Abstract <p>A total of 77 experimental values of reaction rates for the (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(n,2n\)</EquationSource> <!--NuclPhys2560100Titarenko-m1--> </InlineEquation>), (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(n,p\)</EquationSource> <!--NuclPhys2560100Titarenko-m2--> </InlineEquation>), (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(n,pn\)</EquationSource> <!--NuclPhys2560100Titarenko-m3--> </InlineEquation>), (<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(n,\alpha\)</EquationSource> <!--NuclPhys2560100Titarenko-m4--> </InlineEquation>), (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(n,\gamma\)</EquationSource> <!--NuclPhys2560100Titarenko-m5--> </InlineEquation>), and (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(n,f\)</EquationSource> <!--NuclPhys2560100Titarenko-m6--> </InlineEquation>) channels were obtained in the neutron spectrum generated by 21.5 MeV protons irradiating a beryllium target. The measurements were carried out using both natural and highly enriched samples of the following elements: <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m7--> </InlineEquation>Ni, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m8--> </InlineEquation>Zr, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m9--> </InlineEquation>Nb, <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m10--> </InlineEquation>Cd, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m11--> </InlineEquation>Ti, <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m12--> </InlineEquation>Co, <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq13.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{63,65,\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m13--> </InlineEquation>Cu, <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq14.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{64}\)</EquationSource> <!--NuclPhys2560100Titarenko-m14--> </InlineEquation>Zn, <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m15--> </InlineEquation>In, <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m16--> </InlineEquation>Al, <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m17--> </InlineEquation>Mg, <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m18--> </InlineEquation>Fe, <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m19--> </InlineEquation>Au and <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\textrm{nat}}\)</EquationSource> <!--NuclPhys2560100Titarenko-m20--> </InlineEquation>Th. The experiments were performed using the activation technique without destructive analysis of the irradiated samples. Reaction products were measured via <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq21.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--NuclPhys2560100Titarenko-m21--> </InlineEquation>-ray spectrometry employing two coaxial high-purity germanium (HP Ge) detectors and one planar detector. The acquired <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq21.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--NuclPhys2560100Titarenko-m22--> </InlineEquation>-spectra were processed using the GENIE2000 software suite. Independent and/or cumulative reaction rates were calculated using the SIGMA code. In total, 77 reaction products were identified, with half-lives ranging from 9.458 minutes (<InlineEquation ID="IEq23"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq23.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{27}\)</EquationSource> <!--NuclPhys2560100Titarenko-m23--> </InlineEquation>Mg) to 5.27 years (<InlineEquation ID="IEq24"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3625_Article_IEq24.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{60}\)</EquationSource> <!--NuclPhys2560100Titarenko-m24--> </InlineEquation>Co). The resulting dataset was utilized to assess the predictive capabilities of the PHITS-3.31 code coupled with the JENDL-5 nuclear data library, as applied to the modeling of blanket systems in hybrid reactor facilities.</p>

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Benchmark Experiments Using Neutrons Produced by 21.5 MeV Proton Irradiation of a ‘‘Thick’’ Beryllium Target

  • Yu. E. Titarenko,
  • A. A. Arkhipov,
  • S. A. Balyuk,
  • V. F. Batyaev,
  • M. V. Batyaeva,
  • V. D. Davidenko,
  • V. M. Zhivun,
  • Ya. O. Zaritskiy,
  • A. A. Kovalishin,
  • M. V. Kotelniy,
  • A. S. Kirsanov,
  • T. V. Kulevoy,
  • I. V. Mednikov,
  • B. A. Novikov,
  • A. V. Orlov,
  • K. V. Pavlov,
  • V. S. Stolbunov,
  • A. Yu. Titarenko,
  • R. S. Tikhonov,
  • M. N. Shlenskii,
  • N. A. Kovalenko

摘要

Abstract

A total of 77 experimental values of reaction rates for the ( \(n,2n\) ), ( \(n,p\) ), ( \(n,pn\) ), ( \(n,\alpha\) ), ( \(n,\gamma\) ), and ( \(n,f\) ) channels were obtained in the neutron spectrum generated by 21.5 MeV protons irradiating a beryllium target. The measurements were carried out using both natural and highly enriched samples of the following elements: \({}^{\textrm{nat}}\) Ni, \({}^{\textrm{nat}}\) Zr, \({}^{\textrm{nat}}\) Nb, \({}^{\textrm{nat}}\) Cd, \({}^{\textrm{nat}}\) Ti, \({}^{\textrm{nat}}\) Co, \({}^{63,65,\textrm{nat}}\) Cu, \({}^{64}\) Zn, \({}^{\textrm{nat}}\) In, \({}^{\textrm{nat}}\) Al, \({}^{\textrm{nat}}\) Mg, \({}^{\textrm{nat}}\) Fe, \({}^{\textrm{nat}}\) Au and \({}^{\textrm{nat}}\) Th. The experiments were performed using the activation technique without destructive analysis of the irradiated samples. Reaction products were measured via \(\gamma\) -ray spectrometry employing two coaxial high-purity germanium (HP Ge) detectors and one planar detector. The acquired \(\gamma\) -spectra were processed using the GENIE2000 software suite. Independent and/or cumulative reaction rates were calculated using the SIGMA code. In total, 77 reaction products were identified, with half-lives ranging from 9.458 minutes ( \({}^{27}\) Mg) to 5.27 years ( \({}^{60}\) Co). The resulting dataset was utilized to assess the predictive capabilities of the PHITS-3.31 code coupled with the JENDL-5 nuclear data library, as applied to the modeling of blanket systems in hybrid reactor facilities.