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Phys. Rev. C 53, 2763–2769 (1996)

Smooth band termination in 108Sn

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R. Wadsworth, C. W. Beausang, M. Cromaz, J. DeGraaf, T. E. Drake, D. B. Fossan, S. Flibotte, A. Galindo-Uribarri, K. Hauschild, I. M. Hibbert, G. Hackman, J. R. Hughes, V. P. Janzen, D. R. LaFosse, S. M. Mullins, E. S. Paul, D. C. Radford, H. Schnare, P. Vaska, D. Ward, J. N. Wilson, and I. Ragnarsson
Department of Physics, University of York, Heslington, York Y01 5DD, United Kingdom
Oliver Lodge Laboratory, University of Liverpool, Liverpool L69 3BX, United Kingdom
Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7
Department of Physics, S.U.N.Y. at Stony Brook, Stony Brook, New York 11794-3800
Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1
Chalk River Laboratories, AECL, Chalk River, Ontario, Canada K0J 1J0
Department of Mathematical Physics, Lund Institute of Technology, P.O. Box 118, S-221 00, Lund, Sweden

Received 10 October 1995; published in the issue dated June 1996

Three rotational bands in 108Sn have been investigated to high frequency via the 54Fe(58Ni,4p) reaction at 243 MeV. One of these bands is observed to undergo a band crossing at high spin. All three bands show a large decrease in their dynamic moments of inertia, to approximately one third of the rigid body value, as the rotational frequency approaches 1 MeV/ħ. The structures of these bands are thought to be based on 2p-2h proton excitations across the Z=50 shell gap and their properties can be interpreted in terms of cranked Nilsson-Strutinsky calculations. Such calculations predict smooth band terminations for all three struc- tures and a gradual shape change from collective prolate, at low spin, to noncollective oblate at high spin. © 1996 The American Physical Society.

© 1996 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.53.2763
DOI:
10.1103/PhysRevC.53.2763
PACS:
21.10.Re, 27.60.+j, 23.20.Lv