Abstract

The branching fraction of the rare B_{s}^{0}→ϕμ^{+}μ^{-} decay is measured using data collected by the LHCb experiment at center-of-mass energies of 7, 8, and 13TeV, corresponding to integrated luminosities of 1, 2, and 6 fb^{-1}, respectively. The branching fraction is reported in intervals of q^{2}, the square of the dimuon invariant mass. In the q^{2} region between 1.1 and 6.0 GeV^{2}/c^{4}, the measurement is found to lie 3.6 standard deviations below a standard model prediction based on a combination of light cone sum rule and lattice QCD calculations. In addition, the first observation of the rare B_{s}^{0}→f_{2}^{'}(1525)μ^{+}μ^{-} decay is reported with a statistical significance of 9 standard deviations and its branching fraction is determined.

Highlights

  • Background fromB0 → Kþπ−μþμ− and Λ0b → pK−μþμ− decays is found to be non-negligible in the wide mðKþK−Þ window

  • For the rare B0s → φμþμ− decay, a simultaneous extended maximum-likelihood fit of the data samples for the different periods is performed in intervals of q2, where the signal yields are parametrized using Eq (1) and the differential branching fraction is shared between the samples

  • The relative branching fraction measurement is affected by systematic uncertainties on the fit model and the efficiency ratio, where the latter is determined using standard model (SM)

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Summary

Introduction

Background fromB0 → Kþπ−μþμ− and Λ0b → pK−μþμ− decays is found to be non-negligible in the wide mðKþK−Þ window. The yields of the normalization mode for the different data-taking periods are determined using extended unbinned maximum-likelihood fits to the mðKþK−μþμ−Þ distribution. The yields of the normalization mode NJ=ψφ are determined to be 62980 Æ 270, 70970 Æ 290, and 148490 Æ 410 for the three different data-taking periods, where the uncertainties are statistical only.

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