Separable potential model for meson-baryon interaction beyond the S-wave
arXiv:1206.5168 · doi:10.1103/PhysRevC.86.024003
Abstract
A model for low-energy meson-baryon interaction in the strange sector is presented. The interaction is described in terms of separable potentials with multiple partial waves considered. A general solution of Lippmann-Schwinger equation for the scattering of spin zero and spin one-half particles is derived. Next, the general framework is applied to the sector in a simple model with only the S- and P-waves taken into account. The separable potential is designed to match the chiral perturbation theory at lowest nontrivial order. It is shown that although a simple model with three free parameters works well for the S-wave, it fails to reproduce the P-wave features of kaon-nucleon physics. Most importantly, the P-wave interaction is too weak to express a resonant behavior that could be identified as resonance.
References in corpus (14)
- Chiral Dynamics in Nucleons and Nuclei
- Chiral dynamics in the presence of bound states: kaon-nucleon interactions revisited
- Chiral Dynamics and the Low Energy Kaon-Nucleon Interaction
- Nuclear kaon dynamics
- Chiral dynamics of the S11(1535) and S11(1650) resonances revisited
- Kaonic hydrogen X-ray measurement in SIDDHARTA
- Chirally motivated amplitudes for in-medium applications
- K^- nuclear potentials from in-medium chirally motivated models
- Chiral SU(3) Dynamics and Antikaon-Nuclear quasibound States
- Separable potential model for interactions at low energies
- Calculations of nuclear quasi-bound states based on chiral meson-baryon amplitudes
- Kaonic hydrogen versus the low energy data
- Constraints on the threshold K- nuclear potential from FINUDA (stopped K-, pi-) hypernuclear spectra
- Lambda-hypernuclear production in stopped (K-,pion) reactions reexamined