Abstract
The πΛ. N-πσ. N coupled-channel system with quantum numbers (Y, I, JP)=(1, 32, 2+) is studied in a relativistic three-body model, using two-body separable interactions in the dominant p-wave pion-baryon and S13 YN channels. Three-body equations are solved in the complex energy plane to search for quasibound state and resonance poles, producing a robust narrow πΛN resonance about 10-20 MeV below the πσN threshold. Viewed as a dibaryon, it is a S25 quasibound state consisting of σ(1385). N and δ(1232). Y components. Comparison is made between the present relativistic model calculation and a previous, outdated nonrelativistic calculation which resulted in a πΛN bound state. Effects of adding a K̄NN channel are studied and found insignificant. Possible production and decay reactions of this (Y,I,JP)=(1,32,2+) dibaryon are discussed.
| Original language | English |
|---|---|
| Pages (from-to) | 167-178 |
| Number of pages | 12 |
| Journal | Nuclear Physics A |
| Volume | 897 |
| DOIs | |
| State | Published - 2 Jan 2013 |
Keywords
- Dibaryons
- Faddeev equations
- Hyperon-nucleon interactions
- Pion-baryon interactions
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