Fermi operators of scalar, pseudo-scalar, vector or axial-vector type, is unable to explain all the three measurements simultaneously, in particular R_{K^*} in the bin [0.045–1.1], within their experimental 1sigma regions. We point out the possibility to explain R_{K^*} in the low bin by an additional light (lesssim , 20 , {mathrm{MeV}}) vector boson with appropriate coupling strengths to (bar{b} , s) and (bar{e} , e).

Highlights

  • While the result for RK was presented only in the dilepton invariant mass squared, q2 ∈ [1,2,3,4,5,6] GeV2, RK ∗ has been measured in two bins, [0.045–1.1] GeV2 and [1.1–6] GeV2

  • Since C7 and C9 always appear in particular combinations with other Ci≤6 in matrix elements, it is customary to define the following effective Wilson coefficients [58,59]: B( Bs

  • We would like to mention that we have explored the possibility of existence of a pair of new physics (NP) operators simultaneously with unrelated Wilson coefficients

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Summary

Introduction

The LHCb collaboration has recently reported hints of new physics (NP) in lepton flavor non-universal observables RK and RK ∗ ,. The decays B → K (∗)μ+μ− proceed via b → s flavor changing neutral current (FCNC) transitions. The individual branching ratios B B → K (∗)μ+μ− and B B → K (∗)e+e− are predicted with comparatively larger hadronic uncertainties in the SM Their ratio is a theoretically clean observable and predicted to be close to unity in the SM. This is in contrast to some of the angular observables (for example, P5) where considerable debate exists surrounding the issue of theoretical uncertainty due to (unknown) power corrections to the factorization framework and non-local charm loops; see for example [29,50,51,52,53,54,55,56,57]. As the tensor operators do not get generated at the dimension 6 level if the full SM gauge invariance is imposed [60,61], we ignore them in this work

Results
One Wilson coefficient at a time
Combination of Wilson coefficients
Summary
Full Text
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