Mass distributions in monoenergetic-neutron-induced fission of Pu239
James E. Gindler, L.E. Glendenin, Deborah J. Henderson, J.W. Meadows
Abstract
James E. Gindler, L.E. Glendenin, Deborah J. Henderson, J.W. Meadows
Abstract
Fission product yields for 24 masses were determined for the fission of $^{239}\mathrm{Pu}$ with essentially monoenergetic neutrons of 0.17, 1.0, 2.0, 3.4, 4.5, 6.1, and 7.9 MeV. Fission product activities were measured by Ge(Li) $\ensuremath{\gamma}$-ray spectrometry of irradiated $^{239}\mathrm{Pu}$ targets and by chemical separation of the fission product elements followed by $\ensuremath{\beta}$ counting. Yields of near symmetric (valley) fission products increase nearly monotonically with incident neutron energy and do not exhibit a break in the slope of the yield versus neutron energy curve in the energy region where second-chance fission begins. This is in contrast to the curves for $^{232}\mathrm{Th}$, $^{235}\mathrm{U}$, and $^{238}\mathrm{U}$ neutron-induced fission.NUCLEAR REACTIONS, FISSION $^{239}\mathrm{Pu}(n, f)$, ${E}_{n}=0.17, 1.0, 2.0, 3.4, 4.5, 6.1, \mathrm{and} 7.9$ MeV; measured mass yields.
OpenAlex reports 30 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Fission product yields for 24 masses were determined for the fission of $^{239}\mathrm{Pu}$ with essentially monoenergetic neutrons of 0.17, 1.0, 2.0, 3.4, 4.5, 6.1, and 7.9 MeV. Fission product activities were measured by Ge(Li) $\ensuremath{\gamma}$-ray spectrometry of irradiated $^{239}\mathrm{Pu}$ targets and by chemical separation of the fission product elements followed by $\ensuremath{\beta}$ counting. Yields of near symmetric (valley) fission products increase nearly monotonically with incident neutron energy and do not exhibit a break in the slope of the yield versus neutron energy curve in the energy region where second-chance fission begins. This is in contrast to the curves for $^{232}\mathrm{Th}$, $^{235}\mathrm{U}$, and $^{238}\mathrm{U}$ neutron-induced fission.NUCLEAR REACTIONS, FISSION $^{239}\mathrm{Pu}(n, f)$, ${E}_{n}=0.17, 1.0, 2.0, 3.4, 4.5, 6.1, \mathrm{and} 7.9$ MeV; measured mass yields.
Key concepts: Fission, Fission product yield, Physics, Neutron, Nuclear fission product, Nuclear physics, Neutron emission, Yield (engineering)