The BaBar measurements of the ratios R(D ( * ) ) = B(B→D ( * ) τντ ) B(B→D ( * ) µνµ) deviate from the standard model expectation, while new results on the purely leptonic B → τντ mode show a better consistency with the standard model, within the uncertainties. In a new physics scenario, one possibility to accomodate these two experimental facts consists in considering an additional tensor operator in the effective weak hamiltonian. We study the effects of such an operator in a set of observables, in semileptonic B → D ( * ) modes as well as in semileptonic B and Bs decays to excited positive parity charmed mesons.
Recent LHCb measurements show small discrepancies with respect to the Standard Model (SM) predictions in selected angular distributions of the mode B 0 → K Ã0 μ þ μ − . The possibility of explaining such tensions within theories beyond the SM crucially depends on the size of the deviations of the Wilson coefficients of the effective Hamiltonian for this mode, in comparison to their SM values. We analyze this issue in the framework of the Randall-Sundrum model with custodial protection (RS c ); in our study we also consider the mode with τ leptons in the final state. We discuss the small deviations of RS c results from SM ones, found scanning the parameter space of the model.
We study the radiative B → Kη ( ) γ decays, which are important to investigate CP violation, and are also relevant to assess the role of the exclusive modes induced by the b → sγ transition to saturate the inclusive B → Xsγ decay rate. Moreover, these channels do not display the same hierarchy as B → Kη ( ) modes, for which the decay into η is enhanced with respect to one into η. The threebody radiative decays reverse the role: we find that this experimentally observed behavior (although affected by a large uncertainty in the case of the η ) is reproduced in the theoretical analysis. We compute a B * → K form factor, needed for this study, using light cone QCD sum rules, and discuss a relation expected to hold in the large energy limit for the light meson. Finally, we examine B → Kηγ in two extensions of the standard model with universal extra dimensions, to investigate the sensitivity of this rare mode to such a kind of new physics effects.
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