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   JSON PDGID:
B102

${{\mathit \Lambda}_{{{c}}}{(2625)}^{+}}$

$I(J^P)$ = $0(3/2^{-})$ 
The spin-parity has not been measured but is expected to be ${}^{}3/2{}^{-}$: this is presumably the charm counterpart of the strange ${{\mathit \Lambda}{(1520)}}$.
${{\mathit \Lambda}_{{{c}}}{(2625)}^{+}}$ MASS   $2628.00 \pm0.15$ MeV 
 
${{\mathit \Lambda}_{{{c}}}{(2625)}^{+}}–{{\mathit \Lambda}_{{{c}}}^{+}}$ MASS DIFFERENCE   $341.54 \pm0.05$ MeV 
 
${{\mathit \Lambda}_{{{c}}}{(2625)}^{+}}$ WIDTH   $<0.52$ MeV  CL=90.0%
 
${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}}{{\mathit \pi}}$ and its submode ${{\mathit \Sigma}{(2455)}}{{\mathit \pi}}$ are the only strong decays allowed to an excited ${{\mathit \Lambda}_{{{c}}}^{+}}$ having this mass.
$\Gamma_{1}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  [1] $(66.67)\%$ 184
 
$\Gamma_{2}$ ${{\mathit \Sigma}_{{{c}}}{(2455)}^{++}}{{\mathit \pi}^{-}}$   $(3.42\pm{0.27})\%$ 103
 
$\Gamma_{3}$ ${{\mathit \Sigma}_{{{c}}}{(2455)}^{0}}{{\mathit \pi}^{+}}$   $(3.46\pm{0.31})\%$ 103
 
$\Gamma_{4}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ 3-body   $large$ 184
 
$\Gamma_{5}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{0}}$  [2] $<60\%$ CL=90% 293
 
$\Gamma_{6}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \gamma}}$   $<35\%$ CL=90% 319
 
FOOTNOTES