N. Keeley *, T. L. Drummer †, and E. E. Bartosz ‡
Department of Physics, The Florida State University, Tallahassee, Florida 32306-4350
C. R. Brune §
Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255
Triangle Universities Nuclear Laboratory, Durham, North Carolina 27088-0308
P. D. Cathers **
Department of Physics, The Florida State University, Tallahassee, Florida 32306-4350
M. Fauerbach ††
Department of Physics, The Florida State University, Tallahassee, Florida 32306-4350
H. J. Karwowski
Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255
Triangle Universities Nuclear Laboratory, Durham, North Carolina 27088-0308
K. W. Kemper
Department of Physics, The Florida State University, Tallahassee, Florida 32306-4350
B. Kozłowska
Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255;
Triangle Universities Nuclear Laboratory, Durham, North Carolina 27088-0308;
Institute of Physics, University of Silesia, ul. Uniwersytecka 4, 40-007 Katowice, Poland
E. J. Ludwig
Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255
Triangle Universities Nuclear Laboratory, Durham, North Carolina 27088-0308
F. Maréchal ‡‡
Department of Physics, The Florida State University, Tallahassee, Florida 32306-4350
A. J. Mendez ¶
Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255
Triangle Universities Nuclear Laboratory, Durham, North Carolina 27088-0308
E. G. Myers and D. Robson
Department of Physics, The Florida State University, Tallahassee, Florida 32306-4350
K. Rusek
The Andrzej Sołtan Institute for Nuclear Studies, ul. Hoża 69, 00-681 Warsaw, Poland
K. D. Veal a
Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255
Triangle Universities Nuclear Laboratory, Durham, North Carolina 27088-0308
Received 11 December 2002; published 18 April 2003
The results of extensive coupled-reaction-channel calculations are compared with the cross section and new analyzing power data for the 12C(6Li,d)16O reaction leading to the 0.0-MeV 0+, 6.13-MeV 3-, 6.92-MeV 2+, 8.87-MeV 2-, and 10.35-MeV 4+ states of 16O at 6Li bombarding energies of 34 and 50 MeV. All the analyzing power data at both energies and all the cross section data at 50 MeV, with the exception of that for the 12C(6Li,d)16O transition to the 0.0-MeV 0+ state of 16O are presented here for the first time. These results suggest that there are significant multistep contributions to transfers leading to the 0+ and 3- states, while those leading to the 2+ and 4+ states may be reasonably well described by simple direct α transfer. The importance of multistep effects is found to increase with increasing bombarding energy.
©2003 The American Physical Society
URL: http://link.aps.org/doi/10.1103/PhysRevC.67.044604
DOI: 10.1103/PhysRevC.67.044604
PACS: 25.70.Hi, 24.10.Eq, 21.60.Gx
* Email address: keeley@nucmar.physics.fsu.edu
† Present address: University of Illinois, Urbana, Illinois.
‡ Present address: CyTerra Corporation, Orlando, Florida.
§ Present address: Department of Physics and Astronomy, Ohio University, Athens, Ohio.
** Present address: University of Belize, Belize City, Belize.
†† Present address: Florida Gulf Coast University, Fort Myers, Florida.
‡‡ Present address: Institut de Recherches Subatomiques, Strasbourg, France.
¶ Present address: Oak Ridge National Laboratory, Oak Ridge, Tennessee.
a Present address: Los Alamos National Laboratory, Los Alamos, New Mexico.
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