Abstract

We discuss the exclusive radiative decays BKγB\to K^{*}\gamma, BργB \to\rho\gamma, and BωγB\to\omega\gamma in QCD factorization within the Standard Model. The analysis is based on the heavy-quark limit of QCD. Our results for these decays are complete to next-to-leading order in QCD and to leading order in the heavy-quark limit. Special emphasis is placed on constraining the CKM-unitarity triangle from these observables. We propose a theoretically clean method to determine CKM parameters from the ratio of the BρlνB\to\rho l\nu decay spectrum to the branching fraction of BργB\to\rho\gamma. The method is based on the cancellation of soft hadronic form factors in the large energy limit, which occurs in a suitable region of phase space. The ratio of the BργB\to\rho\gamma and BKγB\to K^{*}\gamma branching fractions determines the side RtR_{t} of the standard unitarity triangle with reduced hadronic uncertainties. The recent Babar bound on B(B0ρ0γ)B(B^0\to\rho^0\gamma) implies Rt<0.81(ξ/1.3)R_t < 0.81 (\xi/1.3), with the limiting uncertainty coming only from the SU(3) breaking form factor ratio ξ\xi. This constraint is already getting competitive with the constraint from BsB_{s}-Bˉs\bar B_{s} mixing. Phenomenological implications from isospin-breaking effects are briefly discussed.Comment: 23 pages, 8 figure

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    Last time updated on 04/12/2019