• Spectroscopy and Spectral Analysis
  • Vol. 42, Issue 10, 3024 (2022)
Bing-ying LEI1、*, Bo-ping XU1、1; 2;, Yi-shan WANG1、1; 2;, Xiang-ping ZHU1、1; 2;, Yi-xiang DUAN3、3;, Wei ZHAO1、1; 2;, and Jie TANG1、1; *;
Author Affiliations
  • 11. State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy Sciences, Xi'an 710119, China
  • 33. Key Laboratory of Synthetic and Natural Functional Molecule Chemistry of Ministry of Education, College of Chemistry and Materials Science, Northwest University, Xi'an 710127, China
  • show less
    DOI: 10.3964/j.issn.1000-0593(2022)10-3024-07 Cite this Article
    Bing-ying LEI, Bo-ping XU, Yi-shan WANG, Xiang-ping ZHU, Yi-xiang DUAN, Wei ZHAO, Jie TANG. Investigation of the Spectral Characteristics of Laser-Induced Plasma for Non-Flat Samples[J]. Spectroscopy and Spectral Analysis, 2022, 42(10): 3024 Copy Citation Text show less
    Schematic diagram of the experimental setup
    Fig. 1. Schematic diagram of the experimental setup
    Comparison of the time-integrated spectra under the conditions of non-flat and flat sample surfacesThe rock samples are (a) Coal stone, (b) Tourmaline, (c) Dolomite, (d) Fluorite, and (e) Limonite, respectively
    Fig. 2. Comparison of the time-integrated spectra under the conditions of non-flat and flat sample surfaces
    The rock samples are (a) Coal stone, (b) Tourmaline, (c) Dolomite, (d) Fluorite, and (e) Limonite, respectively
    The influence of laser energy on spectral peak intensity (Fe Ⅰ 404.58 nm and Fe Ⅰ 438.35 nm) under the conditions of non-flat and flat sample surfaceThe variation of (a) the spectral intensity and (b) the reduction factor with laser energy
    Fig. 3. The influence of laser energy on spectral peak intensity (Fe Ⅰ 404.58 nm and Fe Ⅰ 438.35 nm) under the conditions of non-flat and flat sample surface
    The variation of (a) the spectral intensity and (b) the reduction factor with laser energy
    Calculation of electron density and plasma temperatureStark broadening profile of Fe Ⅰ 438.35 nm under the conditions of (a) non-flat and (b) flat sample surface; (c) The variation of electron density with laser energy under the conditions of non-flat and flat sample surface; (d) The variation of the plasma temperature with laser energy under the conditions of non-flat and flat sample surface
    Fig. 4. Calculation of electron density and plasma temperature
    Stark broadening profile of Fe Ⅰ 438.35 nm under the conditions of (a) non-flat and (b) flat sample surface; (c) The variation of electron density with laser energy under the conditions of non-flat and flat sample surface; (d) The variation of the plasma temperature with laser energy under the conditions of non-flat and flat sample surface
    Wavelength
    λ/nm
    Statistical weight of
    upper level of the transitions gm
    Transition probability
    Amn/(×107 s-1)
    Energy of the upper
    level Em/cm-1
    358.121310.234 843.96
    371.99111.626 874.55
    373.48119.033 695.40
    388.6370.526 140.18
    404.5898.636 686.18
    438.35115.034 782.42
    Table 1. Spectroscopic parameters of Fe(Ⅰ) lines in limonite sample
    Bing-ying LEI, Bo-ping XU, Yi-shan WANG, Xiang-ping ZHU, Yi-xiang DUAN, Wei ZHAO, Jie TANG. Investigation of the Spectral Characteristics of Laser-Induced Plasma for Non-Flat Samples[J]. Spectroscopy and Spectral Analysis, 2022, 42(10): 3024
    Download Citation