${{\mathit \Lambda}}$ BARYONS($\mathit S$ = $-1$, $\mathit I$ = 0) ${{\mathit \Lambda}^{0}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$ ${\mathit {\mathit s}}$ INSPIRE search

#### ${{\boldsymbol \Lambda}{(2350)}}$

$I(J^P)$ = $0(9/2^{+})$
DAUM 1968 favors $\mathit J{}^{P} = 7/2{}^{-}$ or ${}^{}9/2{}^{+}$. BRICMAN 1970 favors ${}^{}9/2{}^{+}$. LASINSKI 1971 suggests three states in this region using a Pomeron + resonances model. There are now also three formation experiments from the College de France-Saclay group, DEBELLEFON 1977 , BACCARI 1977 , and DEBELLEFON 1978 , which find ${}^{}9/2{}^{+}$ in energy-dependent partial-wave analyses of ${{\overline{\mathit K}}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit \pi}}$ , ${{\mathit \Lambda}}{{\mathit \omega}}$ , and ${{\mathit N}}{{\overline{\mathit K}}}$ .
 ${{\mathit \Lambda}{(2350)}}$ MASS $2340\text{ to }2370\text{ }(\approx2350)$ MeV
 ${{\mathit \Lambda}{(2350)}}$ WIDTH $100\text{ to }250\text{ }(\approx150)$ MeV
 $\Gamma_{1}$ ${{\mathit N}}{{\overline{\mathit K}}}$ $\sim{}12\%$ 915
 $\Gamma_{2}$ ${{\mathit \Sigma}}{{\mathit \pi}}$ $\sim{}10\%$ 867
 $\Gamma_{3}$ ${{\mathit \Lambda}}{{\mathit \omega}}$ 686
 FOOTNOTES