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Phys. Rev. C 57, 2724–2730 (1998)

Nonresonant direct p- and d-wave neutron capture by 12C

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T. Kikuchi1, Y. Nagai1, T. S. Suzuki1, T. Shima1, T. Kii1, M. Igashira2, A. Mengoni3,4,5, and T. Otsuka3,5
1Tokyo Institute of Technology, Department of Applied Physics, O-okayama, Meguro, Tokyo 152, Japan
2Tokyo Institute of Technology, Research Laboratory for Nuclear Reactors, O-okayama, Meguro, Tokyo 152, Japan
3The Institute of Physical and Chemical Research (RIKEN), Wako, Saitama 351-01, Japan
4National Institute for New Technologies, Energy and Environment (ENEA), v. Don Fiammelli 2, I-40129 Bologna, Italy
5The University of Tokyo, Department of Physics, Hongo, Bunkyo, Tokyo 113, Japan

Received 15 December 1997; published in the issue dated May 1998

Discrete γ rays from the neutron capture state of 13C to its low-lying bound states have been measured using pulsed neutrons at En=550keV. The partial capture cross sections have been determined to be 1.7±0.5, 24.2±1.0, 2.0±0.4, and 1.0±0.4μb for the ground (Jπ=1/2-) and first- (Jπ=1/2+), second- (Jπ=3/2-), and third- (Jπ=5/2+) excited states, respectively. From a comparison with theoretical predictions based on the nonresonant direct radiative capture mechanism, we could determine the spectroscopic factor for the Jπ=1/2+ state to be 0.80±0.04, free from neutron-nucleus interaction ambiguities in the continuum. In addition we have detected the contribution of the nonresonant d-wave capture component in the partial cross sections for transitions leading to the Jπ=1/2- and Jπ=3/2- states. While the s-wave capture dominates at En<~100keV, the d-wave component turns out to be very important at higher energies. From the present investigation the 12C(n,γ)13C reaction rate is obtained for temperatures in the range 107–1010K.

© 1998 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.57.2724
DOI:
10.1103/PhysRevC.57.2724
PACS:
25.40.Lw, 21.10.Jx, 26.20.+f, 26.30.+k