The Octet Meson and Octet Baryon Interaction with strangeness and the
arXiv:1510.00580 · doi:10.1142/S0218301315500883
Abstract
The octet meson and baryon interaction with strangeness is studied fully relativistically with chiral Lagrangian. In this work, a Bethe-Salpeter equation approach with spectator quasipotential approximation is applied to study the reactions with and with all possible partial waves and theoretical results are comparable with experimental data. It is found that the Weinberg-Tomozawa potential derived from the lowest order chiral Lagrangian only provides the contributions from partial waves with spin-parities and . Two-pole structure of the is confirmed with poles at and MeV. The lower and higher poles originate from interaction as a resonance and interaction as a bound state, respectively.
13 pages, 4 figures
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Cited by in corpus (13)
- Nucleon resonances and as strange partners of LHCb pentaquarks
- Understanding spin parity of and in a hadronic molecular state picture
- Molecular picture for and
- Interpretation of as an isoscalar partner of from interaction
- Hidden-strange molecular states and the bound state via a QCD van der Waals force
- Possible molecular states and their productions in nulceon-antinulceon collision
- The and as hidden-strange molecular states from interaction
- Possible molecular states from the interaction
- Pole trajectories from - and -wave interactions
- Role of baryons in decay
- and interactions and LHCb pentaquarks
- (2030) and (2120) as molecular states
- Kaon-induced production of strange hidden-charm molecular pentaquarks from proton