Bulletin of the American Physical Society
2021 Fall Meeting of the APS Division of Nuclear Physics
Volume 66, Number 8
Monday–Thursday, October 11–14, 2021; Virtual; Eastern Daylight Time
Session QF: Nuclear Structure: Heavy Nuclei II
11:30 AM–1:18 PM,
Thursday, October 14, 2021
Room: Berkeley & Clarendon
Chair: Claus Muller-Gatermann, ANL
Abstract: QF.00009 : 233U(n, γ) measurements at LANSCE
1:06 PM–1:18 PM
Presenter:
Esther L Leal-Cidoncha
(Los Alamos National Laboratory)
Author:
Esther L Leal-Cidoncha
(Los Alamos National Laboratory)
alternative to the U-Pu fuel cycle due to its reduced amount of transuranium elements.
The experimental 233U(n,γ) cross section data available in the literature are scarce and
were measured decades ago [1, 2, 3]. An accurate measurement of the 233U(n,γ) cross
section is required by the NCSP (National Critically Safety Program) to complete the
neutron-induced cross section data, and also, as reported by the ORNL, a new evaluation
with revised (renormalized) fission cross section is needed on 233U.
For 233U fission is around one order of magnitude more likely than capture, hence, the
accuracy in the capture cross section measurement relies on the discrimination between
the γ’s produced in capture and fission reactions. This discrimination method requires the
use of an experimental setup combining capture and fission detectors. Therefore a new
measurement has been performed at LANL combining the Detector for Advanced
Neutron Capture Experiments (DANCE) to measure γ’s, with the NEUtron detector array
at dANCE (NEUANCE) to detect neutrons coming from fission and determine by
coincidence the γ’s produced by fission reactions tagging them.
This measurement will provide cross section data in the Resonance Region (RR),
focusing in the Unresolved Resonance Region (URR) in the keV neutron energy.
References
[1] E. Berthoumieux et al., Proceedings of the International Conference on Nuclear Data
for Science and Technology April 22-27, 2007, Nice, France (EDP Sciences, 2008) pp.
571-574.
[2] L. W. Weston et al., Nucl. Sci. Eng. 34, 1 (1968).
[3] J. C. Hopkins and B. C. Diven, Nucl. Sci. Eng. 12:2, 169-177 (1962).
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