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 ${{\mathit K}}{{\mathit \pi}}$   $1425.6 \pm1.5$ MeV (S = 1.1)
NEUTRAL ONLY   $1432.4 \pm1.3$ MeV 
${{\boldsymbol K}_{{2}}^{*}{(1430)}}$ WIDTH
CHARGED ONLY, WITH FINAL STATE ${{\mathit K}}{{\mathit \pi}}$   $98.5 \pm2.7$ MeV (S = 1.1)
NEUTRAL ONLY   $109 \pm5$ MeV (S = 1.9)
$\Gamma_{1}$ ${{\mathit K}}{{\mathit \pi}}$ $(49.9\pm{1.2})\%$S=1.0 619
$\Gamma_{2}$ ${{\mathit K}^{*}{(892)}}{{\mathit \pi}}$ $(24.7\pm{1.5})\%$S=1.0 419
$\Gamma_{3}$ ${{\mathit K}^{*}{(892)}}{{\mathit \pi}}{{\mathit \pi}}$ $(13.4\pm{2.2})\%$S=1.0 372
$\Gamma_{4}$ ${{\mathit K}}{{\mathit \rho}}$ $(8.7\pm{0.8})\%$S=1.2 318
$\Gamma_{5}$ ${{\mathit K}}{{\mathit \omega}}$ $(2.9\pm{0.8})\%$S=1.0 311
$\Gamma_{6}$ ${{\mathit K}^{+}}{{\mathit \gamma}}$ $(2.4\pm{0.5})\times 10^{-3}$S=1.1 627
$\Gamma_{7}$ ${{\mathit K}}{{\mathit \eta}}$ $(1.5^{+3.4}_{-1.0})\times 10^{-3}$S=1.3 486
$\Gamma_{8}$ ${{\mathit K}}{{\mathit \omega}}{{\mathit \pi}}$ $<7.2\times 10^{-4}$CL=95%100
$\Gamma_{9}$ ${{\mathit K}^{0}}{{\mathit \gamma}}$ $<9\times 10^{-4}$626
    constrained fit information