<p>Prompt fission neutron spectra (PFNS) have a significant role in nuclear science and technology. In this study, the PFNS for <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1724_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{239}\text {Pu}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>239</mn> </mmultiscripts> <mtext>Pu</mtext> </mrow> </math></EquationSource> </InlineEquation> are evaluated using both differential and integral experimental data. A method that leverages integral criticality benchmark experiments to constrain the PFNS data is introduced. The measured central values of the PFNS are perturbed by constructing a covariance matrix. The PFNS are sampled using two types of covariance matrices, either generated with an assumed correlation matrix and incorporating experimental uncertainties or derived directly from experimental reports. The joint Monte Carlo transport code is employed to perform transport simulations on five criticality benchmark assemblies by utilizing perturbed PFNS data. Extensive simulations result in an optimized PFNS that shows improved agreement with the integral criticality benchmark experiments. This study introduces a novel approach for optimizing differential experimental data through integral experiments, particularly when a covariance matrix is not provided.</p>

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Optimization of the prompt fission neutron spectra of \(^{239}\)Pu(n,f) via criticality benchmarking

  • Jia-Hao Chen,
  • Bo Yang,
  • Qing-Gang Jia,
  • Rui Li,
  • Wen-Di Chen,
  • Hai-Rui Guo,
  • Wei-Li Sun,
  • Tao Ye

摘要

Prompt fission neutron spectra (PFNS) have a significant role in nuclear science and technology. In this study, the PFNS for \(^{239}\text {Pu}\) 239 Pu are evaluated using both differential and integral experimental data. A method that leverages integral criticality benchmark experiments to constrain the PFNS data is introduced. The measured central values of the PFNS are perturbed by constructing a covariance matrix. The PFNS are sampled using two types of covariance matrices, either generated with an assumed correlation matrix and incorporating experimental uncertainties or derived directly from experimental reports. The joint Monte Carlo transport code is employed to perform transport simulations on five criticality benchmark assemblies by utilizing perturbed PFNS data. Extensive simulations result in an optimized PFNS that shows improved agreement with the integral criticality benchmark experiments. This study introduces a novel approach for optimizing differential experimental data through integral experiments, particularly when a covariance matrix is not provided.