Abstract <p>This study presents the production cross sections of<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3626_Article_IEq7.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{232,230}\)</EquationSource> <!--NuclPhys2560102Titarenko-m7--> </InlineEquation>Pa resulting from proton irradiationof <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3626_Article_IEq8.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{232}\)</EquationSource> <!--NuclPhys2560102Titarenko-m8--> </InlineEquation>Th at an energy of 20.9 MeV. In addition, theexcitation functions of <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3626_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{233}\)</EquationSource> <!--NuclPhys2560102Titarenko-m9--> </InlineEquation>Pa and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3626_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{231}\)</EquationSource> <!--NuclPhys2560102Titarenko-m10--> </InlineEquation>Th produced viaproton-induced reactions on <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3626_Article_IEq8.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{232}\)</EquationSource> <!--NuclPhys2560102Titarenko-m11--> </InlineEquation>Th in the energy range from0.02 to 1.6 GeV are analyzed, with consideration of the possiblecontribution of secondary neutrons to their formation. Theproduction cross sections for all reaction products were measuredusing direct gamma-ray spectrometry without chemical separation.The obtained experimental data are compared with results reportedby other authors, as well as with calculated excitation functionsgenerated using the PHITS-3.31 code (INCL4.6/GEM, JAM, and Bertinimodels) and the TENDL-2023 nuclear data library.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Production Cross Sections of \({}^{{233,232,230}}\)Pa and \({}^{{231}}\)Th via 20.9 MeV Proton Irradiation of \({}^{{232}}\)Th

  • 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,
  • S. E. Vinokurov,
  • A. G. Kazakov,
  • E. Yu. Khvorostinin,
  • A. V. Ignatyuk

摘要

Abstract

This study presents the production cross sections of \({}^{232,230}\) Pa resulting from proton irradiationof \({}^{232}\) Th at an energy of 20.9 MeV. In addition, theexcitation functions of \({}^{233}\) Pa and \({}^{231}\) Th produced viaproton-induced reactions on \({}^{232}\) Th in the energy range from0.02 to 1.6 GeV are analyzed, with consideration of the possiblecontribution of secondary neutrons to their formation. Theproduction cross sections for all reaction products were measuredusing direct gamma-ray spectrometry without chemical separation.The obtained experimental data are compared with results reportedby other authors, as well as with calculated excitation functionsgenerated using the PHITS-3.31 code (INCL4.6/GEM, JAM, and Bertinimodels) and the TENDL-2023 nuclear data library.