Coupled channel Faddeev calculations of a (Kbar-N-pi) quasibound state
arXiv:1103.4757 · doi:10.1016/j.nuclphysa.2011.06.022
Abstract
The (Kbar-N-pi) system is studied using separable interactions fitted to data available on the s-wave (Kbar-N)--(pi-Y) subsystem and the p-wave (pi-N),(pi-Y),(pi-pi) and (pi-Kbar) subsystems. Three-body (Kbar-N-pi)--(pi-Y-pi) coupled channel Faddeev equations with relativistic kinematics are solved in search for quasibound poles in the complex plane, leading to a I(JP)=1(3/2-) (Kbar-N-pi) quasibound state at M ~ (1570 +/- 10) MeV and width greater than 60 MeV near the (Kbar-N-pi) threshold. A D13 Sigma(1570) resonance of molecular structure is thus predicted.
18 pages, 4 figures, 4 tables; v3--a typo corrected in Eq.(7) where the subscripts Lambda and Sigma in v2 and in the published journal version are interchanged, with none of the results and conclusions affected
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- Hadron spectroscopy from strangeness to charm and beauty
- Resonances from reactions with the center of mass energy from 1550 to 1676 MeV
- Separable Representation of Phenomenological Optical Potentials of Woods-Saxon Type
- Relativistic three-body calculations of a Y=1, I=3/2, JP=2+ pi-Lambda-N -- pi-Sigma-N dibaryon
- Pion-assisted charmed dibaryon candidate
- States of with within the Fixed Center Approximation to Faddeev equations
- Separable Representation of Energy-Dependent Optical Potentials
- Three-body hadron systems with strangeness
- Separable Potentials for (d,p) Reaction Calculations