Abstract

The branching fractions of the rare weak $B\to \pi l^+l^-(\nu\bar\nu)$ and $B\to\rho l^+l^-(\nu\bar\nu)$ decays are calculated in the framework of the relativistic quark model based on the quasipotential approach. The form factors parametrizing weak decay matrix elements are explicitly determined in the whole kinematical $q^2$ range without additional assumptions and extrapolations. Relativistic effects are systematically taken into account including recoil effects in meson wave functions and contributions of the intermediate negative-energy states. New experimental data on the differential distributions in the semileptonic heavy-to-light $B\to\pi l\nu_l$ and $B\to\rho l\nu_l$ decays are analyzed in detail. Good agreement of the predictions and data is found. The obtained results for the branching fractions of the rare semileptonic decays are found to be in agreement with other theoretical estimates and recent experimental data available for the $B^+\to\pi^+ \mu^+\mu^-$ decay.

Highlights

  • Br (B+ → π +μ+μ−) = (2.3 ± 0.6 ± 0.1) × 10−8

  • The form factors parametrizing weak decay matrix elements are explicitly determined in the whole kinematical q2 range without additional assumptions and extrapolations

  • In this paper we use the relativistic quark model based on the quasipotential approach and QCD for the calculation of the form factors of weak B decays to final π or ρ mesons

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Summary

Introduction

[12] we calculated the form factors parametrizing matrix elements of the weak vector and axial vector currents for the B → π and B → ρ transitions and on this basis studied the corresponding semileptonic decays B → π(ρ)lνl . In this paper we use the relativistic quark model based on the quasipotential approach and QCD for the calculation of the form factors of weak B decays to final π or ρ mesons.

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