Phys. Rev. C 56, 142 - 153 (1997)

Competing single-particle and collective structures in 86Nb

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S. L. Tabor, J. Döring, G. D. Johns, R. A. Kaye, and G. N. Sylvan
Department of Physics, Florida State University, Tallahassee, Florida 32306

C. J. Gross
ORISE, Oak Ridge Associated Universities, Oak Ridge, Tennessee 37831
Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831

Y. A. Akovali, C. Baktash, and D. W. Stracener
Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831

P. F. Hua, M. Korolija, D. R. LaFosse, and D. G. Sarantites
Chemistry Department, Washington University, St. Louis, Missouri 63130

F. E. Durham
Department of Physics, Tulane University, New Orleans, Louisiana 70118

I. Y. Lee, A. O. Macchiavelli, and , and W. Rathbun
Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720

A. Vander Molen
National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824

Received 25 November 1996

The high-spin structure of odd-odd 86Nb was studied with the early implementation of GAMMASPHERE using 36 Compton-suppressed Ge detectors and the MICROBALL, a 95-element full-sphere charged-particle detector array. High-spin states were populated using the 58Ni(32S,3pn) reaction at 135 MeV with beams from the 88-Inch Cyclotron at Lawrence Berkeley National Laboratory. A number of bands were observed up to spins as high as (31-). The yrast positive-parity band shares many characteristics with the πg9/2⊗νg9/2 bands in other odd-odd f-p-g shell nuclei. These similarities include the behavior of the moments of inertia, the magnitude and phase of the signature splitting and its phase reversal near the 10+ state, and the strong alternations in the B(M1)/B(E2) strengths. The moments of inertia in the lowest pair of negative-parity bands start out with a sharp upbend and then gradually fall back to the rigid-body value. New positive- and negative-parity bands appear in the quasiparticle alignment region and eventually become yrast. Some additional positive-parity states around spin 17ħ are candidates for fully or nearly fully aligned shell-model-like configurations.


©1997 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevC.56.142
DOI: 10.1103/PhysRevC.56.142
PACS: 23.20.En, 23.20.Lv, 25.70.Gh, 27.50.+e

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