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Phys. Rev. C 73, 054604 (2006) [8 pages]

Deducing the 237U(n,f) cross section using the surrogate ratio method

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J. T. Burke*, L. A. Bernstein, J. Escher, L. Ahle, J. A. Church, F. S. Dietrich, K. J. Moody, and E. B. Norman
Lawrence Livermore National Laboratory, Livermore, California 94551, USA

L. Phair, P. Fallon, R. M. Clark, M. A. Deleplanque, M. Descovich, M. Cromaz, I. Y. Lee, A. O. Macchiavelli, M. A. McMahan, L. G. Moretto, E. Rodriguez-Vieitez, and F. S. Stephens
Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA

H. Ai and C. Plettner
Yale University, New Haven, Connecticut 06520, USA

C. Beausang and B. Crider
University of Richmond, Richmond, Virginia 23173, USA

Received 25 January 2006; published 5 May 2006

We have deduced the cross section for 237U(n,f) over an equivalent neutron energy range from 0 to 20 MeV using the surrogate ratio method. A 55 MeV 4He beam from the 88 inch cyclotron at Lawrence Berkeley National Laboratory was used to induce fission in the following reactions: 238U(α,αf) and 236U(α,αf). The 238U reaction was a surrogate for 237U(n,f), and the 236U reaction was used as a surrogate for 235U(n,f). Scattered α particles were detected in a fully depleted segmented silicon telescope array over an angle range of 35° to 60° with respect to the beam axis. The fission fragments were detected in a third independent silicon detector located at backward angles between 106° and 131°.

© 2006 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.73.054604
DOI:
10.1103/PhysRevC.73.054604
PACS:
24.50.+g, 24.75.+i

*Electronic address: burke26@llnl.gov