Infrared and Laser Engineering, Volume. 52, Issue 12, 20230310(2023)

Quantitative analysis of coaxial zoom laser-induced breakdown spectroscopy

Xin Li1,2, Zhengyi Lv3, Bolun Cui1,2, Jiaming Zhang1, Ziying Liu1, Xun Huang1, and Tianzhuo Zhao4,5、*
Author Affiliations
  • 1Beijing Institute of Space Mechanics and Electricity, Beijing 100094, China
  • 2Beijing Aviation Intelligent Remote Sensing Equipment Engineering Technology Research Center, Beijing 100094, China
  • 3Aerospace Dongfanghong Satellite Co. Ltd., Beijing 100094, China
  • 4University of Chinese Academy of Sciences, Beijing 100049, China
  • 5Aerospace Information Research Institute, Chinese Academy of Sciences, Beijing 100094, China
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    Figures & Tables(14)
    Flowchart of zoom-LIBS correction and quantitative analysis
    Schematic of zoom-LIBS equipment
    Estimated electron density using Stark broadening of 308.22 nm
    Results of Saha-Boltzmann method
    Spectral lines involved in the estimation of V1
    Spectral lines involved in the estimation of V1 fitted by LSR
    Spectral lines involved in the estimation of V2
    • Table 1. Main elements content information in samples

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      Table 1. Main elements content information in samples

      TrainingSi/wt.%Mn/wt.%Mg/wt.%Al/wt.%
      No. 15.490.720.7291.16
      No. 26.600.520.5490.71
      No. 37.610.320.3390.55
      No. 48.290.550.5688.88
      No. 58.930.400.3989.12
      No. 610.200.260.2588.57
      No. 76.710.080.5192.07
      No. 88.400.380.3990.07
      No. 99.990.220.1288.61
      PredictionSi/wt.%Mn/wt.%Mg/wt.%Al/wt.%
      No. 109.300.620.2688.70
      No. 116.640.250.3591.65
      No. 127.410.710.7188.83
      No. 135.390.570.5691.06
    • Table 2. Electron impact factor w of Al I 308.22 nm

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      Table 2. Electron impact factor w of Al I 308.22 nm

      Plasma temperature/K$ w $/nm
      50000.00264
      100000.00261
      200000.00250
      400000.00234
    • Table 3. Al lines involved in estimating V1, V2 and Saha-Boltzmann method

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      Table 3. Al lines involved in estimating V1, V2 and Saha-Boltzmann method

      Wavelength/nmIonization degreeAccuracyAij/s−1giEi/eV Saha-BoltzmannEstimation of V1Estimation of V2
      308.22IB+5.87×10744.02YesYes-
      309.27IB+7.29×10764.02YesYes-
      265.25IB1.42×10724.67YesYes-
      256.80IB1.92×10744.83YesYes-
      257.51IC+3.60×10764.83YesYes-
      237.31IB9.07×10765.23YesYes-
      305.71I--67.67-Yes-
      232.16I--68.95-YesYes
      281.62IIA3.57×108111.82Yes-Yes
      466.31IIA+5.81×107313.26Yes--
      358.66IIA2.35×108915.30Yes--
      263.15IIB+2.48×108715.31Yes--
    • Table 4. The ratio of lines involved in the estimation of V1

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      Table 4. The ratio of lines involved in the estimation of V1

      Wavelength/nmRatioEi/eV
      308.222.414.02
      309.272.444.02
      265.252.664.67
      256.803.054.83
      257.512.824.83
      237.313.015.23
      305.714.147.69
      232.164.348.95
    • Table 5. Comparison of two plasma temperature diagnosis methods

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      Table 5. Comparison of two plasma temperature diagnosis methods

      Samples25 mJ65 mJ
      RP/eVS-B/eVRERP/eVS-B/eVRE
      No. 101.271.187.6%1.491.490
      No. 111.241.166.9%1.551.512.6%
      No. 121.191.144.4%1.521.531%
      No. 131.231.175.1%1.481.512%
    • Table 6. Correction results of spectral lines involved in quantitative analysis

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      Table 6. Correction results of spectral lines involved in quantitative analysis

      Lines25 mJ/arb. units40 mJ/arb. units
      OriginalCorrected
      Al 308.22 nm0.741.031
      Al 309.27 nm0.771.061
      Al 281.62 nm0.490.871
      Al 466.31 nm0.460.981
      Si 288.16 nm0.711.061
      Mg 279.55 nm0.621.041
      Mn 259.37 nm0.650.951
    • Table 7. Quantitative inversion results of 4 samples

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      Table 7. Quantitative inversion results of 4 samples

      LocAl/wt.%RESi/wt.%REMn/wt.%REMg/wt.%RE
      Ref88.70-9.30-0.62-0.26-
      No.101.5 m90.131.61%9.210.97%0.5511.29%0.247.69%
      2 m86.242.77%8.518.49%0.594.84%0.2311.54%
      2.4 m85.273.87%8.775.70%0.666.45%0.2911.54%
      2.7 m84.015.29%8.656.99%0.5019.35%0.3223.08%
      3 m85.423.70%8.0313.66%0.4920.97%0.3119.23%
      Ref91.65-6.64-0.25-0.35-
      No.111.5 m92.330.74%5.7713.10%0.4268.00%0.4425.71%
      2 m90.241.54%5.5716.11%0.3124.00%0.4528.57%
      2.4 m91.180.51%6.117.98%0.3540.00%0.328.57%
      2.7 m89.012.88%6.285.42%0.278.00%0.4220.00%
      3 m88.153.82%6.137.68%0.244.00%0.3911.43%
      Ref88.83-7.41-0.72-0.71-
      No.121.5 m92.273.87%7.572.16%0.788.33%0.767.04%
      2 m89.290.52%7.714.05%0.685.56%0.5719.72%
      2.4 m90.712.12%6.985.80%0.8213.89%0.732.82%
      2.7 m86.652.45%7.025.26%0.6312.50%0.8215.49%
      3 m84.145.28%7.987.69%0.711.39%0.6311.27%
      Ref91.06-5.39-0.57-0.56-
      No.131.5 m94.213.46%5.016.49%0.7226.32%0.6923.21%
      2 m93.072.21%5.183.90%0.537.02%0.518.93%
      2.4 m93.262.42%5.252.60%0.5110.53%0.7330.36%
      2.7 m87.144.30%5.174.08%0.4914.04%0.7432.14%
      3 m88.233.11%4.909.09%0.4422.81%0.7635.71%
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    Xin Li, Zhengyi Lv, Bolun Cui, Jiaming Zhang, Ziying Liu, Xun Huang, Tianzhuo Zhao. Quantitative analysis of coaxial zoom laser-induced breakdown spectroscopy[J]. Infrared and Laser Engineering, 2023, 52(12): 20230310

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    Paper Information

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    Received: May. 18, 2023

    Accepted: --

    Published Online: Feb. 23, 2024

    The Author Email: Zhao Tianzhuo (zhaotianzhuo@ucas.ac.cn)

    DOI:10.3788/IRLA20230310

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