• Chinese Optics Letters
  • Vol. 19, Issue 5, 052701 (2021)
Ahui Hou1、2、*, Yihua Hu1、2、**, Nanxiang Zhao1、2, Jiajie Fang1、2, Shilong Xu1、2, and Quan Zhou1、2
Author Affiliations
  • 1State Key Laboratory of Pulsed Power Laser Technology, National University of Defense Technology, Hefei 230037, China
  • 2Anhui Provincial Key Laboratory of Electronic Restriction, National University of Defense Technology, Hefei 230037, China
  • show less
    DOI: 10.3788/COL202119.052701 Cite this Article Set citation alerts
    Ahui Hou, Yihua Hu, Nanxiang Zhao, Jiajie Fang, Shilong Xu, Quan Zhou. Full-waveform fast correction method for photon counting Lidar[J]. Chinese Optics Letters, 2021, 19(5): 052701 Copy Citation Text show less
    Waveform distortion among the pulse laser, photon, and corrected waveforms.
    Fig. 1. Waveform distortion among the pulse laser, photon, and corrected waveforms.
    Comparison with Xu et al.’s method. (a) Correlation distance versus the intensity; (b) time cost versus the width of the time bin.
    Fig. 2. Comparison with Xu et al.’s method. (a) Correlation distance versus the intensity; (b) time cost versus the width of the time bin.
    Description of the photon counting system. (a) Schematic diagram: the components are a semiconductor laser source, a GM-APD detector, a TCSPC system, and the optical system. The optical system contains a beam splitter (BS), PIN fast photodiode, optical attenuation system (OAS), beam expansion (BE), telescope, bandpass filter (BPF), and fiber coupling receiver (FCR); (b) photograph of the experiment system.
    Fig. 3. Description of the photon counting system. (a) Schematic diagram: the components are a semiconductor laser source, a GM-APD detector, a TCSPC system, and the optical system. The optical system contains a beam splitter (BS), PIN fast photodiode, optical attenuation system (OAS), beam expansion (BE), telescope, bandpass filter (BPF), and fiber coupling receiver (FCR); (b) photograph of the experiment system.
    Photon waveform, which is the statistical histogram from multiple cumulative detections of TCSPC and corrected waveform when (a) Ns=0.04 and (b) Ns=0.6. The blue line and the green line are the fitting curves of the photon waveform and the correction waveform, respectively.
    Fig. 4. Photon waveform, which is the statistical histogram from multiple cumulative detections of TCSPC and corrected waveform when (a) Ns=0.04 and (b) Ns=0.6. The blue line and the green line are the fitting curves of the photon waveform and the correction waveform, respectively.
    Correlation distance versus the average number of photons.
    Fig. 5. Correlation distance versus the average number of photons.
    Photon waveforms and correction waveforms of depth targets with (a) Ns=0.02 and (b) Ns=0.5 at Kl=1.4.
    Fig. 6. Photon waveforms and correction waveforms of depth targets with (a) Ns=0.02 and (b) Ns=0.5 at Kl=1.4.
    Photon waveforms and correction waveforms of depth targets with (a) Ns=0.04 and (b) Ns=0.27 at Kl=0.93.
    Fig. 7. Photon waveforms and correction waveforms of depth targets with (a) Ns=0.04 and (b) Ns=0.27 at Kl=0.93.
     Ns0.040.180.390.620.891.10
    RCUncorrected (102)0.050.090.581.984.116.61
    Corrected (102)0.0120.0140.0420.2200.6201.540
    Time cost (103s)0.370.390.420.360.430.38
    Table 1. Comparison of Correction Effects with Different Echo Photon Numbers
    Ahui Hou, Yihua Hu, Nanxiang Zhao, Jiajie Fang, Shilong Xu, Quan Zhou. Full-waveform fast correction method for photon counting Lidar[J]. Chinese Optics Letters, 2021, 19(5): 052701
    Download Citation