Evidence for the decay $Ω_{c}^{0} \to Ï^+Ω(2012)^- \to Ï^+ (\bar{K}Î)^{-}$
arXiv:2106.00892 · doi:10.1103/PhysRevD.104.052005
Abstract
Using a data sample of 980~fb$^{-1}$ collected with the Belle detector operating at the KEKB asymmetric-energy $e^+e^-$ collider, we present evidence for the $Ω(2012)^-$ in the resonant substructure of $Ω_{c}^{0} \to Ï^+ (\bar{K}Î)^{-}$ ($(\bar{K}Î)^{-}$ = $K^-Î^0$ + $\bar{K}^0 Î^-$) decays. The significance of the $Ω(2012)^-$ signal is 4.2$Ï$ after considering the systematic uncertainties. The ratio of the branching fraction of $Ω_{c}^{0} \to Ï^{+} Ω(2012)^- \to Ï^+ (\bar{K}Î)^{-}$ relative to that of $Ω_{c}^{0} \to Ï^{+} Ω^-$ is calculated to be 0.220 $\pm$ 0.059(stat.) $\pm$ 0.035(syst.). The individual ratios of the branching fractions of the two isospin modes are also determined, and found to be ${\cal B}(Ω_{c}^0 \to Ï^+ Ω(2012)^-) \times {\cal B}(Ω(2012)^- \to K^-Î^0)/{\cal B}(Ω_{c}^0 \to Ï^+ K^- Î^0)$ = (9.6 $\pm$ 3.2(stat.) $\pm$ 1.8(syst.))\% and ${\cal B}(Ω_{c}^0 \to Ï^+ Ω(2012)^-) \times {\cal B}(Ω(2012)^- \to \bar{K}^0 Î^-)/{\cal B}(Ω_{c}^0 \to Ï^+ \bar{K}^0 Î^-)$ = (5.5 $\pm$ 2.8(stat.) $\pm$ 0.7(syst.))\%.
9 pages, 4 figures