<p>We present new data on the <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq12.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{63}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>63</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cu(<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq13.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>, n) cross-section studied using a quasi-monochromatic and energy-tunable <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq14.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> beam produced at the Shanghai Laser Electron Gamma Source to resolve the long-standing discrepancy between existing measurements and evaluations of this cross-section. Using an unfolding iteration method, <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq15.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{63}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>63</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cu(<InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq16.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>, n) data were obtained with an uncertainty of less than 4%, and the inconsistencies between the available experimental data were discussed. The <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq17.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray strength function of <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq18.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{63}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>63</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cu(<InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq19.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>, n) was successfully extracted as an experimental constraint. We further calculated the cross-section of the radiative neutron capture reaction <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq20.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{62}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>62</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cu(n, <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq21.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>) using the TALYS code. Our calculation method enables the extraction of (n, <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2024_1631_Article_IEq22.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>) cross-sections for unstable nuclides.</p>

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New measurement of 63Cu(γ, n)62Cu cross-section using quasi-monoenergetic γ-ray beam

  • Zhi-Cai Li,
  • Zi-Rui Hao,
  • Qian-Kun Sun,
  • Yu-Long Shen,
  • Long-Xiang Liu,
  • Hang-Hua Xu,
  • Yue Zhang,
  • Pu Jiao,
  • Meng-Die Zhou,
  • Yu-Xuan Yang,
  • Sheng Jin,
  • Kai-Jie Chen,
  • Zhen-Wei Wang,
  • Shan Ye,
  • Xin-Xiang Li,
  • Chun-Wang Ma,
  • Hong-Wei Wang,
  • Gong-Tao Fan,
  • Wen Luo

摘要

We present new data on the \(^{63}\) 63 Cu( \(\gamma\) γ , n) cross-section studied using a quasi-monochromatic and energy-tunable \(\gamma\) γ beam produced at the Shanghai Laser Electron Gamma Source to resolve the long-standing discrepancy between existing measurements and evaluations of this cross-section. Using an unfolding iteration method, \(^{63}\) 63 Cu( \(\gamma\) γ , n) data were obtained with an uncertainty of less than 4%, and the inconsistencies between the available experimental data were discussed. The \(\gamma\) γ -ray strength function of \(^{63}\) 63 Cu( \(\gamma\) γ , n) was successfully extracted as an experimental constraint. We further calculated the cross-section of the radiative neutron capture reaction \(^{62}\) 62 Cu(n, \(\gamma\) γ ) using the TALYS code. Our calculation method enables the extraction of (n, \(\gamma\) γ ) cross-sections for unstable nuclides.