STRANGE MESONS ($\mathit S$ = $\pm1$, $\mathit C$ = $\mathit B$ = 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
Reviews:
The Charged Kaon Mass
Rare Kaon Decays (rev.)
Dalitz Plot Parameters for ${{\mathit K}}$ $\rightarrow$ 3 ${{\mathit \pi}}$ Decays
${{\mathit K}}{}^{+-}_{{{\mathit \ell}}3}$ 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
${{\mathit K}^{\pm}}$
${{\mathit K}^{0}}$
${{\mathit K}_S^0}$
${{\mathit K}_L^0}$
${{\mathit K}_{{0}}^{*}{(800)}}~$or ${{\mathit \kappa}}$
${{\mathit K}^{*}{(892)}}$
${{\mathit K}_{{1}}{(1270)}}$
${{\mathit K}_{{1}}{(1400)}}$
${{\mathit K}^{*}{(1410)}}$
${{\mathit K}_{{0}}^{*}{(1430)}}$
${{\mathit K}_{{2}}^{*}{(1430)}}$
${{\mathit K}{(1460)}}$
${{\mathit K}_{{2}}{(1580)}}$
${{\mathit K}{(1630)}}$
${{\mathit K}_{{1}}{(1650)}}$
${{\mathit K}^{*}{(1680)}}$
${{\mathit K}_{{2}}{(1770)}}$
${{\mathit K}_{{3}}^{*}{(1780)}}$
${{\mathit K}_{{2}}{(1820)}}$
${{\mathit K}{(1830)}}$
${{\mathit K}_{{0}}^{*}{(1950)}}$
${{\mathit K}_{{2}}^{*}{(1980)}}$
${{\mathit K}_{{4}}^{*}{(2045)}}$
${{\mathit K}_{{2}}{(2250)}}$
${{\mathit K}_{{3}}{(2320)}}$
${{\mathit K}_{{5}}^{*}{(2380)}}$
${{\mathit K}_{{4}}{(2500)}}$
${{\mathit K}{(3100)}}$