New effective interaction for f5pg9-shell nuclei

M. Honma, T. Otsuka, T. Mizusaki, and M. Hjorth-Jensen
Phys. Rev. C 80, 064323 – Published 30 December 2009

Abstract

We present a new effective interaction for shell-model calculations in the model space consisting of the single-particle orbits 1p3/2, 0f5/2, 1p1/2, and 0g9/2. Starting with a realistic interaction based on the Bonn-C potential, 133 two-body matrix elements and four single-particle energies are modified empirically so as to fit 400 experimental energy data out of 69 nuclei with mass numbers A=63~96. The systematics of binding energies, electromagnetic moments and transitions, and low-lying energy levels are described. The soft Z=28 closed core is observed, in contrast to the stable N=50 shell closure. The new interaction is applied to systematic studies of three different chains of nuclei, Ge isotopes around N=40, N=Z nuclei with A=64~70, and N=49 odd-odd nuclei, focusing especially on the role of the g9/2 orbit. The irregular behavior of the 02+ state in Ge isotopes is understood as a result of detailed balance between the N=40 single-particle energy gap and the collective effects. The development of the band structure in N=Z nuclei is interpreted in terms of successive excitations of nucleons into the g9/2 orbit. The triaxial/γ-soft structure in Ge64 and the prolate/oblate shape coexistence in Se68 are predicted, showing a good correspondence with the experimental data. The isomeric states in As66 and Br70 are obtained with the structure of an aligned proton-neutron pair in the g9/2 orbit. Low-lying energy levels in N=49 odd-odd nuclei can be classified as proton-neutron pair multiplets, implying that the obtained single-particle structure in this neutron-rich region appears to be appropriate. These results demonstrate that, in spite of the modest model space, the new interaction turns out to describe rather well properties related to the g9/2 orbit in various cases, including moderately deformed nuclei.

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  • Received 25 June 2009

DOI:https://doi.org/10.1103/PhysRevC.80.064323

©2009 American Physical Society

Authors & Affiliations

M. Honma1, T. Otsuka2,3,4, T. Mizusaki5, and M. Hjorth-Jensen6

  • 1Center for Mathematical Sciences, University of Aizu, Tsuruga, Ikki-machi, Aizu-Wakamatsu, Fukushima 965-8580, Japan
  • 2Department of Physics and Center for Nuclear Study, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
  • 3RIKEN, Hirosawa, Wako-shi, Saitama 351-0198, Japan
  • 4National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824-1321, USA
  • 5Institute of Natural Sciences, Senshu University, Higashimita, Tama, Kawasaki, Kanagawa 214-8580, Japan
  • 6Department of Physics and Center of Mathematics for Applications, University of Oslo, N-0316 Oslo, Norway

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Vol. 80, Iss. 6 — December 2009

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