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基于激光掩星吸收光谱的二氧化碳探测技术

王玉诏 陶宇亮 孙海青 杨超

王玉诏, 陶宇亮, 孙海青, 杨超. 基于激光掩星吸收光谱的二氧化碳探测技术[J]. 中国光学(中英文), 2021, 14(3): 634-642. doi: 10.37188/CO.2020-0201
引用本文: 王玉诏, 陶宇亮, 孙海青, 杨超. 基于激光掩星吸收光谱的二氧化碳探测技术[J]. 中国光学(中英文), 2021, 14(3): 634-642. doi: 10.37188/CO.2020-0201
WANG Yu-Zhao, TAO Yu-Liang, SUN Hai-Qing, YANG Chao. Carbon dioxide detection technology based on the laser occultation absorption spectrum[J]. Chinese Optics, 2021, 14(3): 634-642. doi: 10.37188/CO.2020-0201
Citation: WANG Yu-Zhao, TAO Yu-Liang, SUN Hai-Qing, YANG Chao. Carbon dioxide detection technology based on the laser occultation absorption spectrum[J]. Chinese Optics, 2021, 14(3): 634-642. doi: 10.37188/CO.2020-0201

基于激光掩星吸收光谱的二氧化碳探测技术

基金项目: 民用航天十三五预研项目资助(No. D040105)
详细信息
    作者简介:

    王玉诏(1984—),男,河北南宫人,博士,高级工程师,2011年于北京理工大学获得工学博士学位,主要研究领域为激光雷达、激光遥感. E-mail:zz0525wyz@163.com

  • 中图分类号: P407.5, P412.27

Carbon dioxide detection technology based on the laser occultation absorption spectrum

Funds: Supported by Civil Aerospace 13 th Five-Year Pre-research Project (No. D040105)
More Information
  • 摘要: 本文分析了固定波长激光掩星差分吸收技术的优点和不足,介绍了可调谐激光直接吸收光谱技术测量原理。分析了最优波长透过率与信噪比的关系以及测量误差与背景光干扰的关系。根据高灵敏度探测器的工作波长范围,选择了6310.915 cm−1、6310.893 cm−1、6310.890 cm−1、6310.8834 cm−1作为吸收的工作波长,同时选择6310.15 cm−1作为参考波长,并对各波长的探测能力进行了仿真分析。通过仿真结果可知,在1 km垂直分辨率下,在5~35 km内CO2浓度探测误差优于0.9%,7~42 km范围内的探测误差优于0.4%。该技术降低了系统成本和复杂度,有利于星载产品的设计和实现。

     

  • 图 1  直接吸收光谱激光掩星探测原理

    Figure 1.  Detection principle of laser occultation direct absorption spectroscopy

    图 2  信噪比SNR与透过率关系

    Figure 2.  The relationship of SNR and transmission T

    图 3  (a)背景光谱与(b)CO2光谱对比(波数ν范围5882 cm−1~7143 cm−1,高度5 km)

    Figure 3.  Comparison of (a) background spectrum and (b) CO2 spectrum (The range of wave number ν is 5882 cm−1~7143 cm−1 and the height is 5 km.)

    图 4  背景光谱干扰误差

    Figure 4.  Error caused by background spectral interference

    (λon is 6310.915 cm−1 @ 5~10 km, 6310.893 cm−1 @ 11~18 km, 6310.890 cm−1 @ 19~26 km, 6310.8834 cm−1 @ 27~39 km, and λoff is 6310.15 cm−1)

    图 5  探测信噪比仿真结果

    Figure 5.  Simulation results of detection SNR

    图 6  累积次数的高度分布

    Figure 6.  Height distribution of cumulative times

    图 7  探测误差随高度分布

    Figure 7.  Distribution of detection error varying with height

    表  1  系统仿真参数

    Table  1.   System simulation parameters

    System parameterValueUnit
    Orbit altitude of laser transmitter500km
    Orbit altitude of laser receiver600km
    repetition rate40Hz
    Laser power1W
    Laser wavenumber6309.8834~6311.8834cm−1
    Absorption wavenumber6310.915@5~10 km, 6310.893@11~18 km,
    6310.890@19~26 km, 6310.8834 @27~39 km
    cm−1
    Reference wavenumber6310.15cm−1
    Laser line width10MHz
    Laser beam divergence0.3mrad
    Telescope diameter0.3m
    System optical efficiency0.51
    Detector responsivity (InGaAs-APD,
    C30662, 1584.6 nm)
    10.3A/W
    Nominal gain101
    Noise factor5.51
    Dark current45nA
    Spectral noise current0.7pA/rt (Hz)
    Bandwidth3000Hz
    下载: 导出CSV
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出版历程
  • 收稿日期:  2020-12-28
  • 修回日期:  2021-01-08
  • 网络出版日期:  2021-03-27
  • 刊出日期:  2021-05-14

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