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
See related reviews:
Charged Kaon Mass
Rare Kaon Decays
Dalitz Plot Parameters for ${{\mathit K}}$ $\rightarrow$ 3 ${{\mathit \pi}}$ Decays
${{\mathit K}}{}^{\pm}_{{{\mathit \ell}}3}$ and ${{\mathit K}}{}^{0}_{{{\mathit \ell}}3}$ Form Factors
$\mathit CPT$ Invariance Tests in Neutral Kaon Decay
$\mathit CP$ Violation in ${{\mathit K}_S^0}$ $\rightarrow$ 3 ${{\mathit \pi}}$
$\mathit V_{{\mathit {\mathit u}}{\mathit {\mathit d}}}$, $\mathit V_{{\mathit {\mathit u}}{\mathit {\mathit s}}}$ the Cabibbo Angle, and CKM Unitarity
$\mathit CP$ Violation in ${{\mathit K}_L^0}$ Decays
$\Delta \mathit S$ = $\Delta \mathit Q$ in ${{\mathit K}^{0}}$ Decays
${{\mathit K}^{*}{(892)}}$ Masses and Mass Differences
${{\mathit K}^{\pm}}$
$1/2(0^{-})$
${{\mathit K}^{0}}$
$1/2(0^{-})$
${{\mathit K}_S^0}$
$1/2(0^{-})$
${{\mathit K}_L^0}$
$1/2(0^{-})$
${{\mathit K}_{{0}}^{*}{(700)}}$
aka ${{\mathit \kappa}}$; was ${{\mathit K}_{{0}}^{*}{(800)}}$
$1/2(0^{+})$
${{\mathit K}^{*}{(892)}}$
$1/2(1^{-})$
${{\mathit K}_{{1}}{(1270)}}$
$1/2(1^{+})$
${{\mathit K}_{{1}}{(1400)}}$
$1/2(1^{+})$
${{\mathit K}^{*}{(1410)}}$
$1/2(1^{-})$
${{\mathit K}_{{0}}^{*}{(1430)}}$
$1/2(0^{+})$
${{\mathit K}_{{2}}^{*}{(1430)}}$
$1/2(2^{+})$
${{\mathit K}{(1460)}}$
$1/2(0^{-})$
${{\mathit K}_{{2}}{(1580)}}$
$1/2(2^{-})$
${{\mathit K}{(1630)}}$
$1/2(?^{?})$
${{\mathit K}_{{1}}{(1650)}}$
$1/2(1^{+})$
${{\mathit K}^{*}{(1680)}}$
$1/2(1^{-})$
${{\mathit K}_{{2}}{(1770)}}$
$1/2(2^{-})$
${{\mathit K}_{{3}}^{*}{(1780)}}$
$1/2(3^{-})$
${{\mathit K}_{{2}}{(1820)}}$
$1/2(2^{-})$
${{\mathit K}{(1830)}}$
$1/2(0^{-})$
${{\mathit K}_{{0}}^{*}{(1950)}}$
$1/2(0^{+})$
${{\mathit K}_{{2}}^{*}{(1980)}}$
$1/2(2^{+})$
${{\mathit K}_{{4}}^{*}{(2045)}}$
$1/2(4^{+})$
${{\mathit K}_{{2}}{(2250)}}$
$1/2(2^{-})$
${{\mathit K}_{{3}}{(2320)}}$
$1/2(3^{+})$
${{\mathit K}_{{5}}^{*}{(2380)}}$
$1/2(5^{-})$
${{\mathit K}_{{4}}{(2500)}}$
$1/2(4^{-})$
${{\mathit K}{(3100)}}$
$?^?(?^{? ?})$
 
   Indicates established particles.