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

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

Neither of $\mathit J$ or ${}^{P}$ has actually been measured. Nor have any absolute branching fractions been measured.
${{\mathit \Xi}_{{c}}^{+}}$ MASS   $2467.94 {}^{+0.17}_{-0.20}$ MeV 
${{\mathit \Xi}_{{c}}^{+}}$ MEAN LIFE   $(4.56 \pm0.05) \times 10^{-13}$ s 
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.