<p>The illicit trafficking of special nuclear materials (SNMs) poses a grave threat to global security and necessitates the development of effective nuclear material identification methods. This study investigated a method to isotopically identify the SNMs, including <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{233,235,238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>233</mn> <mo>,</mo> <mn>235</mn> <mo>,</mo> <mn>238</mn> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>U,<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq4.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{239-242}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>239</mn> <mo>-</mo> <mn>242</mn> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>Pu, and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{232}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>232</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Th, based on the detection of delayed <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq1.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>-rays from photofission fragments. The delayed <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq1.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 spectra resulting from the photofission of SNMs irradiated by a 14&#xa0;MeV <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq1.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 with a total of 10<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>9</mn> </mmultiscripts> </math></EquationSource> </InlineEquation> were simulated using Geant4. Three high-yield fission fragments, namely<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{138}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>138</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cs, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq11.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{89}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>89</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Rb, and <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq12.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{94}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>94</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Y, were selected as candidate fragments for SNM identification. The yield ratios of these three fragments were calculated, and the results from the different SNMs were compared. The yield ratio of <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{138}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>138</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cs/<InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq11.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{89}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>89</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Rb was used to identify most SNMs, including <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{233,235,238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>233</mn> <mo>,</mo> <mn>235</mn> <mo>,</mo> <mn>238</mn> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>U, <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq16.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{242}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>242</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Pu, and <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{232}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>232</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Th, with a confidence level above 95<InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq18.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\%\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>%</mo> </math></EquationSource> </InlineEquation>. To identify <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq19.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{239-241}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>239</mn> <mo>-</mo> <mn>241</mn> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>Pu with the same confidence, a higher total number of 10<sup>11</sup>&#xa0;<InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq1.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> beams is required. However, although the <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq12.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{94}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>94</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Y/<InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq11.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{89}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>89</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Rb ratio is suitable for elementally identifying SNMs, isotopic identification is difficult. In addition, the count rate of the delayed <InlineEquation ID="IEq23"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1725_Article_IEq1.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> above 3&#xa0;MeV can be used to rapidly detect the presence of nuclear materials.</p>

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Isotopic identification of special nuclear materials based on delayed \(\gamma\) rays from photofission fragments

  • Mei-Zhi Wang,
  • Hao-Yang Lan,
  • Di Wu,
  • Xin-Lu Xu,
  • Rui-Rui Xu,
  • Xue-Qing Yan,
  • Wen Luo

摘要

The illicit trafficking of special nuclear materials (SNMs) poses a grave threat to global security and necessitates the development of effective nuclear material identification methods. This study investigated a method to isotopically identify the SNMs, including \(^{233,235,238}\) 233 , 235 , 238 U, \(^{239-242}\) 239 - 242 Pu, and \(^{232}\) 232 Th, based on the detection of delayed \(\gamma\) γ -rays from photofission fragments. The delayed \(\gamma\) γ -ray spectra resulting from the photofission of SNMs irradiated by a 14 MeV \(\gamma\) γ beam with a total of 10 \(^{9}\) 9 were simulated using Geant4. Three high-yield fission fragments, namely \(^{138}\) 138 Cs, \(^{89}\) 89 Rb, and \(^{94}\) 94 Y, were selected as candidate fragments for SNM identification. The yield ratios of these three fragments were calculated, and the results from the different SNMs were compared. The yield ratio of \(^{138}\) 138 Cs/ \(^{89}\) 89 Rb was used to identify most SNMs, including \(^{233,235,238}\) 233 , 235 , 238 U, \(^{242}\) 242 Pu, and \(^{232}\) 232 Th, with a confidence level above 95 \(\%\) % . To identify \(^{239-241}\) 239 - 241 Pu with the same confidence, a higher total number of 1011  \(\gamma\) γ beams is required. However, although the \(^{94}\) 94 Y/ \(^{89}\) 89 Rb ratio is suitable for elementally identifying SNMs, isotopic identification is difficult. In addition, the count rate of the delayed \(\gamma\) γ above 3 MeV can be used to rapidly detect the presence of nuclear materials.