NUCLEAR TECHNIQUES, Volume. 47, Issue 1, 010401(2024)

Flat-topped cusp-like shaper algorithm based on the unfolding-synthesis technique

Jimei LAN1, Wencheng YIN2, Yu LIU2, Tong SHEN1、*, Jinzhao ZHANG3, and Yangchun LENG1
Author Affiliations
  • 1Southwest University of Science and Technology, Mianyang 621010, China
  • 2China Nuclear Power Engineering Co., Ltd, Shenzhen 518124, China
  • 3Third Institute of Oceanography, Ministry of Natural Resources, Xiamen 361005, China
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    Figures & Tables(12)
    Transfer function model of peak pulse shaping
    Definition of the shape of a flat-top peaking pulse and its derivatives (a) Shape of the pulse h(n), where na=10, nb=20, nc=30, (b) First derivative h1(n), (c) Second derivative h2(n), (d) Third derivative h3(n)
    Parameter settings for flat-top peaking pulse shaping
    Photograph of experimental test setup
    Digital spectroscopy measurement system
    Different shaping filter effects under noise interference(a) Flat-top peaking pulse shaping, (b) Flat-top pulse shaping with a width of 0, (c) Triangular filter shaping
    Recognition performance of trapezoidal shaping and flat-top peaking shaping with the same rise time and shaping time under different pileup conditions: recognition performance at (a) Pileup level 0<l<nb, where na=40, nb=80 and nc=200, (b) Pileup level l=nb, (c) Pileup level nb<l<na+nb (color online)
    Gaussian shaping stacking identification results
    Testing performance of FPGA-based digital spectroscopy system
    • Table 1. Comparison of signal amplitude using three different methods

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      Table 1. Comparison of signal amplitude using three different methods

      输入电压

      Input voltage / mV

      输出电压Output voltage / mV

      平顶尖峰脉冲成形

      Flat-top peaking pulse shaping

      平顶宽度为0的尖峰脉冲成形

      Flat-top pulse shaping with width of 0

      三角滤波成形

      Triangular filter shaping

      4040.0740.1440.13
      4040.0040.2040.19
      4039.9239.2039.36
      4040.1940.2740.25
      4039.7839.8339.80
      4040.0340.0840.05
      4040.0740.0640.08
      4039.9239.9139.89
      4040.0240.1040.12
      4039.9739.9639.92
    • Table 2. Numerical spectrum analyzer system measurements of the characteristic peak channel address of 137Cs

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      Table 2. Numerical spectrum analyzer system measurements of the characteristic peak channel address of 137Cs

      测量时间

      Measure time / min

      第一次

      First time

      第二次

      Second time

      第三次

      Third time

      12 5522 5432 538
      52 5492 5472 548
      102 5532 5532 549
    • Table 3. Comparisons of characteristic peak count rates for 137Cs

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      Table 3. Comparisons of characteristic peak count rates for 137Cs

      方法

      Methods

      峰位计数率1

      Count rates 1 / s-1

      峰位计数率2

      Count rates 2 / s-1

      平顶尖峰脉冲成形 Flat-top peaking pulse shaping23.542 623
      三角成形 Triangular shaping24.252 487
      梯形成形 trapezoidal shaping22.362 253
      高斯成形Gaussian shaping20.521 877
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    Jimei LAN, Wencheng YIN, Yu LIU, Tong SHEN, Jinzhao ZHANG, Yangchun LENG. Flat-topped cusp-like shaper algorithm based on the unfolding-synthesis technique[J]. NUCLEAR TECHNIQUES, 2024, 47(1): 010401

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    Paper Information

    Category: Research Articles

    Received: Jul. 6, 2023

    Accepted: --

    Published Online: Mar. 7, 2024

    The Author Email: SHEN Tong (沈统)

    DOI:10.11889/j.0253-3219.2024.hjs.47.010401

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