• NUCLEAR TECHNIQUES
  • Vol. 47, Issue 6, 060401 (2024)
Yunchen QIAN1, Jianbin ZHOU1,*, Quanwei LIU2, Yingjie MA1..., Yi LIU1 and Xu HONG1|Show fewer author(s)
Author Affiliations
  • 1College of Nuclear Technology and Automation Engineering, Chengdu University of Technology, Chengdu 610059, China
  • 2China Nuclear Power Engineering Co., Ltd., Beijing 100840, China
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    DOI: 10.11889/j.0253-3219.2024.hjs.47.060401 Cite this Article
    Yunchen QIAN, Jianbin ZHOU, Quanwei LIU, Yingjie MA, Yi LIU, Xu HONG. Trigonometric functions-based gaussian-like shaping algorithms for nuclear signals[J]. NUCLEAR TECHNIQUES, 2024, 47(6): 060401 Copy Citation Text show less
    Comparison of trigonometry-based Gaussian-like and Gaussian pulse (Gaussian pulse: μ = 2, σ = 0.4, Gaussian-like pulse: tc = 2)
    Fig. 1. Comparison of trigonometry-based Gaussian-like and Gaussian pulse (Gaussian pulse: μ = 2, σ = 0.4, Gaussian-like pulse: tc = 2)
    Dual exponential signal (a) and Gaussian-like signal (b)
    Fig. 2. Dual exponential signal (a) and Gaussian-like signal (b)
    Cascade structure of Gaussian-like pulse shaping algorithm for a dual exponential signal
    Fig. 3. Cascade structure of Gaussian-like pulse shaping algorithm for a dual exponential signal
    Gaussian-like shaping with different shaping parameters(a) Falling edge attenuation constant τ1, (b) Rising edge attenuation constant τ2, (c) Shaping width nc
    Fig. 4. Gaussian-like shaping with different shaping parameters(a) Falling edge attenuation constant τ1, (b) Rising edge attenuation constant τ2, (c) Shaping width nc
    Impact of different nc values on frequency characteristics
    Fig. 5. Impact of different nc values on frequency characteristics
    Shaping pulses obtained by different pulse shaping algorithms
    Fig. 6. Shaping pulses obtained by different pulse shaping algorithms
    Experimental platform for energy dispersive X-ray fluorescence spectroscopy analysis based on a Fast SDD detector
    Fig. 7. Experimental platform for energy dispersive X-ray fluorescence spectroscopy analysis based on a Fast SDD detector
    Energy spectrum obtained by different pulse shaping algorithms (tube current: 15.7 μA, peaking time: 1.8 μs)(a) Sin shaping, (b) Gaussian-like shaping
    Fig. 8. Energy spectrum obtained by different pulse shaping algorithms (tube current: 15.7 μA, peaking time: 1.8 μs)(a) Sin shaping, (b) Gaussian-like shaping
    Relationship between energy resolution and peaking time for different tube flows(a) 15.7 μA, (b) 31.4 μA, (c) 78.4 μA, (d) 156.9 μA
    Fig. 9. Relationship between energy resolution and peaking time for different tube flows(a) 15.7 μA, (b) 31.4 μA, (c) 78.4 μA, (d) 156.9 μA
    Relationship between the characteristic peak area of the energy spectrum and peaking time for different tube flows(a) 15.7 μA, (b) 31.4 μA, (c) 78.4 μA, (d) 156.9 μA
    Fig. 10. Relationship between the characteristic peak area of the energy spectrum and peaking time for different tube flows(a) 15.7 μA, (b) 31.4 μA, (c) 78.4 μA, (d) 156.9 μA
    Yunchen QIAN, Jianbin ZHOU, Quanwei LIU, Yingjie MA, Yi LIU, Xu HONG. Trigonometric functions-based gaussian-like shaping algorithms for nuclear signals[J]. NUCLEAR TECHNIQUES, 2024, 47(6): 060401
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