• Laser & Optoelectronics Progress
  • Vol. 59, Issue 10, 1018001 (2022)
Yameng Di1、2, Shuo Liu1、2, Zhenxu Bai1、2, Yanyan Deng1、2, Lü Zhiwei1、2, and Yuanqin Xia1、2、*
Author Affiliations
  • 1Center for Advanced Laser Technology, Hebei University of Technology, Tianjin 300401, China
  • 2Hebei Key Laboratory of Advanced Laser Technology and Equipment, Tianjin 300401, China
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    DOI: 10.3788/LOP202259.1018001 Cite this Article Set citation alerts
    Yameng Di, Shuo Liu, Zhenxu Bai, Yanyan Deng, Lü Zhiwei, Yuanqin Xia. Coherent Anti-Stokes Raman Scattering Microscopic Imaging of Melamine Crystals[J]. Laser & Optoelectronics Progress, 2022, 59(10): 1018001 Copy Citation Text show less
    Relationship between linear chirp parameters and glass rod length. (a) Change of chirp when glass rod length is 1-15 cm; (b) change of chirp when glass rod length is 10-13 cm
    Fig. 1. Relationship between linear chirp parameters and glass rod length. (a) Change of chirp when glass rod length is 1-15 cm; (b) change of chirp when glass rod length is 10-13 cm
    Overall design scheme of spectral focusing cars microscopic imaging system
    Fig. 2. Overall design scheme of spectral focusing cars microscopic imaging system
    Melamine CARS microscopic imaging results under different conditions. (a) Melamine CARS microscopic imaging results under time coincidence; (b) shift pump pulse imaging results; (c) shift Stokes pulse imaging results; (d) non-time zero imaging results
    Fig. 3. Melamine CARS microscopic imaging results under different conditions. (a) Melamine CARS microscopic imaging results under time coincidence; (b) shift pump pulse imaging results; (c) shift Stokes pulse imaging results; (d) non-time zero imaging results
    Microscopic imaging and Gaussian fitting curve of melamine CARS. (a) Microscopic imaging of melamine CARS; (b) Gaussian fitting curve of CARS signal in A region
    Fig. 4. Microscopic imaging and Gaussian fitting curve of melamine CARS. (a) Microscopic imaging of melamine CARS; (b) Gaussian fitting curve of CARS signal in A region
    Melamine CARs microscopic imaging results under different rotation angles of half wave plate in the pump light. (a)-(e) Imaging results corresponding to rotation angles of 0°, 20°, 40°, 60°, and 80°; (f) imaging result of maximum inhibition of non-resonant background; (g) resonance signal, non-resonant background, and ratio changes of resonance signal to non-resonant signal
    Fig. 5. Melamine CARs microscopic imaging results under different rotation angles of half wave plate in the pump light. (a)-(e) Imaging results corresponding to rotation angles of 0°, 20°, 40°, 60°, and 80°; (f) imaging result of maximum inhibition of non-resonant background; (g) resonance signal, non-resonant background, and ratio changes of resonance signal to non-resonant signal
    Melamine CARS microscopic imaging results under different rotation angles of half wave plate in Stokes light. (a)(b) Imaging results corresponding to rotation angles of 20° and 70°; (c) imaging result of maximum inhibition of non-resonant background; (d) resonance signal, non-resonant background and ratio changes of resonance signal to non-resonant signal
    Fig. 6. Melamine CARS microscopic imaging results under different rotation angles of half wave plate in Stokes light. (a)(b) Imaging results corresponding to rotation angles of 20° and 70°; (c) imaging result of maximum inhibition of non-resonant background; (d) resonance signal, non-resonant background and ratio changes of resonance signal to non-resonant signal
    Yameng Di, Shuo Liu, Zhenxu Bai, Yanyan Deng, Lü Zhiwei, Yuanqin Xia. Coherent Anti-Stokes Raman Scattering Microscopic Imaging of Melamine Crystals[J]. Laser & Optoelectronics Progress, 2022, 59(10): 1018001
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