The large-N limit is used to obtain a consistent picture of the K → ππ matrix elements. It is confirmed that the dominant Q6 penguin matrix elements are enhanced by an order of magnitude compared to those of the current-current operators and that this result is consistent with chiral perturbation theory. An additional enhancement of the penguin contributions is identified with respect to standard estimates which comes from an incomplete GIM cancellation above the charm quark mass. Performing the short-distance analysis to first nontrivial order in 1/N its validity and simplicity is demonstrated. Encouraging results are obtained for A(K → ππ) amplitudes and it is pointed out that further improvements can be obtained through the inclusion of ...
The SU(3) chiral limit K → ππ matrix elements of the electroweak penguin operators, Q7,8, are determ...
Firstly, we use the recent ALEPH/OPAL data on the V-A spectral functions for fixing the continuum th...
I : Chiral Perturbation Theory is introduced and its applications to semileptonic and nonleptonic ka...
The large-N limit is used to obtain a consistent picture of the K → ππ matrix elements. It is confir...
We use the large-N limit to obtain a consistent picture of the K → ππ amplitudes, A(K → ππ). We emph...
The K → ππ system is analyzed in the chiral limit within the Standard Model. We discuss how to conne...
Recent work by J. Prades and myself on K → ππ is described. The first part describes our method to c...
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 ...
We extend in several respects our earlier work on O(p2) corrections to the matrix elements of the el...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
We discuss the matching between long-distance and short-distance at next-to-leading in 1/Nc and show...
We calculate the logarithmic corrections to the matrix elements for K+ → π+ and K → vacuum (which ar...
We study the scaling of kaon decay amplitudes with the number of colours, N, in a theory with four d...
Abstract: In the calculation of non-leptonic weak decay rates, a \mismatch " arises when the QC...
The SU(3) chiral limit K → ππ matrix elements of the electroweak penguin operators, Q7,8, are determ...
Firstly, we use the recent ALEPH/OPAL data on the V-A spectral functions for fixing the continuum th...
I : Chiral Perturbation Theory is introduced and its applications to semileptonic and nonleptonic ka...
The large-N limit is used to obtain a consistent picture of the K → ππ matrix elements. It is confir...
We use the large-N limit to obtain a consistent picture of the K → ππ amplitudes, A(K → ππ). We emph...
The K → ππ system is analyzed in the chiral limit within the Standard Model. We discuss how to conne...
Recent work by J. Prades and myself on K → ππ is described. The first part describes our method to c...
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 ...
We extend in several respects our earlier work on O(p2) corrections to the matrix elements of the el...
In the calculation of non-leptonic weak decay rates, a "mismatch" arises when the QCD evolution of t...
We discuss the matching between long-distance and short-distance at next-to-leading in 1/Nc and show...
We calculate the logarithmic corrections to the matrix elements for K+ → π+ and K → vacuum (which ar...
We study the scaling of kaon decay amplitudes with the number of colours, N, in a theory with four d...
Abstract: In the calculation of non-leptonic weak decay rates, a \mismatch " arises when the QC...
The SU(3) chiral limit K → ππ matrix elements of the electroweak penguin operators, Q7,8, are determ...
Firstly, we use the recent ALEPH/OPAL data on the V-A spectral functions for fixing the continuum th...
I : Chiral Perturbation Theory is introduced and its applications to semileptonic and nonleptonic ka...