Alpha-like quartet condensation and isovector pairing correlations in N=Z nuclei
arXiv:1203.0779 · doi:10.1103/PhysRevC.85.061303
Abstract
We propose a simple quartet condensation model (QCM) which describes with very high accuracy the isovector pairing correlations in self-conjugate nuclei. The quartets have an alpha-like structure and are formed by collective isovector pairs. The accuracy of the QCM is tested for N=Z nuclei for which exact shell model diagonalizations can be performed. The calculations are done with two isovector pairing forces, one extracted from standard shell model interactions and the other of seniority type, acting, respectively, upon spherical and axially-deformed single-particle states. It is shown that for all calculated nuclei the QCM gives very accurate values for the pairing correlations energies, with errors which do not exceed 1%. These results show clearly that the correlations induced by the isovector pairing in self-conjugate nuclei are of quartet type and also indicate that QCM is the proper tool to calculate the isovector proton-neutron correlations in mean field pairing models.
11 pages, two tables
References in corpus (6)
- Competing orders in one dimensional spin 3/2 fermionic systems
- Accuracy of BCS-based approximations for pairing in small Fermi systems
- Isovector neutron-proton pairing with particle number projected BCS
- Unified BCS-like model of pairing and alpha-correlations
- Systematic study of proton-neutron pairing correlations in the nuclear shell model
- Pairing and alpha-like quartet condensation in N=Z nuclei
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