<p>Particle identification (PID) was developed for a newly constructed <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(4\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>4</mn> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation> CsI(Tl) detector array using machine learning methods. This work presents the construction of the CsI (Tl) array, experimental setup, and the machine learning approaches employing fuzzy c-means (FCM) and support vector machine (SVM). Unlike traditional fitting methods which are typically effective only at high energies, the FCM and SVM provide robust particle identification across the full energy spectrum, thereby enhancing data quality and counting statistics in fusion evaporation experiments. Particles such as <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\upalpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">α</mi> </math></EquationSource> </InlineEquation> (<i>Z</i> = 2), <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\text {p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>p</mtext> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\text {d}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>d</mtext> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\text {t}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>t</mtext> </math></EquationSource> </InlineEquation> (<i>Z</i> = 1), as well as <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\upgamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">γ</mi> </math></EquationSource> </InlineEquation> (<i>Z</i> = 0) can be classified automatically using FCM. With dedicated training on five distinct waveforms corresponding to particles emitted from fusion evaporation reactions, the SVM demonstrates enhanced separation capability. The SVM outperforms FCM, particularly in scenarios involving weakly bound projectiles such as <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(^{7}\text {Li}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>7</mn> </mmultiscripts> <mtext>Li</mtext> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^{9}\text {Be}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>9</mn> </mmultiscripts> <mtext>Be</mtext> </mrow> </math></EquationSource> </InlineEquation>. The effectiveness of these classification models was evaluated through offline analysis using <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\upgamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">γ</mi> </math></EquationSource> </InlineEquation>-ray coincidence and particle-gating techniques. The results demonstrate that machine learning methods provide comprehensive particle identification across all energy ranges and the SVM method contributes to an approximate 50<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\%\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>%</mo> </math></EquationSource> </InlineEquation> increase in particle-gated coincidence statistics in the present experiment. The integration of machine learning in particle identification opens new possibilities for advancing nuclear-structure studies and analysis of complex reaction dynamics.</p>

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Machine learning-based particle identification in CsI(Tl) detectors: fuzzy clustering and support vector machine

  • Jun-Hong Xu,
  • Yong-De Fang,
  • Si-Cheng Wang,
  • Bing Ding,
  • Eiji Ideguchi,
  • M. Kumar Raju,
  • M. P. Carpenter,
  • Xu-Yang Wang,
  • Hong-Yi Wu,
  • Wei Hua,
  • Jian-Hong Li,
  • Zi-Hao Jia,
  • Wen Liang,
  • Song Guo,
  • Guang-Shun Li,
  • Yun-Hua Qiang,
  • Min-Liang Liu,
  • Wen-Qiang Zhang,
  • Chen-Xu Jia,
  • Ruo-Fu Chen,
  • Jie Chen,
  • Yun Zheng,
  • Cong-Bo Li,
  • Xiao-Guang Wu,
  • Min Zheng,
  • Zi-Hao Zhao,
  • Yun-Qiu Li,
  • Jin-Ze Li,
  • Rui Hong,
  • Zi-Yang He,
  • Tian-Xiao Li,
  • C. M. Petrache,
  • Xiao-Hong Zhou,
  • Zai-Guo Gan,
  • Yu-Hu Zhang

摘要

Particle identification (PID) was developed for a newly constructed \(4\pi \) 4 π CsI(Tl) detector array using machine learning methods. This work presents the construction of the CsI (Tl) array, experimental setup, and the machine learning approaches employing fuzzy c-means (FCM) and support vector machine (SVM). Unlike traditional fitting methods which are typically effective only at high energies, the FCM and SVM provide robust particle identification across the full energy spectrum, thereby enhancing data quality and counting statistics in fusion evaporation experiments. Particles such as \(\upalpha \) α (Z = 2), \(\text {p}\) p , \(\text {d}\) d and \(\text {t}\) t (Z = 1), as well as \(\upgamma \) γ (Z = 0) can be classified automatically using FCM. With dedicated training on five distinct waveforms corresponding to particles emitted from fusion evaporation reactions, the SVM demonstrates enhanced separation capability. The SVM outperforms FCM, particularly in scenarios involving weakly bound projectiles such as \(^{7}\text {Li}\) 7 Li or \(^{9}\text {Be}\) 9 Be . The effectiveness of these classification models was evaluated through offline analysis using \(\upgamma \) γ -ray coincidence and particle-gating techniques. The results demonstrate that machine learning methods provide comprehensive particle identification across all energy ranges and the SVM method contributes to an approximate 50 \(\%\) % increase in particle-gated coincidence statistics in the present experiment. The integration of machine learning in particle identification opens new possibilities for advancing nuclear-structure studies and analysis of complex reaction dynamics.