• Chinese Journal of Quantum Electronics
  • Vol. 41, Issue 4, 578 (2024)
FU Xiaoqing1,*, WANG Jingge1, DAI Bo1, LIANG Fangyuan1, and LIU Jiaxin2
Author Affiliations
  • 1School of Physics and Engineering, Henan University of Science and Technology, Luoyang 471023, China
  • 2No.5715 Factory, People's Liberation Army, Luoyang 471000, China
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    DOI: 10.3969/j.issn.1007-5461.2024.04.002 Cite this Article
    Xiaoqing FU, Jingge WANG, Bo DAI, Fangyuan LIANG, Jiaxin LIU. Spectral characteristics of laser induced breakdown spectroscopy based on cylindrical focusing lens[J]. Chinese Journal of Quantum Electronics, 2024, 41(4): 578 Copy Citation Text show less
    Schematic of the experimental setup
    Fig. 1. Schematic of the experimental setup
    Topography of laser ablation craters generated by spherical lens focusing (a) and cylindrical lens focusing (b)
    Fig. 2. Topography of laser ablation craters generated by spherical lens focusing (a) and cylindrical lens focusing (b)
    Comparison of characteristic emission spectra between cylindrical lens and spherical lens LIBS of alloy steel samples
    Fig. 3. Comparison of characteristic emission spectra between cylindrical lens and spherical lens LIBS of alloy steel samples
    Variation of spectral line intensity and relative standard deviation (RSD) with the number of ablation. (a) Signal intensity of Mn I: 403.08 nm; (b) Signal intensity of Mn II: 259.37 nm; (c) Background intensity of Mn I: 403.08 nm;(d) Background intensity of Mn II: 259.37 nm
    Fig. 4. Variation of spectral line intensity and relative standard deviation (RSD) with the number of ablation. (a) Signal intensity of Mn I: 403.08 nm; (b) Signal intensity of Mn II: 259.37 nm; (c) Background intensity of Mn I: 403.08 nm;(d) Background intensity of Mn II: 259.37 nm
    Boltzmann plots under spherical lens focusing and cylindrical lens focusing (a) and stability comparison of plasma temperature (b)
    Fig. 5. Boltzmann plots under spherical lens focusing and cylindrical lens focusing (a) and stability comparison of plasma temperature (b)
    Lorentz fitting of Fe I atomic spectral lines under spherical lens focusing and cylindrical lens focusing (a) and stability comparison of the corresponding electron density (b)
    Fig. 6. Lorentz fitting of Fe I atomic spectral lines under spherical lens focusing and cylindrical lens focusing (a) and stability comparison of the corresponding electron density (b)
    Calibation plots obtained for Mn (a), Cr (b) and Ni (c) elements in alloy steel
    Fig. 7. Calibation plots obtained for Mn (a), Cr (b) and Ni (c) elements in alloy steel
    SampleMn / %Cr / %Ni / %
    1#0.5032.461.76
    2#0.2430.864.40
    3#0.931.430.108
    4#1.330.2782.66
    5#2.11.831.03
    6#1.323.160.35
    Table 1. Standard mass content percentage of Mn, Cr and Ni in alloy steel samples
    Wavelength/nmAki/ (107s-1)Ek/eVgk
    306.723.124.9557
    344.061.713.6037
    355.4914.006.31913
    360.678.296.12913
    361.887.224.4157
    385.990.973.2109
    Table 2. Spectroscopic parameters of Fe I used in temperature calculation by Boltzmann plot
    Species

    σB× 10-3

    (spherical)

    σB × 10-3

    (cylindrical)

    CLOD × 10-2

    (spherical)

    CLOD × 10-2

    (cylindrical)

    CLOD (spherical) / CLOD (cylindrical)
    Mn3.901.306.181.544.01
    Cr8.504.108.043.572.25
    Ni8.304.3027.312.72.15
    Table 3. Comparison of CLOD between spherical lens focus and cylindrical lens focus LIBS for different elements
    Xiaoqing FU, Jingge WANG, Bo DAI, Fangyuan LIANG, Jiaxin LIU. Spectral characteristics of laser induced breakdown spectroscopy based on cylindrical focusing lens[J]. Chinese Journal of Quantum Electronics, 2024, 41(4): 578
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