Abstract <p>In the present work, based on a combined model of photonucleon reactions, the activities of the prospective medical isotope <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{161}\)</EquationSource> <!--BPhysMGU2570080Fursova-m3--> </InlineEquation>Tb, produced via the reactions <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{162}\)</EquationSource> <!--BPhysMGU2570080Fursova-m4--> </InlineEquation>Dy(<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--BPhysMGU2570080Fursova-m5--> </InlineEquation>,1p) and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{163}\)</EquationSource> <!--BPhysMGU2570080Fursova-m6--> </InlineEquation>Dy(<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--BPhysMGU2570080Fursova-m7--> </InlineEquation>,1n1p) at electron beam energies ranging from the reaction thresholds up to 55 MeV, were calculated. For photonuclear production of isotopes, information on the formation of by-product nuclides is also necessary, therefore the reactions <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{162}\)</EquationSource> <!--BPhysMGU2570080Fursova-m8--> </InlineEquation>Dy(<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--BPhysMGU2570080Fursova-m9--> </InlineEquation>,1n1p)<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{160}\)</EquationSource> <!--BPhysMGU2570080Fursova-m10--> </InlineEquation>Tb, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{163}\)</EquationSource> <!--BPhysMGU2570080Fursova-m11--> </InlineEquation>Dy(<InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--BPhysMGU2570080Fursova-m12--> </InlineEquation>,1p)<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{162}\)</EquationSource> <!--BPhysMGU2570080Fursova-m13--> </InlineEquation>Tb and <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{163}\)</EquationSource> <!--BPhysMGU2570080Fursova-m14--> </InlineEquation>Dy(<InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--BPhysMGU2570080Fursova-m15--> </InlineEquation>,2n1p)<InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{160}\)</EquationSource> <!--BPhysMGU2570080Fursova-m16--> </InlineEquation>Tb were studied. The calculation results indicate the feasibility of using a monoisotopic <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{162}\)</EquationSource> <!--BPhysMGU2570080Fursova-m17--> </InlineEquation>Dy target for photonuclear production of <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{161}\)</EquationSource> <!--BPhysMGU2570080Fursova-m18--> </InlineEquation>Tb at electron beam energies of 21–22 MeV, and a monoisotopic <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8830_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{163}\)</EquationSource> <!--BPhysMGU2570080Fursova-m19--> </InlineEquation>Dy target at energies of 29–30 MeV.</p>

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Theoretical Calculations of \({}^{\boldsymbol{161}}\)Tb Production on Dysprosium Isotopes

  • N. Yu. Fursova,
  • R. A. Aliev,
  • S. S. Belyshev,
  • A. A. Kuznetsov

摘要

Abstract

In the present work, based on a combined model of photonucleon reactions, the activities of the prospective medical isotope \({}^{161}\) Tb, produced via the reactions \({}^{162}\) Dy( \(\gamma\) ,1p) and \({}^{163}\) Dy( \(\gamma\) ,1n1p) at electron beam energies ranging from the reaction thresholds up to 55 MeV, were calculated. For photonuclear production of isotopes, information on the formation of by-product nuclides is also necessary, therefore the reactions \({}^{162}\) Dy( \(\gamma\) ,1n1p) \({}^{160}\) Tb, \({}^{163}\) Dy( \(\gamma\) ,1p) \({}^{162}\) Tb and \({}^{163}\) Dy( \(\gamma\) ,2n1p) \({}^{160}\) Tb were studied. The calculation results indicate the feasibility of using a monoisotopic \({}^{162}\) Dy target for photonuclear production of \({}^{161}\) Tb at electron beam energies of 21–22 MeV, and a monoisotopic \({}^{163}\) Dy target at energies of 29–30 MeV.