The (2j-1) rule with other interactions

Abstract

We recently formulated a rule for isomeric states for a system of 4 nucleons with isospin T=1, namely that if the nucleons are in a single j shell then states with angular momenta J=2 and J=(2j-1) are either isomeric or ground states [ze12]. To show that this is a robust result, we here consider a new interaction from the literature that was used to discuss even-even and odd-even nuclei. We here apply it to an odd-odd nucleus.

arXiv admin note: substantial text overlap with arXiv:1107.4068, arXiv:1112.4801

References in corpus (4)

• Nuclear magic numbers: new features far from stability
• g9/2 nuclei and neutron-proton interaction
• Wave functions in the f_{7/2} shell, for educational purposes and ideas
• High-spin μs isomeric states in 96Ag

Cited by in corpus (7)

• Odd- J Pairing in Nuclei
• Importance of static quadrupole moments for determining collective aspects of nuclear structure: N=Z calculations with four and eight valence particles
• Symplectic group structure of the 48Cr, 88Ru, and 92Pd ground states
• Cooperation of anti-aligning and aligning shell-model forces for N=Z
• Symmetries in the \bm{g_{9/2}} shell
• Isobaric analog states in the f_{7/2} and g_{9/2} shells
• Schematic Interactions with Many Degeneracies