Abstract

We study the long-distance contribution to ${B}_{s}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ decay, which is generated by the two-photon intermediate state via the ${B}_{s}\ensuremath{\rightarrow}{\ensuremath{\gamma}}^{*}{\ensuremath{\gamma}}^{*}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ transition. It is found that the dispersive two-photon amplitude can interfere with the dominant short-distance amplitude, which gives rise to new theoretical uncertainty in the branching ratio of ${B}_{s}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$. Our analysis shows that, by taking into account present experimental constraints, this uncertainty could be up to the same order of magnitude as some theoretical uncertainties of $\mathcal{B}({B}_{s}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}})$ given in the past literature. Future precise studies of the double radiative ${B}_{s}\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma}$ decay, both experimentally and theoretically, may help to reduce the uncertainty. This novel effect has never been examined in ${B}_{s}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ decay.

Highlights

  • Rare leptonic B-meson decays Bq → lþl− with q 1⁄4 d, s and l 1⁄4 e, μ, τ, which are helicity suppressed in the standard model (SM), could offer powerful tools to probe new physics scenarios beyond the SM

  • Using the same numerical inputs for C10 and jVÃtbVtsj as in Ref. [7], together with our estimate of ReI, we find that the dispersive long-distance two-photon transition may give rise to the theoretical uncertainty of the branching ratio of Bs → μþμ− decay, which could be up to

  • The decay rate is dominated by the short-distance contribution in the SM, which has been calculated very precisely

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Summary

INTRODUCTION

Rare leptonic B-meson decays Bq → lþl− with q 1⁄4 d, s and l 1⁄4 e, μ, τ, which are helicity suppressed in the standard model (SM), could offer powerful tools to probe new physics scenarios beyond the SM. BðBs → μþμ−Þ 1⁄4 ð3.0 Æ 0.6þ−00..23Þ × 10−9; ð1Þ and the current world average by the Particle Data Group [5] is These measurements are in agreement with present SM predictions given in Refs. It is thought that the SM contributions to the Bq → lþl− decay can be described by an effective theory after integrating the heavy particles including the top quark, the Higgs boson, and weak gauge bosons W and Z. It is seen that the decay is characterized by a purely leptonic final state, its nonperturbative strong interaction effects are confined to the matrix element h0jqγμγ5bjBqðpÞi 1⁄4 ifBq pμ: ð4Þ. The rare Bq → lþl− decay could be theoretically quite clean, which is well suited for precision flavor physics.

Published by the American Physical Society
ΓðBs γγÞ
Re I
Findings
DISCUSSION AND SUMMARY
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