Neutron-induced fission fragment angular distributions, anisotropy, and linear momentum transfer measured with the NIFFTE fission time projection chamber

D. Hensle, J. T. Barker, J. S. Barrett, N. S. Bowden, K. J. Brewster, J. Bundgaard, Z. Q. Case, R. J. Casperson, D. A. Cebra, T. Classen, D. L. Duke, N. Fotiadis, J. Gearhart, V. Geppert-Kleinrath, U. Greife, E. Guardincerri, C. Hagmann, M. Heffner, C. R. Hicks, D. HigginsL. D. Isenhower, K. Kazkaz, A. Kemnitz, K. J. Kiesling, J. King, J. L. Klay, J. Latta, E. Leal, W. Loveland, M. Lynch, J. A. Magee, B. Manning, M. P. Mendenhall, M. Monterial, S. Mosby, G. Oman, C. Prokop, S. Sangiorgio, K. T. Schmitt, B. Seilhan, L. Snyder, F. Tovesson, C. L. Towell, R. S. Towell, T. R. Towell, N. Walsh, T. S. Watson, L. Yao, W. Younes

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Abstract

The Neutron Induced Fission Fragment Tracking Experiment (NIFFTE) collaboration has performed measurements with a fission time projection chamber to study the fission process by reconstructing full three-dimensional tracks of fission fragments and other ionizing radiation. The amount of linear momentum imparted to the fissioning nucleus by the incident neutron can be inferred by measuring the opening angle between the fission fragments. Using this measured linear momentum, fission fragment angular distributions can be converted to the center-of-mass frame for anisotropy measurements. Angular anisotropy is an important experimental observable for understanding the quantum mechanical state of the fissioning nucleus and vital to determining detection efficiency for cross section measurements. Neutron linear momentum transfer to fissioning U235, U238, and Pu239 and fission fragment angular anisotropy of U235 and U238 as a function of neutron energies in the range 130 keV-250 MeV are presented.

Original languageEnglish
Article number014605
JournalPhysical Review C
Volume102
Issue number1
DOIs
StatePublished - Jul 2020
Externally publishedYes

Funding

This work was performed under the auspices of the US Department of Energy by Lawrence Livermore National Laboratory under Contract No. DE-AC52-07NA27344. The neutron beam for this work was provided by LANSCE, which is funded by the US Department of Energy and operated by Los Alamos National Security, LLC, under Contract No. DE-AC52-06NA25396. University collaborators acknowledge support for this work from the US Department of Energy Nuclear Energy Research Initiative Project No. 08-014, the DOE-NNSA Stewardship Science Academic Alliances Program, under Grant No. DE-NA0002921, and through subcontracts from LLNL and LANL.

FundersFunder number
DOE-NNSADE-NA0002921
U.S. Department of Energy
Lawrence Livermore National LaboratoryDE-AC52-06NA25396, DE-AC52-07NA27344, 08-014
Los Alamos National Laboratory

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