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

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

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

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

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$m_c/m_s$ with Brillouin fermions

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

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$O(a)$ Improvement for Quenched Wilson Fermions

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$O(a)$ Improvement of Nucleon Matrix Elements

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

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

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

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

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

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

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

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

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

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$η'$-$η_c$-mixing with improved stochastic estimators

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$Λ(1405)$ from lattice QCD

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$Λ_{QCD}$ from gluon and ghost propagators

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