• Chinese Journal of Lasers
  • Vol. 45, Issue 7, 0702006 (2018)
Jinmei Wang, Huijuan Zheng, Peichao Zheng*, and Guining Tan
Author Affiliations
  • Chongqing Municipal Level Key Laboratory of Photoelectric Information Sensing and Transmission Technology, College of Optoelectronic Engineering, Chongqing University of Posts and Telecommunications, Chongqing 400065, China
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    DOI: 10.3788/CJL201845.0702006 Cite this Article Set citation alerts
    Jinmei Wang, Huijuan Zheng, Peichao Zheng, Guining Tan. Spectral Characteristics of Coptis Chinensis Plasma Induced by Orthogonal Re-Heating Double-Pulse Laser[J]. Chinese Journal of Lasers, 2018, 45(7): 0702006 Copy Citation Text show less
    Experimental setup of orthogonal RDP-LIBS
    Fig. 1. Experimental setup of orthogonal RDP-LIBS
    Coptis Chinensis. (a) Purchased real objects; (b) samples after preparation
    Fig. 2. Coptis Chinensis. (a) Purchased real objects; (b) samples after preparation
    Spectral intensities and SBRs of four characteristic spectral lines versus detection delay. (a) Fe I; (b) CN; (c) Ca II; (d) Al I
    Fig. 3. Spectral intensities and SBRs of four characteristic spectral lines versus detection delay. (a) Fe I; (b) CN; (c) Ca II; (d) Al I
    Spectral intensities and SBRs of four characteristic spectral lines versus pulse interval under different energy groups. (a)(b) Fe I; (c)(d) CN; (e)(f) Ca II; (g)(h) Al I
    Fig. 4. Spectral intensities and SBRs of four characteristic spectral lines versus pulse interval under different energy groups. (a)(b) Fe I; (c)(d) CN; (e)(f) Ca II; (g)(h) Al I
    Spectral intensities and SBRs of four characteristic spectral lines versus pulse interval (E1=15 mJ, E2=35 mJ, T1=1.5 μs). (a) Fe I; (b) CN; (c) Ca II; (d) Al I
    Fig. 5. Spectral intensities and SBRs of four characteristic spectral lines versus pulse interval (E1=15 mJ, E2=35 mJ, T1=1.5 μs). (a) Fe I; (b) CN; (c) Ca II; (d) Al I
    Signal intensity comparison for SP-LIBS and RDP-LIBS
    Fig. 6. Signal intensity comparison for SP-LIBS and RDP-LIBS
    Boltzmann linear fitting of Ca II spectral line of Coptis Chinensis samples. (a) RDP-LIBS; (b) SP-LIBS
    Fig. 7. Boltzmann linear fitting of Ca II spectral line of Coptis Chinensis samples. (a) RDP-LIBS; (b) SP-LIBS
    Electron excitation temperature of plasma versus detection delay
    Fig. 8. Electron excitation temperature of plasma versus detection delay
    Electron number density of plasma versus detection delay
    Fig. 9. Electron number density of plasma versus detection delay
    Characteristic spectral lineEnhancement factorRSD of SP-LIBS /%RSD of RDP-LIBS /%
    Fe I 358.17 nm4.013.511.1
    CN 388.34 nm5.59.16.1
    Ca II 393.37 nm10.010.38.7
    Al I 396.15 nm3.521.011.3
    Table 1. Enhancement factor of spectral intensity and RSD for four characteristic spectral lines
    Wavelength λ/nmTransition parameterWeight factor ofup level gkTransitionprobability Aki /s-1Energy /eV
    EkEi
    317.933p64d 2D5/2→3p64p 2P3/263.6×1087.0491503.150984
    370.603p65s 2S1/2→3p64p 2P1/228.8×1076.4678753.123349
    373.693p65s 2S1/2→3p64p 2P3/221.7×1086.4678753.150984
    393.373p64p 2P3/2→3p64s 2S1/241.47×1083.1509840
    396.853p64p 2P1/2→3p64s 2S1/221.4×1083.1233490
    Table 2. Spectral parameters of Ca II spectral line used for Boltzmann fitting
    Jinmei Wang, Huijuan Zheng, Peichao Zheng, Guining Tan. Spectral Characteristics of Coptis Chinensis Plasma Induced by Orthogonal Re-Heating Double-Pulse Laser[J]. Chinese Journal of Lasers, 2018, 45(7): 0702006
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