Abstract

We revisit rare radiative leptonic decays ${B}_{s,d}\ensuremath{\rightarrow}\ensuremath{\gamma}{e}^{+}{e}^{\ensuremath{-}}$ and ${B}_{s,d}\ensuremath{\rightarrow}\ensuremath{\gamma}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ in the standard model and provide the updated estimates for various differential distributions (the branching ratios, the forward-backward asymmetry, and ${R}_{\ensuremath{\mu}/e}$, the ratio of the differential distribution for muons over electrons in the final state). The new ingredients of this work compared to the existing theoretical analyses are the following: (i) we calculate all ${B}_{d}\ensuremath{\rightarrow}\ensuremath{\gamma}$ and ${B}_{s}\ensuremath{\rightarrow}\ensuremath{\gamma}$ form factors induced by the vector, axial-vector, tensor and pseudotensor quark currents within the relativistic dispersion approach based on the constituent quark picture; (ii) we perform a detailed analysis of the charm-loop contributions to radiative leptonic decays: we obtain constraints imposed by electromagnetic gauge invariance and discuss the existing ambiguities in the charmonia contributions.

Highlights

  • Rare radiative leptonic Bðs;dÞ → γlþl− decays are one of the flavor-changing neutral current (FCNC) decays: at the quark level, they are induced by b → fs; dg quark transitions, which in the standard model (SM) are forbidden at tree level

  • The new ingredients of this work compared to the existing theoretical analyses are the following: (i) we calculate all Bd → γ and Bs → γ form factors induced by the vector, axial-vector, tensor and pseudotensor quark currents within the relativistic dispersion approach based on the constituent quark picture; (ii) we perform a detailed analysis of the charm-loop contributions to radiative leptonic decays: we obtain constraints imposed by electromagnetic gauge invariance and discuss the existing ambiguities in the charmonia contributions

  • The invariant form factors, which parameterize the corresponding amplitudes, depend on two variable k02 and k2, where k0 is the momentum emitted from the FCNC b → ðs; dÞ vertex, and k is the momentum of the virtual photon

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Summary

INTRODUCTION

Rare radiative leptonic Bðs;dÞ → γlþl− decays are one of the flavor-changing neutral current (FCNC) decays: at the quark level, they are induced by b → fs; dg quark transitions, which in the standard model (SM) are forbidden at tree level. Such transitions occur via penguin and box diagrams containing loops and lead to small branching ratios, of order 10−8–10−10 [1]. The C7γ part in Eq (2.2) emerges from the diagrams in Fig. 1(a,c) with the virtual photon emitted from the penguin

Ãts C7γ ðμÞ e 8π2 mb sσμνð1 þ γ5Þb
Direct emission of the real photon from valence quarks of the B meson
Direct emission of the virtual photon from valence quarks of the B meson
Bremsstrahlung
CONSTRAINTS ON THE TRANSITION FORM FACTORS
Form factors of the axial-vector weak current
Form factors of the tensor weak current
Form factors of the pseudotensor weak current
CHARM-LOOP CONTRIBUTIONS TO THE AMPLITUDE
Charming penguins
Factorizable part of the amplitude Hμα
Adding nonfactorizable corrections to the amplitude Hμα
V 20 15 10
Weak annihilation
F TV ðq2Þ
Parameters of the model
The differential distributions
The differential branching ratios
R e Bs '
Forward-backward asymmetry
Findings
CONCLUSIONS
Full Text
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