Single-particle spectral function of the hyperon in finite nuclei
arXiv:1603.05635 · doi:10.1016/j.nuclphysa.2016.11.002
Abstract
The spectral function of the hyperon in finite nuclei is calculated from the corresponding self-energy, which is constructed within a perturbative many-body approach using some of the hyperon-nucleon interactions of the Jülich and Nijmegen groups. Binding energies, wave functions and disoccupation numbers of different single-particle states are obtained for various hypernuclei from He to Pb. The agreement between the calculated binding energies and experimental data is qualitatively good. The small spin-orbit splitting of the and wave states is confirmed. The discrete and the continuum contributions of the single- spectral function are computed. Their appearance is qualitatively similar to that of the nucleons. The -factor, that measures the importance of correlations, is also calculated. Our results show that its value is relatively large, indicating that the hyperon is less correlated than nucleons. This is in agreement with the results obtained by other authors for the correlations of the in infinite nuclear matter. The disoccupation numbers are obtained by integrating the spectral function over the energy. Our results show that the discrete contribution to the disoccupation number decreases when increasing the momentum of the . This indicates that, in the production reactions of hypernuclei, the hyperon is mostly formed in a quasi-free state.
27 pages, 9 figures, 4 tables. Corrected version accepted for publication in Nuclear Physics A
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Cited by in corpus (9)
- Strangeness in Nuclei and Neutron Stars
- Hyperon-nucleon interaction within chiral effective field theory revisited
- Impact of chiral hyperonic three-body forces on neutron stars
- Hyperons: the strange ingredients of the nuclear equation of state
- Hyperon-nuclear interactions from SU(3) chiral effective field theory
- Structure of single- hypernuclei with chiral hyperon-nucleon potentials
- Charmed nuclei within a microscopic many-body approach
- Predictions for charmed nuclei based on forces inferred from lattice QCD simulations
- Properties of hyperons in nuclear matter from chiral hyperon-nucleon interactions at next-to-next-to-leading order