Addendum to: Nature Physics https://doi.org/10.1038/s41567-021-01478-8. Published online 15 March 2022.

In a new analysis since the publication of the original article, the LHCb collaboration performs a simultaneous test of muon-electron universality using \({B}^{+}\to {K}^{+}{{\mathscr{l}}}^{-}{{\mathscr{l}}}^{+}\) and \({B}^{0}\to {K}^{* 0}{{\mathscr{l}}}^{-}{{\mathscr{l}}}^{+}\) (\({\mathscr{l}}=e,\mu\)) decays with data collected between 2011 and 2018, corresponding to an integrated luminosity of 9 fb−1(ref. 1). Further details are provided in ref. 2. The decay-rate ratios of muon to electron modes, \({R}_{K}\) and \({R}_{{K}^{* }}\), are measured in two \({q}^{2}\) regions, \(0.1 < {q}^{2} < 1.1\,{\rm{G}}e{V}^{2}/{c}^{4}\) (low-\({q}^{2}\)) and \(1.1 < {q}^{2} < 6.0\,{\rm{G}}e{V}^{2}/{c}^{4}\) (central-\({q}^{2}\)).

In ref. 1 the value of \({R}_{K}\) in the central-\({q}^{2}\) range is measured with the same data sample as in the initial Nature Physics publication, but different selection requirements and analysis procedures are used. The value obtained in ref. 1, \({R}_{K}({\mathrm{central}}-{q}^{2})=0.949_{-0.041}^{+0.042}({stat})_{-0.022}^{+0.022}({syst})\), differs from the originally published result in Nature Physics. The new analysis finds that a component of the shift can be attributed to statistical effects (with a Gaussian distribution width of 0.033, as evaluated through pseudoexperiments). The main differences come from the reduction of misidentified hadronic backgrounds to the electron-decay mode due to a tighter electron particle identification working point (shift of 0.064) and the modelling of the remaining residual contribution (shift of 0.038). The new \({R}_{K}\) central-\({q}^{2}\) value is compatible with the Standard Model prediction1 and supersedes the result originally published. The numerical results initially presented in this paper should not be used as input for any meta analysis.