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

# ${{\boldsymbol K}_{{2}}^{*}{(1430)}}$ $I(J^P)$ = $1/2(2^{+})$

We consider that phase-shift analyses provide more reliable determinations of the mass and width.
${{\boldsymbol K}_{{2}}^{*}{(1430)}}$ MASS
 CHARGED ONLY, WITH FINAL STATE ${{\mathit K}}{{\mathit \pi}}$ $1427.3 \pm1.5$ MeV (S = 1.3)
 NEUTRAL ONLY $1432.4 \pm1.3$ MeV
${{\boldsymbol K}_{{2}}^{*}{(1430)}}$ WIDTH
 CHARGED ONLY, WITH FINAL STATE ${{\mathit K}}{{\mathit \pi}}$ $100.0 \pm2.1$ MeV
 NEUTRAL ONLY $109 \pm5$ MeV (S = 1.9)
 constrained fit information