Classification of States in O(8) Proton-Neutron Pairing Model

Details Classification of States in O(8) Proton-Neutron Pairing Model Classification of States in O(8) Proton-Neutron Pairing Model

2005-03-04

arxiv.org/abs/nucl-th/0503010v1

Nucl.Phys. A764 (2006) 181-204

Physics

Nuclear Physics

Nuclear Theory

52 pages, 12 tables

Scientific paper

10.1016/j.nuclphysa.2005.09.011

Isoscalar (T=0) plus isovector (T=1) pairing hamiltonian in LS-coupling, which is important for heavy N=Z nuclei, is solvable in terms of a O(8) algebra for some special values of the mixing parameter that measures the competition between T=0 and T=1 pairing. The O(8) algebra is generated, amongst others, by the $S=1,T=0$ and $S=0,T=1$ pair creation and annihilation operators . Shell model algebras, with only number conserving operators, that are complementary to the $O(8) \supset O_{ST}(6) \supset O_S(3) \otimes O_T(3)$, $O(8) \supset [ O_S(5) \supset O_S(3) ] \otimes O_T(3)$ and $O(8) \supset [ O_T(5) \supset O_T(3)] \otimes O_S(3)$ sub-algebras are identified. The problem of classification of states for a given number of nucleons (called `plethysm' problem in group theory), for these group chains is solved explicitly for states with O(8) seniority $v=0, 1, 2, 3$ and 4. Using them, band structures in isospin space are identified for states with $v=0, 1, 2$ and 3.

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