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Phys. Rev. C 71, 051601(R) (2005) [4 pages]

Two-neutron transfer in the 6He+209Bi reaction near the Coulomb barrier

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P. A. DeYoung1, Patrick J. Mears1, J. J. Kolata2, E. F. Aguilera3, F. D. Becchetti4, Y. Chen4, M. Cloughesy2, H. Griffin4, C. Guess1, J. D. Hinnefeld5, H. Jiang4, Scott R. Jones6, U. Khadka1, D. Lizcano3, E. Martinez-Quiroz3, M. Ojaniega4, G. F. Peaslee7, A. Pena1, J. Rieth1, S. VanDenDriessche5, and J. A. Zimmerman6
1Department of Physics and Engineering, Hope College, Holland, Michigan 49423-9000
2Physics Department, University of Notre Dame, Notre Dame, Indiana, 46556-5670
3Departamento del Acelerador, Instituto Nacional de Investigaciones Nucleares, A.P. 18-1027, C.P. 11801, Mexico, D.F.
4Physics Department, University of Michigan, Ann Arbor, Michigan 48109-1120
5Physics Department, Indiana University South Bend, South Bend, Indiana 46634-7111
6Department of Chemistry, Southwest Missouri State University, Springfield, Missouri 65804-0094
7Department of Chemistry, Hope College, Holland, Michigan 49423-9000

Received 13 September 2004; published 13 May 2005

The cross section for α-particle emission in the 6He+209Bi reaction at energies near the Coulomb barrier is remarkably large. Possible reactions that may produce the observed α particles include two-neutron transfer, one-neutron transfer, and direct projectile breakup. Each of these mechanisms results in a distinctive angular correlation between the α particle and the outgoing neutron(s). A neutron-α-particle coincidence experiment was performed to study two-neutron transfer to unbound states of 211Bi. It is shown that approximately 55% of the observed α-particle yield at and beyond the grazing angle is because of this process. This is more than 2.5 times the fraction attributable to single-neutron transfer. The corresponding 2n-transfer cross section is 0.4 ± 0.1 b.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.71.051601
DOI:
10.1103/PhysRevC.71.051601
PACS:
25.60.Je, 27.20.+n