Revisiting the one leptoquark solution to the R(D(∗))R(D^{(\ast)}) anomalies and its phenomenological implications

preprint2016arXivOpen access

Abstract

It has been shown recently that the anomalies observed in Bˉ→D(∗)τνˉτ\bar B\to D^{(\ast)}τ\barν_τ and Bˉ→Kˉℓ+ℓ−\bar B\to \bar K\ell^+\ell^- decays could be resolved with just one scalar leptoquark. Fitting to the current data on R(D(∗))R(D^{(\ast)}) along with acceptable q2q^2 distributions in Bˉ→D(∗)τνˉτ\bar B\to D^{(\ast)}τ\barν_τ decays, four best-fit solutions for the operator coefficients have been found. In this paper, we explore the possibilities of how to discriminate these four solutions. Firstly, we find that two of them are already excluded by the decay Bc−→τ−νˉτB_c^-\to τ^-\barν_τ, because the predicted decay widths have already overshot the total width ΓBcΓ_{B_c}. It is then found that the remaining two solutions result in two effective Hamiltonians governing b→cτνˉτb\to c τ\barν_τ transition, which differ by a sign and enhance the absolute value of the coefficient of cˉLγμbL τˉLγμντL\bar c_Lγ_μb_L\,\bar τ_Lγ^μ{ν_τ}_L operator by about 12%12\%. However, they give nearly the same predictions as in the SM for the D∗D^\ast and ττ longitudinal polarizations as well as the lepton forward-backward asymmetries in Bˉ→D(∗)τνˉτ\bar B\to D^{(\ast)}τ\barν_τ decays. For the other observables like B(Bc−→τ−νˉτ)\mathcal B(B_c^-\to τ^-\barν_τ), B(Bc−→γτ−νˉτ)\mathcal B(B_c^- \to γτ^-\barν_τ), RD(∗)(q2)R_{D^{(\ast)}}(q^2), dB(Bˉ→D(∗)τνˉτ)/dq2{\rm d}\mathcal B(\bar B\to D^{(\ast)}τ\barν_τ)/{\rm d}q^2 and B(Bˉ→Xcτνˉτ)\mathcal B(\bar B\to X_cτ\barν_τ), on the other hand, the two solutions give sizable enhancements relative to the SM predictions. With measurement of Bc−→τ−νˉτB_c^-\to τ^-\barν_τ at LHCb and refined measurements of observables in Bˉ→D(∗)τνˉτ\bar B\to D^{(\ast)}τ\barν_τ at both LHCb and Belle-II, such a specific NP scenario could be further deciphered.

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