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

# ${{\boldsymbol \Sigma}{(3170)}}$ Bumps $I(J^P)$ = $1(?^{?})$

Seen by AMIRZADEH 1979 as a narrow 6.5-standard-deviation enhancement in the reaction ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Y}^{*+}}{{\mathit \pi}^{-}}$ using data from independent high statistics bubble chamber experiments at 8.25 and 6.5 ${\mathrm {GeV/}}\mathit c$. The dominant decay modes are multibody, multistrange final states and the production is via isospin-${}^{}3/2{}^{}$ baryon exchange. Isospin ${}^{}1{}^{}$ is favored. Not seen in a ${{\mathit K}^{-}}{{\mathit p}}$ experiment in LASS at 11 ${\mathrm {GeV/}}\mathit c$ (ASTON 1985B).
 ${{\mathit \Sigma}{(3170)}}$ MASS (PRODUCTION EXPERIMENTS) $\approx3170$ MeV
 ${{\mathit \Sigma}{(3170)}}$ WIDTH (PRODUCTION EXPERIMENTS)
 $\Gamma_{1}$ ${{\mathit \Lambda}}{{\mathit K}}{{\overline{\mathit K}}}$ seen
 $\Gamma_{2}$ ${{\mathit \Sigma}}{{\mathit K}}{{\overline{\mathit K}}}$ seen
 $\Gamma_{3}$ ${{\mathit \Xi}}{{\mathit K}}$ seen