• Chinese Journal of Lasers
  • Vol. 49, Issue 6, 0611001 (2022)
Yuyin Dai1, Dan Yu2, Yinghua Li1、*, Anmin Chen3, and Mingxing Jin3
Author Affiliations
  • 1Nuclear Medicine Department, the First Bethune Hospital of Jilin University, Changchun, Jilin 130021, China
  • 2Basic Aviation College, Air Force Aviation University, Changchun, Jilin 130022, China
  • 3Institute of Atomic and Molecular Physics, Jilin University, Changchun, Jilin 130012, China
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    DOI: 10.3788/CJL202249.0611001 Cite this Article Set citation alerts
    Yuyin Dai, Dan Yu, Yinghua Li, Anmin Chen, Mingxing Jin. Effect of Different Numbers of Spatial Confinement Walls on Laser-Induced Cu Plasma Spectra[J]. Chinese Journal of Lasers, 2022, 49(6): 0611001 Copy Citation Text show less
    Schematics of LIBS experimental setup and cavities. (a) Schematic of LIBS experimental setup (M, mirror; PD, photodiode; DM,dichroic mirror; I, iris; L, lens; ICCD, intensified CCD); (b) schematics of cavities with different numbers of confinement walls (2, 3, and 4) and cavity with cylindrical confinement wall
    Fig. 1. Schematics of LIBS experimental setup and cavities. (a) Schematic of LIBS experimental setup (M, mirror; PD, photodiode; DM,dichroic mirror; I, iris; L, lens; ICCD, intensified CCD); (b) schematics of cavities with different numbers of confinement walls (2, 3, and 4) and cavity with cylindrical confinement wall
    Spectra for different numbers of confinement walls at delay time of 12.5 μs. Gate width of ICCD is 0.5 μs, and laser energy is 45 mJ. (a) Wall number is 0; (b) wall number is 2;(c) wall number is 3; (d) wall number is 4
    Fig. 2. Spectra for different numbers of confinement walls at delay time of 12.5 μs. Gate width of ICCD is 0.5 μs, and laser energy is 45 mJ. (a) Wall number is 0; (b) wall number is 2;(c) wall number is 3; (d) wall number is 4
    Time-resolved spectral intensity of Cu (I) line at 521.82 nm for different numbers of confinement walls. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Fig. 3. Time-resolved spectral intensity of Cu (I) line at 521.82 nm for different numbers of confinement walls. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Comparison of enhancement factor of Cu (I) line at 521.82 nm for different numbers of confinement walls and cylindrical confinement wall at delay time of 12.5 μs. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Fig. 4. Comparison of enhancement factor of Cu (I) line at 521.82 nm for different numbers of confinement walls and cylindrical confinement wall at delay time of 12.5 μs. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Comparison of spatially confined laser-induced Cu plasma for different numbers of confinement walls. (a) Shock wave generation; (b) shock wave reflection; (c) shock wave meets plasma; (d) shock wave compresses plasma
    Fig. 5. Comparison of spatially confined laser-induced Cu plasma for different numbers of confinement walls. (a) Shock wave generation; (b) shock wave reflection; (c) shock wave meets plasma; (d) shock wave compresses plasma
    Time-resolved signal-background ratio (SBR) of Cu (I) line at 521.82 nm for different numbers of confinement walls. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Fig. 6. Time-resolved signal-background ratio (SBR) of Cu (I) line at 521.82 nm for different numbers of confinement walls. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Time-resolved electron temperature for different numbers of confinement walls. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Fig. 7. Time-resolved electron temperature for different numbers of confinement walls. Gate width of ICCD is 0.5 μs and laser energy is 45 mJ. (a) Gain is 50; (b) gain is 70
    Wavelength /nmEm/eVgmAmn/(108 s-1)
    510.553.8240.02
    515.326.1940.60
    521.826.1960.75
    Table 1. Physical parameters of Cu (I) spectral lines[28]
    Yuyin Dai, Dan Yu, Yinghua Li, Anmin Chen, Mingxing Jin. Effect of Different Numbers of Spatial Confinement Walls on Laser-Induced Cu Plasma Spectra[J]. Chinese Journal of Lasers, 2022, 49(6): 0611001
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