Abstract
Two issues have been identified in the measurement of the differential branching fraction of B^{0}→K^{*}(892)^{0}µ^{+}µ^{} decays presented in ref. [1]. Both of these issues involve the calculation of the ratio of efficiencies between the decay(Formula presented.)(normalisation mode) and the decay B^{0}→K^{*}(892)^{0}µ^{+}µ^{} (signal mode), denoted as R_{ϵ} in eq. (7.1) of ref. [1]. What follows is a brief description of the nature of these problems, followed by the corrected results.
Original language  English (US) 

Article number  142 
Journal  Journal of High Energy Physics 
Volume  2017 
Issue number  4 
DOIs 

State  Published  Apr 1 2017 
ASJC Scopus subject areas
 Nuclear and High Energy Physics
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The Lhcb Collaboration (2017). Erratum to: Measurements of the Swave fraction in B 0 → K + π − μ + μ − decays and the B 0 → K ∗(892)0 μ + μ − differential branching fraction (Journal of High Energy Physics, (2016), 2016, 11, (47), 10.1007/JHEP11(2016)047). Journal of High Energy Physics, 2017(4), [142]. https://doi.org/10.1007/JHEP04(2017)142