<p>The integration of thermal/fast neutron spectroscopy with gamma-ray detection in a single compact system remains a major challenge in radiation monitoring. Here, we present a novel dual-mode detector design based on isotopically enriched Cs<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>LiYCl<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(_6\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>6</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>:Ce (CLYC) crystals coupled to high-gain silicon photomultipliers (SiPMs). By utilizing the distinct scintillation decay characteristics of CLYC for neutrons and gamma rays, we achieved excellent particle identification performance through an optimized charge-comparison pulse shape discrimination (PSD) algorithm. The <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(^6\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>6</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Li-enriched CLYC-6 enables efficient thermal neutron detection via the <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(^6\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>6</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Li(n, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(^3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>H reaction, while the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(^7\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>7</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Li-enriched CLYC-7 exploits the <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>35</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cl(n, p)<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>35</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>S and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>35</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cl(n, <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(^{32}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>32</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>P reactions for fast neutron spectroscopy. Our CLYC-6 (95% <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^6\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>6</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Li) thermal neutron-gamma detector exhibits a gamma energy resolution of 6.52% at 662 keV, with a figure of merit (FOM) value reaching <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\sim \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>∼</mo> </math></EquationSource> </InlineEquation>3.84 for thermal neutrons. The CLYC-7 (over 99% <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(^7\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>7</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Li) fast neutron-gamma detector exhibits a gamma energy resolution of 6.73% at 662 keV, with an FOM value reaching <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\sim \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>∼</mo> </math></EquationSource> </InlineEquation>2.35 for fast neutrons; moreover, there is a good linear relationship between the fast neutron energy and the corresponding peak position in the energy spectrum. The quenching factors for protons and <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> particles are calculated to be 0.90 and 0.53, respectively, for the reactions <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>35</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cl(n, p)<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>35</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>S and <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(^{35}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>35</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Cl(n, <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(^{32}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>32</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>P. Our measurements demonstrate that the SiPM-based readout not only supports significant miniaturization but also preserves the excellent intrinsic spectral performance of CLYC. This work lays a solid experimental foundation for next-generation portable, magnetic-field-insensitive multi-mode radiation spectrometers.</p>

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High-performance neutron-gamma dual-mode spectroscopy using isotopically enriched CLYC scintillators and SiPM readout

  • Aiqin Gao,
  • Xilei Sun,
  • Guopu Qu,
  • Yangfu Wang,
  • Jun Hu,
  • Xiaoshan Jiang,
  • Tao Liu,
  • Lei Cao,
  • Hao Wei,
  • Wenjie Zhang,
  • Wenjie Li

摘要

The integration of thermal/fast neutron spectroscopy with gamma-ray detection in a single compact system remains a major challenge in radiation monitoring. Here, we present a novel dual-mode detector design based on isotopically enriched Cs \(_2\) 2 LiYCl \(_6\) 6 :Ce (CLYC) crystals coupled to high-gain silicon photomultipliers (SiPMs). By utilizing the distinct scintillation decay characteristics of CLYC for neutrons and gamma rays, we achieved excellent particle identification performance through an optimized charge-comparison pulse shape discrimination (PSD) algorithm. The \(^6\) 6 Li-enriched CLYC-6 enables efficient thermal neutron detection via the \(^6\) 6 Li(n, \(\alpha \) α ) \(^3\) 3 H reaction, while the \(^7\) 7 Li-enriched CLYC-7 exploits the \(^{35}\) 35 Cl(n, p) \(^{35}\) 35 S and \(^{35}\) 35 Cl(n, \(\alpha \) α ) \(^{32}\) 32 P reactions for fast neutron spectroscopy. Our CLYC-6 (95% \(^6\) 6 Li) thermal neutron-gamma detector exhibits a gamma energy resolution of 6.52% at 662 keV, with a figure of merit (FOM) value reaching \(\sim \) 3.84 for thermal neutrons. The CLYC-7 (over 99% \(^7\) 7 Li) fast neutron-gamma detector exhibits a gamma energy resolution of 6.73% at 662 keV, with an FOM value reaching \(\sim \) 2.35 for fast neutrons; moreover, there is a good linear relationship between the fast neutron energy and the corresponding peak position in the energy spectrum. The quenching factors for protons and \(\alpha \) α particles are calculated to be 0.90 and 0.53, respectively, for the reactions \(^{35}\) 35 Cl(n, p) \(^{35}\) 35 S and \(^{35}\) 35 Cl(n, \(\alpha \) α ) \(^{32}\) 32 P. Our measurements demonstrate that the SiPM-based readout not only supports significant miniaturization but also preserves the excellent intrinsic spectral performance of CLYC. This work lays a solid experimental foundation for next-generation portable, magnetic-field-insensitive multi-mode radiation spectrometers.