We calculate the one-loop contributions to the difference \Delta_{\pi K} between the isoscalar on-shell pion-kaon scattering amplitude at the Cheng-Dashen point and the scalar form factor \Gamma_K (2M_\pi^2) in the framework of three flavor chiral perturbation theory. These corrections turn out to be small. This is further sharpened by treating the kaons as heavy fields (two flavor chiral perturbation theory). We also analyze the two-loop corrections to the kaon scalar form factor based on a dispersive technique. We find that these corrections are smaller than in the comparable case of the scalar form factor of the pion. This is related to the weaker final state interactions in the pion-kaon channel
The pion mass dependence of the nucleon mass within the covariant SU(2) baryon chiral perturbation t...
We derive a simplified representation for the pion mass to two loops in three-flavour chiral perturb...
We develop a unitarity approach to consider the final state interaction corrections to the tree leve...
We calculate the one-loop contributions to the difference Delta(piK) between the isoscalar on-shell ...
We calculate the vector and scalar form factors of the pion to two loops in Chiral Perturbation Theo...
First it is shown that the tree amplitude for pion pion scattering in the minimal linear sigma model...
First it is shown that the tree amplitude for pion–pion scattering in the minimal linear sigma mode...
First it is shown that the tree amplitude for pion pion scattering in the minimal linear sigma model...
An earlier calculation in a generalized linear sigma model showed that the well-known current algebr...
I review recent progress made in the description of pion-nucleon scattering, the $\sigma$--term, the...
The weak decay of the kaon to two pions is studied within the model of Nambu and Jona-Lasinio. Using...
The five different K -> 3 Pi and the three K -> 2 Pi decays are calculated in Chiral Perturbation Th...
The five different K -> 3 Pi and the three K -> 2 Pi decays are calculated in Chiral Perturbation Th...
We quantify the important effect of strong final state interactions id the weak K --> 2 pi amplitude...
We quantify the important effect of strong final state interactions id the weak K --> 2 pi amplitude...
The pion mass dependence of the nucleon mass within the covariant SU(2) baryon chiral perturbation t...
We derive a simplified representation for the pion mass to two loops in three-flavour chiral perturb...
We develop a unitarity approach to consider the final state interaction corrections to the tree leve...
We calculate the one-loop contributions to the difference Delta(piK) between the isoscalar on-shell ...
We calculate the vector and scalar form factors of the pion to two loops in Chiral Perturbation Theo...
First it is shown that the tree amplitude for pion pion scattering in the minimal linear sigma model...
First it is shown that the tree amplitude for pion–pion scattering in the minimal linear sigma mode...
First it is shown that the tree amplitude for pion pion scattering in the minimal linear sigma model...
An earlier calculation in a generalized linear sigma model showed that the well-known current algebr...
I review recent progress made in the description of pion-nucleon scattering, the $\sigma$--term, the...
The weak decay of the kaon to two pions is studied within the model of Nambu and Jona-Lasinio. Using...
The five different K -> 3 Pi and the three K -> 2 Pi decays are calculated in Chiral Perturbation Th...
The five different K -> 3 Pi and the three K -> 2 Pi decays are calculated in Chiral Perturbation Th...
We quantify the important effect of strong final state interactions id the weak K --> 2 pi amplitude...
We quantify the important effect of strong final state interactions id the weak K --> 2 pi amplitude...
The pion mass dependence of the nucleon mass within the covariant SU(2) baryon chiral perturbation t...
We derive a simplified representation for the pion mass to two loops in three-flavour chiral perturb...
We develop a unitarity approach to consider the final state interaction corrections to the tree leve...