${{\boldsymbol K}_S^0}$ FORM FACTORS

For discussion, see note on ${{\mathit K}}_{{{\mathit \ell}}3}$ form factors in the ${{\mathit K}^{\pm}}$ section of the Particle Listings above. Because the semileptonic branching fraction is smaller in ${{\mathit K}_S^0}$ than ${{\mathit K}_L^0}$ by the ratio of the mean lives, the ${{\mathit K}_S^0}$ semileptonic form factor has so far been measured only in the ${{\mathit K}_{{{e3}}}}$ mode using the linear expansion $\mathit f_{+}(\mathit t$) = $\mathit f_{+}$(0) (1 + $\lambda _{+}\mathit t$ $/{{\mathit m}^{2}}_{{{\mathit \pi}^{+}}}$), which gives the vector form factor ${{\mathit f}_{{+}}}({{\mathit t}}$) relative to its value at ${{\mathit t}}$ = 0.

$\lambda _{+}$ (LINEAR ENERGY DEPENDENCE OF $\boldsymbol f_{+}$ IN ${{\boldsymbol K}_{{e3}}^{0}}$ DECAY) INSPIRE search

VALUE ($ 10^{-2} $) EVTS DOCUMENT ID TECN
$3.39$ $\pm0.41$ 15k
AMBROSINO
2006E
KLOE
  References:
AMBROSINO 2006E
PL B636 173 Study of the Branching Ratio and Charge Asymmetry for the Decay ${{\mathit K}_S^0}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit e}}{{\mathit \nu}}$ with the KLOE Detector