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${\mathit m}_{{{\mathit B}_{{{J}}}{(5840)}^{+}}}–{\mathit m}_{{{\mathit B}^{*0}}}$

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M224DM2

VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT • • We do not use the following data for averages, fits, limits, etc. • • $565$ $\pm15$ $\pm14$ 7k 1 AAIJ 2015 AB LHCB ${{\mathit p}}{{\mathit p}}$ at 7, 8 TeV 1  AAIJ 2015AB reports $\lbrack{}{\mathit m}_{{{\mathit B}_{{{J}}}^{+}}}–{\mathit m}_{{{\mathit B}^{0}}}$] $−$ (${\mathit m}_{{{\mathit B}^{*+}}}–{\mathit m}_{{{\mathit B}^{+}}}$) $−$ ${\mathit m}_{{{\mathit \pi}^{+}}}$ = $425$ $\pm15$ $\pm14$ MeV which we adjust by the ${{\mathit \pi}^{+}}$ mass. The masses inside the square brackets were measured for each candidate event. The result assumes $\mathit P$ = $−(-1){}^{J}$, (${\mathit m}_{{{\mathit B}^{*0}}}–{\mathit m}_{{{\mathit B}^{0}}}$) = (${\mathit m}_{{{\mathit B}^{*+}}}–{\mathit m}_{{{\mathit B}^{+}}}$) = $45.01$ $\pm0.30$ $\pm0.23$ MeV, and uses three relativistic Breit-Wigner functions in the fit for mass difference.

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