In this talk, I first motivate the use of Chiral Perturbation Theory in the context of Lattice QCD. In particular, I explain how partially quenched QCD, which has, in general, unequal valence- and sea-quark masses, can be used to obtain real-world (i.e. unquenched) results for low-energy constants. In the second part, I review how Chiral Perturbation Theory may be used to overcome theoretical difficulties which afflict the computation of non-leptonic kaon decay rates from Lattice QCD. I argue that it should be possible to determine at least the O(p^2) weak low-energy constants reliably from numerical computations of the K to pi and K to vacuum matrix elements of the corresponding weak operators
We present the inconsistencies which arise in quenched QCD in AI = 1/2 non-leptonic kaon decays usin...
AbstractWe use one-loop SU(2)L×SU(2)R chiral perturbation theory (SU(2) ChPT) to study the behaviour...
Recently, we pointed out that chiral transformation properties of strong penguin operators change in...
The coupling constants of the order p^2 low-energy weak effective lagrangian can be determined from ...
These lectures describe the use of effective field theories to extrapolate results from the paramete...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose cou...
I discuss the progress in the use of analytic techniques for low energy QCD, in particular as applie...
Quantum chromodynamics (QCD) is the fundamental theory that describes the interaction of quarks and ...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
It has been proposed that partially quenched chiral perturbation theory can be used together with pa...
Recent developments in lattice QCD calculation of weak matrix elements involving light quarks are de...
Computing hadronic observables by solving QCD from first principles with realistic quark masses is a...
This talks contains a short introduction to Chiral Perturbation Theory and the existing calculations...
We present the inconsistencies which arise in quenched QCD in AI = 1/2 non-leptonic kaon decays usin...
AbstractWe use one-loop SU(2)L×SU(2)R chiral perturbation theory (SU(2) ChPT) to study the behaviour...
Recently, we pointed out that chiral transformation properties of strong penguin operators change in...
The coupling constants of the order p^2 low-energy weak effective lagrangian can be determined from ...
These lectures describe the use of effective field theories to extrapolate results from the paramete...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose cou...
I discuss the progress in the use of analytic techniques for low energy QCD, in particular as applie...
Quantum chromodynamics (QCD) is the fundamental theory that describes the interaction of quarks and ...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
It has been proposed that partially quenched chiral perturbation theory can be used together with pa...
Recent developments in lattice QCD calculation of weak matrix elements involving light quarks are de...
Computing hadronic observables by solving QCD from first principles with realistic quark masses is a...
This talks contains a short introduction to Chiral Perturbation Theory and the existing calculations...
We present the inconsistencies which arise in quenched QCD in AI = 1/2 non-leptonic kaon decays usin...
AbstractWe use one-loop SU(2)L×SU(2)R chiral perturbation theory (SU(2) ChPT) to study the behaviour...
Recently, we pointed out that chiral transformation properties of strong penguin operators change in...