Low-lying isomeric levels in {sup 75}Cu

Isomeric low-lying states were identified and investigated in the {sup 75}Cu nucleus. Two states at 61.8(5)- and 128.3(7)-keV excitation energies with half-lives of 370(40)- and 170(15)-ns were assigned as {sup 75m1}Cu and {sup 75m2}Cu, respectively. The measured half-lives combined with the recent...

Full description

Saved in:
Bibliographic Details
Published in:Physical review. C, Nuclear physics Vol. 81; no. 3
Main Authors: Daugas, J. M., Faul, T., Sauvestre, J. E., Grawe, H., Pfuetzner, M., Sawicka, M., Grzywacz, R., Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, Lewitowicz, M., France, G. de, Lopez Jimenez, M. J., Oliveira Santos, F. de, Achouri, N. L., Angelique, J. C., Baiborodin, D., Bentida, R., Beraud, R., Emsallem, A., Borcea, C., Bingham, C. R., Grzywacz, K. L.
Format: Journal Article
Language:English
Published: United States 15-03-2010
Subjects:
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:Isomeric low-lying states were identified and investigated in the {sup 75}Cu nucleus. Two states at 61.8(5)- and 128.3(7)-keV excitation energies with half-lives of 370(40)- and 170(15)-ns were assigned as {sup 75m1}Cu and {sup 75m2}Cu, respectively. The measured half-lives combined with the recent spin assignment of the ground state allow one to deduce tentatively spin and parity of the two isomers and the dominant multipolarities of the isomeric transitions with respect to the systematics of the Cu isotopes. Shell-model calculations using an up-to-date effective interaction reproduce the evolution of the 1/2{sup -}, 3/2{sup -}, and 5/2{sup -} states for the neutron-rich odd-mass Cu isotopes when filling the nug{sub 9/2}. The results indicate a significant change in the nuclear structure in this region, where a single-particle 5/2{sup -} state coexists with more and more collective 3/2{sup -} and 1/2{sup -} levels at low excitation energies.
ISSN:0556-2813
1089-490X
DOI:10.1103/PHYSREVC.81.034304