Purpose <p>The methods for the determination of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(^{235}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>235</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U/<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^{238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>238</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U atom ratio are usually laborious and expensive, such as the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>/<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> spectrometry and mass spectroscopic techniques. This study proposes a less labor intensive method as the low-energy photon spectrometry technique with acceptable precision.</p> Methods <p>A methodology based on the low-energy photon spectrometry with a silicon drift detector (SDD) is developed for the determination of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(^{235}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>235</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U/<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(^{238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>238</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U atom ratio of depleted uranium samples. The SDD is well suited for measuring low-energy photons emitted from thin uranium sample source with low self-absorption, and the <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^{235}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>235</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U/<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(^{238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>238</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U atom ratio is determined by the <i>X</i>/<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray analysis with little sample preparation.</p> Results <p>The low-energy photon spectrometry employs a silicon drift detector to detect a thin piece of depleted uranium sample. The <i>X</i>/<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray peaks at 13.0, 13.3, 13.56, 15.6, 16.2, 16.78, 17.17 and 19.58&#xa0;keV are detected and analysed. By solving the equation of the peak net areas, the <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{235}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>235</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U/<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(^{238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>238</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U atom ratio is determined with the standard uncertainty less than 10.7%. The result is well consistent with the data obtained by the ICP-MS method.</p> Conclusion <p>The low-energy photon spectrometry with a silicon drift detector (SDD) is proved to be capable for the determination of <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(^{235}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>235</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U/<InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(^{238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>238</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U atom ratio by comparing with the mass spectroscopic technique result. The advantages of this method are that very little sample preparation is required and the analysis is non-destructive. To improve the accuracy of the method, the nuclear databases for <i>X</i>/<InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray of <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(^{235}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>235</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U/<InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(^{238}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>238</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>U chains should be complemented in future.</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

Determination of \(^{235}\)U/\(^{238}\)U atom ratio by low-energy photon spectrometry with a silicon drift detector

  • Hai Fei Zhang,
  • Wei Chen,
  • Wen Biao Liu,
  • Xiao Long Huang,
  • Wei Sheng,
  • Xue Mei Wang,
  • Dong Yang

摘要

Purpose

The methods for the determination of \(^{235}\) 235 U/ \(^{238}\) 238 U atom ratio are usually laborious and expensive, such as the \(\alpha \) α / \(\gamma \) γ spectrometry and mass spectroscopic techniques. This study proposes a less labor intensive method as the low-energy photon spectrometry technique with acceptable precision.

Methods

A methodology based on the low-energy photon spectrometry with a silicon drift detector (SDD) is developed for the determination of \(^{235}\) 235 U/ \(^{238}\) 238 U atom ratio of depleted uranium samples. The SDD is well suited for measuring low-energy photons emitted from thin uranium sample source with low self-absorption, and the \(^{235}\) 235 U/ \(^{238}\) 238 U atom ratio is determined by the X/ \(\gamma \) γ -ray analysis with little sample preparation.

Results

The low-energy photon spectrometry employs a silicon drift detector to detect a thin piece of depleted uranium sample. The X/ \(\gamma \) γ -ray peaks at 13.0, 13.3, 13.56, 15.6, 16.2, 16.78, 17.17 and 19.58 keV are detected and analysed. By solving the equation of the peak net areas, the \(^{235}\) 235 U/ \(^{238}\) 238 U atom ratio is determined with the standard uncertainty less than 10.7%. The result is well consistent with the data obtained by the ICP-MS method.

Conclusion

The low-energy photon spectrometry with a silicon drift detector (SDD) is proved to be capable for the determination of \(^{235}\) 235 U/ \(^{238}\) 238 U atom ratio by comparing with the mass spectroscopic technique result. The advantages of this method are that very little sample preparation is required and the analysis is non-destructive. To improve the accuracy of the method, the nuclear databases for X/ \(\gamma \) γ -ray of \(^{235}\) 235 U/ \(^{238}\) 238 U chains should be complemented in future.