1999
DOI: 10.1103/physrevc.59.3009
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Soft-core baryon-baryon potentials for the complete baryon octet

Abstract: SU(3) symmetry relations on the recently constructed hyperon-nucleon potentials are used to develop potential models for all possible baryon-baryon interaction channels. The main focus is on the interaction channels with total strangeness S = −2, −3, and −4, for which no experimental data exist yet. The potential models for these channels are based on SU(3) extensions of potential models for the S = 0 and S = −1 sectors, which are fitted to experimental data. Although the SU(3) symmetry is not taken to be exac… Show more

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Cited by 387 publications
(548 citation statements)
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“…The inclusion of the hyperon-hyperon interaction leads to a further softening of the EOS, since this interaction is attractive over the whole density range explored. This is mainly due to the ΣΣ interaction which is strongly enough to develop a bound state [4]. We note, however, that the ΛΛ attraction produced by this model is only mild, not being able to reproduce the experimental 2Λ separation energy of ∆B ΛΛ ∼ 4 − 5 MeV.…”
Section: Discussionmentioning
confidence: 78%
See 1 more Smart Citation
“…The inclusion of the hyperon-hyperon interaction leads to a further softening of the EOS, since this interaction is attractive over the whole density range explored. This is mainly due to the ΣΣ interaction which is strongly enough to develop a bound state [4]. We note, however, that the ΛΛ attraction produced by this model is only mild, not being able to reproduce the experimental 2Λ separation energy of ∆B ΛΛ ∼ 4 − 5 MeV.…”
Section: Discussionmentioning
confidence: 78%
“…[4]. This potential describes all the strangeness sectors from S = 0 to S = −4 and is based on SU(3) extensions of the Nijmegen nucleon-nucleon and hyperon-nucleon potentials.…”
Section: Formalismmentioning
confidence: 99%
“…In our work the Nijmegen soft-core NY potentials NSC89 [11], NSC97f [12], or ESC08b [13] are used, which are fitted to the available experimental NY scattering data, together with the nucleonic forces + TBF introduced before. With the NN and NY potentials, the various G matrices are evaluated by solving numerically the Bethe-Goldstone equation, written in operatorial form as with the s.p.…”
Section: Hyperons In Nuclear Mattermentioning
confidence: 99%
“…In order to understand the enhancement factor as a function of the Λ-n relative momentum q, we computed the enhancement factors, as a function of q, by using combinations of a and r from Refs. [11][12][13][14][15][16][17].…”
Section: Feasibility Of the Measurement Of λ-N Final State Interactiomentioning
confidence: 99%