CHARMED BARYONS
($\mathit C$ = $+1$)
${{\mathit \Lambda}_{{{c}}}^{+}}$ = ${{\mathit u}}{{\mathit d}}{{\mathit c}}$, ${{\mathit \Sigma}_{{{c}}}^{++}}$ = ${{\mathit u}}{{\mathit u}}{{\mathit c}}$, ${{\mathit \Sigma}_{{{c}}}^{+}}$ = ${{\mathit u}}{{\mathit d}}{{\mathit c}}$, ${{\mathit \Sigma}_{{{c}}}^{0}}$ = ${{\mathit d}}{{\mathit d}}{{\mathit c}}$,
${{\mathit \Xi}_{{{c}}}^{+}}$ = ${{\mathit u}}{{\mathit s}}{{\mathit c}}$, ${{\mathit \Xi}_{{{c}}}^{0}}$ = ${{\mathit d}}{{\mathit s}}{{\mathit c}}$, ${{\mathit \Omega}_{{{c}}}^{0}}$ = ${{\mathit s}}{{\mathit s}}{{\mathit c}}$		 INSPIRE search

${{\mathit \Xi}_{{{c}}}^{+}}$ $I(J^P)$ = $1/2(1/2^{+})$ 

Neither of $\mathit J$ or ${}^{P}$ has actually been measured.
${{\mathit \Xi}_{{{c}}}^{+}}$ MASS   $2467.79 \pm0.15$ MeV (S = 1.1)
${{\mathit \Xi}_{{{c}}}^{+}}$ MEAN LIFE   $(4.53 \pm0.05) \times 10^{-13}$ s 
${{\mathit \Xi}_{{{c}}}^{+}}$, ${{\overline{\mathit \Xi}}_{{{c}}}^{-}}$ $\mathit CP$-VIOLATING DECAY ASYMMETRIES
$\mathit A_{CP}({{\mathit \Sigma}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$) in ${{\mathit \Xi}_{{{c}}}^{+}}$ $\rightarrow$ ${{\mathit \Sigma}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$, ${{\overline{\mathit \Xi}}_{{{c}}}^{-}}$ $\rightarrow$ ${{\overline{\mathit \Sigma}}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$   $0.10 \pm0.07$  
$\mathit A_{CP}({{\mathit \Sigma}^{+}}{{\mathit K}^{+}}{{\mathit K}^{-}}$) in ${{\mathit \Xi}_{{{c}}}^{+}}$ $\rightarrow$ ${{\mathit \Sigma}^{+}}{{\mathit K}^{+}}{{\mathit K}^{-}}$, ${{\overline{\mathit \Xi}}_{{{c}}}^{-}}$ $\rightarrow$ ${{\overline{\mathit \Sigma}}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$   $0.04 \pm0.07$  
Branching fractions marked with a footnote, e.g. [$\mathit a$], have been corrected for decay modes not observed in the experiments. For example, the submode fraction ${{\mathit \Xi}_{{{c}}}^{+}}$ $\rightarrow$ ${{\mathit \Sigma}^{+}}{{\overline{\mathit K}}^{*}{(892)}^{0}}$ seen in ${{\mathit \Xi}_{{{c}}}^{+}}$ $\rightarrow$ ${{\mathit \Sigma}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ has been multiplied up to include ${{\overline{\mathit K}}^{*}{(892)}^{0}}$ $\rightarrow$ ${{\overline{\mathit K}}^{0}}{{\mathit \pi}^{0}}$ decays.