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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%

${{\mathit \Lambda}_{{{c}}}{(2625)}^{+}}$ DECAY MODES
${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}}{{\mathit \pi}}$ and its submode ${{\mathit \Sigma}{(2455)}}{{\mathit \pi}}$ are the only strong decays allowed to an excited ${{\mathit \Lambda}_{{{c}}}^{+}}$ having this mass.
Mode   Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/ Conf. Level P(MeV/c)   $\Gamma_{1}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ [1] ($50$ $\pm7$ ) $\%$ 184   $\Gamma_{2}$ ${{\mathit \Sigma}_{{{c}}}{(2455)}^{++}}{{\mathit \pi}^{-}}$ ($2.6$ $\pm0.4$ ) $\%$ 103   $\Gamma_{3}$ ${{\mathit \Sigma}_{{{c}}}{(2455)}^{0}}{{\mathit \pi}^{+}}$ ($2.6$ $\pm0.4$ ) $\%$ 103   $\Gamma_{4}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ 3-body large 184   $\Gamma_{5}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{0}}$ [2] <50 $\%$ CL=90% 293   $\Gamma_{6}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \gamma}}$ <26 $\%$ CL=90% 319

[1] In the isospin limit, this braching fraction would be 2/3, the other 1/3 being decays to ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$. [2] A test that the isospin is indeed 0, so that the particle is indeed a ${{\mathit \Lambda}_{{{c}}}^{+}}$.