Infrared and Laser Engineering, Volume. 52, Issue 5, 20220715(2023)

Simulation of high spectral resolution oceanic particulate carbon profile detection system

Fu Yang1... Wenhao Chen1, Yanyu Lu1 and Yan He2,* |Show fewer author(s)
Author Affiliations
  • 1College of Science, Donghua University, Shanghai 201620, China
  • 2Key Laboratory of Space Laser Communication and Detection Technolog, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
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    Figures & Tables(10)
    High spectral resolution detection principle for iodine molecular absorption cells
    Hyperspectral mode of filtering
    Flowchart of oceanographic lidar simulation system [13]
    (a) Maximum sounding depth in some waters of the Indian Ocean; (b) Maximum sounding depth in some waters of the South Pacific Ocean; (c) Maximum ocean depth estimation using space-based ocean lidar, Liu Qun et al[12]
    Scattering spectrum of interaction between laser and sea water[17]
    Variation of normalized intensity with temperature under central frequency dithering
    Schematic diagram for an HSRL return spectra
    • Table 1. Parameters of lidar

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      Table 1. Parameters of lidar

      ParameterValue
      Wavelength $ \lambda $532.2
      Lidar altitude ${ {H} }$2 000
      Pulse energy $ E $1
      Pulse repetition frequency/kHz5
      Pulse width $ \mathrm{\Delta }t $10
      Receiver effective area A/m20.031 4
      Refraction index $ n $1.35
      Transmittance of the receiver optics ${T}_{{\rm{0}}}$0.5
      Transmittance through the sea surface $ {T}_{s} $0.95
      Quantum efficiency of PMT0.1
      Dynamic range of PMT/dB50
      Overlap factor $ O $1
      Splitting ratio1∶4
    • Table 2. Characteristics of the different operating wavelengths of the shipboard detection system

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      Table 2. Characteristics of the different operating wavelengths of the shipboard detection system

      Wavelength/nmLineCenter frequency jitter range at 5‰ error of normalized intensity/MHz
      532.1985-±60
      532.24231111±30
      532.24511110±90
      532.28971105±30
      532.29281104±60
    • Table 3. Characteristics of the different operating wavelengths of the airborne detection system

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      Table 3. Characteristics of the different operating wavelengths of the airborne detection system

      Wavelength/ nm Extinction ratio/ dB FWHM/ GHz Line$ {T}_{m};{T}_{a} $Normalization intensity change (4-32 ℃) $ {T}_{m};{T}_{a} $ change (±60 MHz) Normalization intensity change (±60 MHz)
      532.198528.81.42-64.4%; 99.5%3‰17.8‰; 2.4‰3‰
      532.245130.21.28111058.5%; 99.8%2‰2.9‰; 0.8‰5‰
      532.289725.91.28110556.7%; 99.5%2‰0.7‰; 2.1‰4‰
      532.292830.91.40110460.8%; 99.8%5‰1.3‰; 0.3‰5‰
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    Fu Yang, Wenhao Chen, Yanyu Lu, Yan He. Simulation of high spectral resolution oceanic particulate carbon profile detection system[J]. Infrared and Laser Engineering, 2023, 52(5): 20220715

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    Paper Information

    Category: Laser & laser optics

    Received: Oct. 12, 2022

    Accepted: --

    Published Online: Jul. 4, 2023

    The Author Email: He Yan (heyan@siom.ac.cn)

    DOI:10.3788/IRLA20220715

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