NUCLEAR TECHNIQUES, Volume. 47, Issue 12, 120402(2024)

Gaussian pulse shaping algorithm based on finite impulse response filters

Haixi HUANG1,2, Xu HONG1,2、*, Junlong LIU1,2, Xinru SONG1,2, Lin LI1,2, and Chengzhuo ZHOU1,2
Author Affiliations
  • 1(Applied Nuclear Technology in Geosciences Key Laboratory of Sichuan Province (Chengdu University of Technology), Chengdu 610059, China)
  • 2College of Nuclear Technology and Automation Engineering, Chengdu University of Technology, Chengdu 610059, China
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    Figures & Tables(12)
    Logic block diagram of FIR filter
    (a) Process of quantizing hs[n], (b) Schematic diagram of quantized Gaussian pulse shaping impulse response signal ĥs[n]
    Comparison of hs[n] before and after quantization (a), shaped pulse (b) and frequency-domain characteristics (c) of GPS under different quantization accuracies (color online)
    Shaped pulses (a~c) and amplitude-frequency characteristics (d~f) of GPS under different additional truncation parameters (a, d) Δnl=Δn, Δnr=0; (b, e) Δnl=0, Δnr=Δn; (c, f) Δnl=Δn, Δnr=Δn
    Shaped pulses for different values of Δnr at Δnl =33
    Shaping pulse (a~c) and amplitude-frequency characteristics (d~f) of truncated GPS and normal GPS with different peaking times
    Block diagram of digital multichannel analyzer architecture
    Energy spectra of Gaussian pulse shaping at the peaking time of 780 ns with different quantization accuracies
    Peak area (a) and energy resolution (b) of the Mn Kα peak of GPS with different quantization accuracies
    Peak area (a) and energy resolution (b) of the Mn Kα peak of three shaping methods with different peaking times
    • Table 1. Characteristics of filter coefficient sequences under different peaking times and quantization accuracies

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      Table 1. Characteristics of filter coefficient sequences under different peaking times and quantization accuracies

      达峰时间

      Peaking time / ns

      量化精度

      Quantization accuracyQ / bits

      NlNrM
      1202-5410
      4-6512
      8-8716
      16-10920
      2402-8716
      4-111022
      8-151430
      16-201940
      4202-151430
      4-201940
      8-262552
      16-353470
      6002-191737
      4-272553
      8-363572
      16-5049100
      7802-231943
      4-333165
      8-464592
      16-6463128
      9602-333064
      4-444287
      8-5958118
      16-8179161
      1 1402-383372
      4-5149101
      8-7068139
      16-9594190
    • Table 2. Characteristics of the filter coefficient sequence after introducing additional truncation at different peaking times

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      Table 2. Characteristics of the filter coefficient sequence after introducing additional truncation at different peaking times

      原始达峰时间

      Initial peaking time / ns

      截断后成形脉冲达峰时间

      Peaking time after truncation / ns

      ΔnlΔnrM
      240120131215
      420240222028
      600420282448
      780600332768
      960780403190
      1 1409604535110
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    Haixi HUANG, Xu HONG, Junlong LIU, Xinru SONG, Lin LI, Chengzhuo ZHOU. Gaussian pulse shaping algorithm based on finite impulse response filters[J]. NUCLEAR TECHNIQUES, 2024, 47(12): 120402

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    Paper Information

    Category: NUCLEAR ELECTRONICS AND INSTRUMENTATION

    Received: Mar. 21, 2024

    Accepted: --

    Published Online: Jan. 15, 2025

    The Author Email: HONG Xu (HONGXu)

    DOI:10.11889/j.0253-3219.2024.hjs.47.120402

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