STRANGE MESONS ($\mathit S$ = $\pm1$, $\mathit C$ = $\mathit B$ = $\mathit{0}$)

${{\mathit K}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit s}}}$, ${{\mathit K}^{0}}$ = ${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit s}}}$, ${{\overline{\mathit K}}^{0}}$ = ${\mathit {\overline{\mathit d}}}$ ${\mathit {\mathit s}}$, ${{\mathit K}^{-}}$ = ${\mathit {\overline{\mathit u}}}$ ${\mathit {\mathit s}}$, similarly for ${{\mathit K}^{*}}$'s
Charged Kaon Mass
Rare Kaon Decays
Dalitz Plot Parameters for ${{\mathit K}}$ $\rightarrow$ 3 ${{\mathit \pi}}$ Decays
$\mathit CPT$ 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
Scalar Mesons below 1 GeV
${{\mathit K}^{*}{(892)}}$ 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 ${{\mathit K}_{{0}}^{*}{(800)}}$ 		$1/2(0^{+})$  
• ${{\mathit K}^{*}{(892)}}$
$1/2(1^{-})$  
• ${{\mathit K}_{{1}}{(1270)}}$
$1/2(1^{+})$  
• ${{\mathit K}_{{1}}{(1400)}}$
$1/2(1^{+})$  
• ${{\mathit K}^{*}{(1410)}}$
$1/2(1^{-})$  
• ${{\mathit K}_{{0}}^{*}{(1430)}}$
$1/2(0^{+})$  
• ${{\mathit K}_{{2}}^{*}{(1430)}}$
$1/2(2^{+})$  
• ${{\mathit K}{(1460)}}$
$1/2(0^{-})$  
${{\mathit K}_{{2}}{(1580)}}$
$1/2(2^{-})$  
${{\mathit K}{(1630)}}$
$1/2(?^{?})$  
• ${{\mathit K}_{{1}}{(1650)}}$
$1/2(1^{+})$  
• ${{\mathit K}^{*}{(1680)}}$
$1/2(1^{-})$  
• ${{\mathit K}_{{2}}{(1770)}}$
$1/2(2^{-})$  
• ${{\mathit K}_{{3}}^{*}{(1780)}}$
$1/2(3^{-})$  
• ${{\mathit K}_{{2}}{(1820)}}$
$1/2(2^{-})$  
${{\mathit K}{(1830)}}$
$1/2(0^{-})$  
${{\mathit K}_{{0}}^{*}{(1950)}}$
$1/2(0^{+})$  
• ${{\mathit K}_{{2}}^{*}{(1980)}}$
$1/2(2^{+})$  
• ${{\mathit K}_{{4}}^{*}{(2045)}}$
$1/2(4^{+})$  
${{\mathit K}_{{2}}{(2250)}}$
$1/2(2^{-})$  
${{\mathit K}_{{3}}{(2320)}}$
$1/2(3^{+})$  
${{\mathit K}_{{5}}^{*}{(2380)}}$
$1/2(5^{-})$  
${{\mathit K}_{{4}}{(2500)}}$
$1/2(4^{-})$  
${{\mathit K}{(3100)}}$
aka ${{\mathit K}_{{J}}^{?}{(3100)}}$ 		$?^?(?^{? ?})$  
 
•   Indicates established particles.