Abstract
An extended mean-field model is presented that describes states of different isospin in odd-odd and even-even nuclei. Excitation energies of the states in even-even as well as and states in odd-odd nuclei are calculated. It is shown that the structure of these states can be determined in a consistent manner when both isoscalar and isovector pairing collectivity as well as isospin projection (treated here within the isocranking approximation) are taken into account. In particular, in odd-odd nuclei, the interplay between quasiparticle excitations (relevant for the case of states) and isorotations (relevant for the case of states) explains the near degeneracy of these states.
- Received 1 December 2000
DOI:https://doi.org/10.1103/PhysRevLett.87.052504
©2001 American Physical Society