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Phys. Rev. Lett. 98, 102501 (2007) [4 pages]

Effect of γ Softness on the Stability of Chiral Geometry: Spectroscopy of 106Ag

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P. Joshi1, M. P. Carpenter2, D. B. Fossan3, T. Koike3,4, E. S. Paul5, G. Rainovski5,3,6, K. Starosta3,7, C. Vaman3,7, and R. Wadsworth1
1Department of Physics, University of York, Heslington, YO10 5DD, United Kingdom
2Argonne National Laboratory, 9700 South Cass Avenue, Argonne, Illinois 60439, USA
3Department of Physics and Astronomy, SUNY, Stony Brook, New York 11794-3800, USA
4Graduate School of Science, Tohoku University, Sendai, 980-8578, Japan
5Oliver Lodge Laboratory, Department of Physics, University of Liverpool, Liverpool, L69 7ZE, United Kingdom
6St. Kliment Ohridski University of Sofia, Sofia 1164, Bulgaria
7NSCL, Michigan State University, 164 South Shaw Lane, East Lansing, Michigan 48824-1321, USA

Received 26 September 2006; published 7 March 2007

A study of the nucleus 106Ag has revealed the presence of two strongly coupled negative-parity rotational bands up to the 19- and 20- states, respectively, which cross each other at spin I∼14. The data suggest that near the crossover point the bands correspond to different shapes, which is different to the behavior expected from a pair of chiral bands. Inspection of the properties of these bands indicates a triaxial and a planar nature of rotation for the two structures. Possible causes for this may be understood in terms of a shape transformation resulting from the large degree of γ softness of 106Ag. These data, along with the systematics of the odd-odd structures in the mass 100 region, suggest that γ softness has marked implications for the phenomenon of nuclear chirality.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.98.102501
DOI:
10.1103/PhysRevLett.98.102501
PACS:
21.10.Re, 21.60.Ev, 23.20.−g, 27.60.+j