A study of the B$^+$ $\to$ J$/\psi\overline{ \Lambda}$p decay using proton-proton collision data collected at $\sqrt{ s} =$ 8 TeV by the CMS experiment at the LHC, corresponding to an integrated luminosity of 19.6 fb$^{ -1}$, is presented. The ratio of branching fractions $\mathcal{ B}$(B$^+$ $\to$ J$/\psi\overline{ \Lambda}$p ) / $\mathcal{ B}$(B$^+$ $\to$ J$/\psi$K$^*$(892)$^+$) is measured to be (1.054 $\pm$ 0.057 (stat) $\pm$ 0.035 (syst) $\pm$ 0.011 ($\mathcal{ B}$))%, where the last uncertainty reflects the uncertainties in the world-average branching fractions of $\overline{ \Lambda}$ and K$^*$(892)$^+$ decays to reconstructed final states. The invariant mass distributions of the J$/\psi\overline{ \Lambda}$, J$/\psi$p, and $\overline{ \Lambda}$p systems produced in the B$^+$ $\to$ J$/\psi\overline{ \Lambda}$p decay are investigated and found to be inconsistent with the pure phase space hypothesis. The analysis is extended by using a model-independent angular amplitude analysis, which shows that the observed invariant mass distributions are consistent with the contributions from excited kaons decaying to the $\overline{ \Lambda}$p system.
Categories: hep-ex