$K^{+}\toπ^{+}π^{0}$ decays at next-to-leading order in the chiral expansion on finite volumes

$K^{\ast}(892)^0$ and $\bar{K}^{\ast}(892)^0$ production in central Pb+Pb, Si+Si, C+C and inelastic p+p collisions at 158$A$~GeV

$K^{\star}(892)^{0}$ Production in Relativistic Heavy Ion Collisions at $\sqrt{s_{_{NN}}}=130$ GeV

$K_0$ of purely infinite simple regular rings

$K_1$ of separative exchange rings and C*-algebras with real rank zero

$K_L \ra μ^\pm e^\mp ν\overlineν$ as background to $K_L \ra μ^\pm e^\mp$

$K_L \to γν> \barν$ decay beyond the standard model

$K_L \to π^0 e^+ e^-$ and $B \to X_s \ell^+ \ell^-$ Decay in the MSSM

$K_L \to π^0 ν\bar ν$ Beyond the Standard Model

$K_L \to π^0 ν\barν$ in Little Higgs model

$K_L \to π^o ν\barν$ in the Aspon Model

$K_L \to π^o ν\overlineν$ in Extended Higgs Models

$K_L\toγν\barν$ in the Light Front Model

$K_s^0 Hadronization Following DIS at CLAS

$k_T$ and threshold resummations

$k_T$ factorization of exclusive $B$ meson decays

$k_T$ factorization of exclusive processes

$K_{e5}$ Decays in Chiral Perturbation Theory

$K_{L e5}$ decay as a background in search for $K_{L} \to π^{0} μ^{\pm} e^{\mp}$

$K_{l3}$ prospects from NA48/2