<p>The role of chlorine as a neutron poison and as a seed for producing radioactive waste in nuclear systems has driven a renewed interest to improve its nuclear data uncertainties. Additionally, basic and applied science programs that use CLYC (Cs<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(_2\)</EquationSource> </InlineEquation>LiYCl<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(_6\)</EquationSource> </InlineEquation>:Ce) detectors for neutron spectroscopy and monitoring are also very sensitive to any change in chlorine nuclear data for simulations of the detector response. In this work, sensitivities relevant for these different applications are addressed through simulations of the efficiency of CLYC detectors in a fast fission spectrum when applying new chlorine nuclear data as input. These simulations are validated by an experimental measurement using CLYC detectors coupled to an ionization chamber loaded with a <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(^{252}\)</EquationSource> </InlineEquation>Cf spontaneous fission source. The results are then used to obtain the first reliable direct measurement of the <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> </InlineEquation>Cl(<i>n</i>,<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(p_0\)</EquationSource> </InlineEquation>) and summed <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> </InlineEquation>Cl(<i>n</i>,<i>p</i>+<i>n</i>,<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\alpha\)</EquationSource> </InlineEquation>) fission spectrum average cross sections, found to be 54.7(32) and 105.0(98) mb, respectively. The results are within uncertainty of calculated fission spectrum averaged cross sections based on recently re-evaluated chlorine nuclear data, which confirm recent impact studies performed for the Molten Chloride Reactor Experiment. Meanwhile, there currently exists only one published criticality benchmark experiment that is sufficiently sensitive to chlorine nuclear data. Discrepancies are found with this set of criticality safety benchmarks, which are more sensitive to thermal and epithermal neutron energies than the energies, above 100&#xa0;keV, tested in this current work. Hence, there is still a need to re-evaluate the chlorine nuclear data at lower energies to assess these discrepancies. Interpretation of the data from future “faster” criticality benchmarks, which are needed for next-gen fast reactor designs, benefit from the improved constraints on the chlorine nuclear data validated in this work.</p>

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Constraining the impact of chlorine as a neutron absorber in next-gen fast reactor designs

  • K. Hanselman,
  • I. J. Allan,
  • S. A. Kuvin,
  • T. Kawano,
  • N. Kleedtke,
  • H. Y. Lee,
  • S. N. Paneru,
  • N. Thompson,
  • J. Winkelbauer,
  • T. Cisneros,
  • B. Harper,
  • M. Wargon

摘要

The role of chlorine as a neutron poison and as a seed for producing radioactive waste in nuclear systems has driven a renewed interest to improve its nuclear data uncertainties. Additionally, basic and applied science programs that use CLYC (Cs \(_2\) LiYCl \(_6\) :Ce) detectors for neutron spectroscopy and monitoring are also very sensitive to any change in chlorine nuclear data for simulations of the detector response. In this work, sensitivities relevant for these different applications are addressed through simulations of the efficiency of CLYC detectors in a fast fission spectrum when applying new chlorine nuclear data as input. These simulations are validated by an experimental measurement using CLYC detectors coupled to an ionization chamber loaded with a \(^{252}\) Cf spontaneous fission source. The results are then used to obtain the first reliable direct measurement of the \(^{35}\) Cl(n, \(p_0\) ) and summed \(^{35}\) Cl(n,p+n, \(\alpha\) ) fission spectrum average cross sections, found to be 54.7(32) and 105.0(98) mb, respectively. The results are within uncertainty of calculated fission spectrum averaged cross sections based on recently re-evaluated chlorine nuclear data, which confirm recent impact studies performed for the Molten Chloride Reactor Experiment. Meanwhile, there currently exists only one published criticality benchmark experiment that is sufficiently sensitive to chlorine nuclear data. Discrepancies are found with this set of criticality safety benchmarks, which are more sensitive to thermal and epithermal neutron energies than the energies, above 100 keV, tested in this current work. Hence, there is still a need to re-evaluate the chlorine nuclear data at lower energies to assess these discrepancies. Interpretation of the data from future “faster” criticality benchmarks, which are needed for next-gen fast reactor designs, benefit from the improved constraints on the chlorine nuclear data validated in this work.