Localized , and Single-Particle Potentials in Finite Nuclei Calculated with Quark-Model Baryon-Baryon Interactions
arXiv:0904.0517 · doi:10.1103/PhysRevC.79.054318
Abstract
Localized single-particle potentials for all octet baryons, , , , and , in finite nuclei, C, O, Si, Ca, Fe, and Zr, are calculated using the quark-model baryon-baryon interactions. -matrices evaluated in symmetric nuclear matter in the lowest order Brueckner theory are applied to finite nuclei in local density approximation. Non-local potentials are localized by a zero-momentum Wigner transformation. Empirical single-particle properties of the nucleon and the hyperon in nuclear medium have been known to be explained semi-quantitatively in the LOBT framework. Attention is focused in the present consideration on predictions for the and hyperons. The unified description for the octet baryon-baryon interactions by the SU quark-model enables us to obtain less ambiguous extrapolation to the and sectors based on the knowledge in the sector than other potential models. The mean field is shown to be weakly attractive at the surface, but turns to be repulsive inside, which is consistent with the experimental evidence. The hyperon s.p. potential is also attractive at the nuclear surface region, and inside fluctuates around zero. Hence hypernuclear bound states are unlikely. We also evaluate energy shifts of the and atomic levels in Si and Fe, using the calculated s.p. potentials.
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Cited by in corpus (15)
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