CorrelatedΛc+Λ¯c−production ine+e−annihilations ats∼10.5 GeV
Abstract
Using 13.6 ${\mathrm{fb}}^{\ensuremath{-}1}$ of continuum two-jet ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}c\overline{c}$ events collected with the CLEO detector, we have searched for baryon number correlations at the primary quark level. We have measured the likelihood for a ${\ensuremath{\Lambda}}_{c}^{+}$ charmed baryon to be produced in the hemisphere opposite a ${\overline{\ensuremath{\Lambda}}}_{c}^{\ensuremath{-}}$ relative to the likelihood for a ${\ensuremath{\Lambda}}_{c}^{+}$ charmed baryon to be produced opposite an anticharmed meson $\overline{D};$ in all cases, the reconstructed hadrons must have momentum greater than 2.3 $\mathrm{GeV}/c.$ We find that, given a ${\overline{\ensuremath{\Lambda}}}_{c}^{\ensuremath{-}}$ (reconstructed in five different decay modes), a ${\ensuremath{\Lambda}}_{c}^{+}$ is observed in the opposite hemisphere $(0.72\ifmmode\pm\else\textpm\fi{}0.11)%$ of the time (not corrected for efficiency). By contrast, given a $\overline{D}$ in one hemisphere, a ${\ensuremath{\Lambda}}_{c}^{+}$ is observed in the opposite hemisphere only $(0.21\ifmmode\pm\else\textpm\fi{}0.02)%$ of the time. Normalized to the total number of either ${\overline{\ensuremath{\Lambda}}}_{c}^{\ensuremath{-}}$ or $\overline{D}$ ``tags,'' it is therefore $3.52\ifmmode\pm\else\textpm\fi{}0.45\ifmmode\pm\else\textpm\fi{}0.42$ times more likely to find a ${\ensuremath{\Lambda}}_{c}^{+}$ opposite a ${\overline{\ensuremath{\Lambda}}}_{c}^{\ensuremath{-}}$ than a $\overline{D}$ meson. This enhancement is not observed in the JETSET 7.3 ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}c\overline{c}$ Monte Carlo simulation.
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