Measurement of branching fractions of $Î_{c}^{+}$ decays to $Σ^{+} K^{+} K^{-}$, $Σ^{+}Ï$ and $Σ^{+} K^{+} Ï^{-}(Ï^{0})$
arXiv:2304.09405 · doi:10.1007/JHEP09(2023)125
Abstract
Based on 4.5 fb$^{-1}$ data taken at seven center-of-mass energies ranging from 4.600 to 4.699 GeV with the BESIII detector at the BEPCII collider, we measure the branching fractions of $Î_{c}^{+}\rightarrowΣ^{+}+hadrons$ relative to $Î_{c}^{+}\rightarrow Σ^+ Ï^+ Ï^-$. Combining with the world average branching fraction of $Î_{c}^{+}\rightarrow Σ^+ Ï^+ Ï^-$, their branching fractions are measured to be $(0.377\pm0.042\pm0.018\pm0.021)\%$ for $Î_{c}^{+}\rightarrowΣ^{+} K^{+} K^{-}$, $(0.200\pm0.023\pm0.010\pm0.011)\%$ for $Î_{c}^{+}\rightarrowΣ^{+} K^{+} Ï^{-}$, $(0.414\pm0.080\pm0.029\pm0.023)\%$ for $Î_{c}^{+}\rightarrowΣ^{+}Ï$ and $(0.197\pm0.036\pm0.008\pm0.011)\%$ for $Î_{c}^{+}\rightarrowΣ^{+}K^{+} K^{-}$(non-$Ï$). In all the above results, the first uncertainties are statistical, the second are systematic and the third are from external input of the branching fraction of $Î_{c}^{+}\rightarrow Σ^+ Ï^+ Ï^-$. Since no signal for $Î_{c}^{+}\rightarrowΣ^{+} K^{+} Ï^{-}Ï^{0}$ is observed, the upper limit of its branching fraction is determined to be 0.11\% at the 90$\%$ confidence level.