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Hauptverfasser: Dongwi, D. H., Snyder, L., Aguilar, V., Androski, N., Anastasiou, M., Bowden, N. S., Chemey, A., Classen, T., Alencar, J. E. Fuzaro, Greife, U., Haseman, M., Isenhower, L. D., Klay, J. L., Loveland, W., Mendenhall, M. P., Monterial, M., Silveira, M., Prokop, C., Watson, T. S., Yao, L.
Format: Preprint
Veröffentlicht: 2024
Schlagworte:
Online-Zugang:https://arxiv.org/abs/2409.18279
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author Dongwi, D. H.
Snyder, L.
Aguilar, V.
Androski, N.
Anastasiou, M.
Bowden, N. S.
Chemey, A.
Classen, T.
Alencar, J. E. Fuzaro
Greife, U.
Haseman, M.
Isenhower, L. D.
Klay, J. L.
Loveland, W.
Mendenhall, M. P.
Monterial, M.
Silveira, M.
Prokop, C.
Watson, T. S.
Yao, L.
author_facet Dongwi, D. H.
Snyder, L.
Aguilar, V.
Androski, N.
Anastasiou, M.
Bowden, N. S.
Chemey, A.
Classen, T.
Alencar, J. E. Fuzaro
Greife, U.
Haseman, M.
Isenhower, L. D.
Klay, J. L.
Loveland, W.
Mendenhall, M. P.
Monterial, M.
Silveira, M.
Prokop, C.
Watson, T. S.
Yao, L.
contents The NIFFTE fission Time Projection Chamber (fissionTPC) has been used to measure the $^{239}$Pu(n,f)/$^{235}$U(n,f) cross-section ratio for neutron-induced fission in the range of 0.1 - 100 MeV, with high precision. A white neutron source was provided by the Los Alamos Neutron Science Center, where the experiment was conducted as a remeasurement to evaluate a roughly 2% discrepancy of the previous fissionTPC results with ENDF/B-VIII.0. A detailed accounting of measurement uncertainties was performed, based on the fissionTPC's novel ability to provide three-dimensional reconstruction of fission-fragment ionization profiles. Current results obtained using a vapor-deposited, highly uniform $^{239}$Pu target, in comparison to the measurement published in 2021, where a $^{239}$Pu electroplated target was used, are presented and discussed. The remeasurement presented here is in agreement with the previous fissionTPC result within measurement uncertainties.
format Preprint
id arxiv_https___arxiv_org_abs_2409_18279
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Remeasurement of the $^{239}$Pu(n,f)/$^{235}$U(n,f) Cross-Section Ratio with the NIFFTE fission Time Projection Chamber Using Vapor-deposited Targets
Dongwi, D. H.
Snyder, L.
Aguilar, V.
Androski, N.
Anastasiou, M.
Bowden, N. S.
Chemey, A.
Classen, T.
Alencar, J. E. Fuzaro
Greife, U.
Haseman, M.
Isenhower, L. D.
Klay, J. L.
Loveland, W.
Mendenhall, M. P.
Monterial, M.
Silveira, M.
Prokop, C.
Watson, T. S.
Yao, L.
Nuclear Experiment
The NIFFTE fission Time Projection Chamber (fissionTPC) has been used to measure the $^{239}$Pu(n,f)/$^{235}$U(n,f) cross-section ratio for neutron-induced fission in the range of 0.1 - 100 MeV, with high precision. A white neutron source was provided by the Los Alamos Neutron Science Center, where the experiment was conducted as a remeasurement to evaluate a roughly 2% discrepancy of the previous fissionTPC results with ENDF/B-VIII.0. A detailed accounting of measurement uncertainties was performed, based on the fissionTPC's novel ability to provide three-dimensional reconstruction of fission-fragment ionization profiles. Current results obtained using a vapor-deposited, highly uniform $^{239}$Pu target, in comparison to the measurement published in 2021, where a $^{239}$Pu electroplated target was used, are presented and discussed. The remeasurement presented here is in agreement with the previous fissionTPC result within measurement uncertainties.
title Remeasurement of the $^{239}$Pu(n,f)/$^{235}$U(n,f) Cross-Section Ratio with the NIFFTE fission Time Projection Chamber Using Vapor-deposited Targets
topic Nuclear Experiment
url https://arxiv.org/abs/2409.18279