STRANGE MESONS
($\boldsymbol S$ = $\pm1$, $\boldsymbol C$ = $\boldsymbol B$ = 0)
${{\mathit K}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit s}}}$, ${{\mathit K}^{0}}$ = ${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit s}}}$, ${{\overline{\mathit K}}^{0}}$ = ${\mathit {\overline{\mathit d}}}$ ${\mathit {\mathit s}}$, ${{\mathit K}^{-}}$ = ${\mathit {\overline{\mathit u}}}$ ${\mathit {\mathit s}}$, similarly for ${{\mathit K}^{*}}$'s
INSPIRE search

${{\boldsymbol K}{(3100)}}$ $I^G(J^{PC})$ = $?^?(?^{? ?})$ 

Narrow peak observed in several ( ${{\mathit \Lambda}}{{\overline{\mathit p}}}$ + pions) and ( ${{\overline{\mathit \Lambda}}}{{\mathit p}}$ + pions) states in ${{\mathit \Sigma}^{-}}{}^{}\mathrm {Be}$ reactions by BOURQUIN 1986 and in ${{\mathit n}}{{\mathit p}}$ and ${{\mathit n}}$ A reactions by ALEEV 1993 . Not seen by BOEHNLEIN 1991 . If due to strong decays, this state has exotic quantum numbers ($\mathit B=0,\mathit Q=+1,\mathit S=-1$ for ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{+}}$ and $\mathit I$ ${}\geq{}$ 3$/$2 for ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{-}}$ ). Needs confirmation.
${{\boldsymbol K}{(3100)}}$ MASS
Mass $\mathit m$   $\approx3100$ MeV 
3-BODY DECAYS   $3054 \pm11$ MeV 
4-BODY DECAYS   $3059 \pm11$ MeV 
5-BODY DECAYS
${{\boldsymbol K}{(3100)}}$ WIDTH
3-BODY DECAYS
4-BODY DECAYS
5-BODY DECAYS
$\Gamma_{1}$ ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{+}}$ 
$\Gamma_{2}$ ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{-}}$ 
$\Gamma_{3}$ ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ 
$\Gamma_{4}$ ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{+}}$ 
$\Gamma_{5}$ ${{\mathit \Lambda}}{{\overline{\mathit p}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ 
$\Gamma_{6}$ ${{\mathit \Sigma}{(1385)}^{+}}{{\overline{\mathit p}}}$