$K\to(ππ)_{I=2}$ decays and twisted boundary conditions

$K\toππ$ Decays with Domain Wall Fermions: Lattice Matrix Elements

$K\toππ$ from electroweak penguins in $N_f=2$ domain-wall QCD

$K\toππ$ matrix elements beyond the leading-order chiral expansion

$K^{+}\toπ^{+}π^{0}$ Decay Amplitude in Quenched Lattice QCD

$K^{+}\toπ^{+}π^{0}$ Decay Amplitude with the Wilson Quark Action in Quenched Lattice QCD

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

$m_c/m_s$ with Brillouin fermions

$N_f = 2+1+1$ flavours of twisted mass quarks: cut-off effects at tree-level of perturbation theory

$O(a)$ Improvement for Quenched Wilson Fermions

$O(a)$ Improvement of Nucleon Matrix Elements

$O(aα_s)$ matching coefficients for the $ΔB$=2 operators in the lattice static theory

$O(α_{s}a)$ matching coefficients for axial vector current and $ΔB$$=$2 operator

$q\bar q$ and $2q2\bar q$ systems in terms of P-vortices

$Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$

$SU(2)$ gauge theory in the maximally abelian gauge without monopoles

$Z_6$ symmetry, electroweak transition, and magnetic monopoles at high temperature

$α_S$ from Lattice QCD: progresses and perspectives for a realistic full-QCD determination of the running Strong coupling

$γN \to Δ$ transition form factors in Quenched and $N_F=2$ QCD

$ΔI = 3/2$ kaon weak matrix elements with non-zero total momentum