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
Summary
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.
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