The coupling constants of the order p^2 low-energy weak effective lagrangian can be determined from the K → π and K → 0 weak matrix elements, choosing degenerate quark masses for the first of these. However, for typical values of quark masses in Lattice QCD computations, next-to-leading O(p^4) corrections are too large to be ignored, and will need to be included in future analyses. Here we provide the complete O(p^4) expressions for these matrix elements obtained from Chiral Perturbation Theory, valid for partially quenched QCD with N degenerate sea quarks. Quenched QCD corresponds to the special case N = 0. We also discuss the role of the η' meson in some detail, and we give numerical examples of the size of chiral logarithms.
The transformation properties of strong penguin operators under the action of the flavor group chang...
We present the inconsistencies which arise in quenched QCD in AI = 1/2 non-leptonic kaon decays usin...
We properly define off-shell K → π transition amplitudes and use them to extract information for on-...
The coupling constants of the order p^2 low-energy weak effective lagrangian can be determined from ...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
Abstract: In the calculation of non-leptonic weak decay rates, a \mismatch " arises when the QC...
We explore the application of the domain wall fermion formalism of lattice QCD to calculate the K ⃗ ...
We calculate the logarithmic corrections to the matrix elements for K+ → π+ and K → vacuum (which ar...
We present the ingredients for determining K+ → π+π0 matrix elements via the combination of lattice ...
In this talk, I first motivate the use of Chiral Perturbation Theory in the context of Lattice QCD. ...
The large-N limit is used to obtain a consistent picture of the K → ππ matrix elements. It is confir...
We review lattice results relevant for pion and kaon physics with the aim of making them easily acce...
The transformation properties of strong penguin operators under the action of the flavor group chang...
We present the inconsistencies which arise in quenched QCD in AI = 1/2 non-leptonic kaon decays usin...
We properly define off-shell K → π transition amplitudes and use them to extract information for on-...
The coupling constants of the order p^2 low-energy weak effective lagrangian can be determined from ...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
Abstract: In the calculation of non-leptonic weak decay rates, a \mismatch " arises when the QC...
We explore the application of the domain wall fermion formalism of lattice QCD to calculate the K ⃗ ...
We calculate the logarithmic corrections to the matrix elements for K+ → π+ and K → vacuum (which ar...
We present the ingredients for determining K+ → π+π0 matrix elements via the combination of lattice ...
In this talk, I first motivate the use of Chiral Perturbation Theory in the context of Lattice QCD. ...
The large-N limit is used to obtain a consistent picture of the K → ππ matrix elements. It is confir...
We review lattice results relevant for pion and kaon physics with the aim of making them easily acce...
The transformation properties of strong penguin operators under the action of the flavor group chang...
We present the inconsistencies which arise in quenched QCD in AI = 1/2 non-leptonic kaon decays usin...
We properly define off-shell K → π transition amplitudes and use them to extract information for on-...