• Acta Optica Sinica
  • Vol. 40, Issue 24, 2430002 (2020)
Weihua Huang, Chunjing He, Weiqian Zhao**, and Lirong Qiu*
Author Affiliations
  • Beijing Key Laboratory for Precision Optoelectronic Measurement Instrument and Technology, School of Optics and Photonics, Beijing Institute of Technology, Beijing 100081, China
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    DOI: 10.3788/AOS202040.2430002 Cite this Article Set citation alerts
    Weihua Huang, Chunjing He, Weiqian Zhao, Lirong Qiu. Development of Confocal LIBS Microscope[J]. Acta Optica Sinica, 2020, 40(24): 2430002 Copy Citation Text show less
    Principle of confocal LIBS imaging system
    Fig. 1. Principle of confocal LIBS imaging system
    Axial response curve for confocal LIBS imaging system
    Fig. 2. Axial response curve for confocal LIBS imaging system
    Influence of pinhole size on the spatial resolution of confocal microscope. (a) Influence of pinhole size on FWHM and signal intensity of confocal lateral response curve; (b) influence of pinhole size on FWHM and signal intensity of confocal axial response curve
    Fig. 3. Influence of pinhole size on the spatial resolution of confocal microscope. (a) Influence of pinhole size on FWHM and signal intensity of confocal lateral response curve; (b) influence of pinhole size on FWHM and signal intensity of confocal axial response curve
    LIBS spectrum collection module. (a) Collection light path of LIBS signals; (b) entrance of the collection fiber
    Fig. 4. LIBS spectrum collection module. (a) Collection light path of LIBS signals; (b) entrance of the collection fiber
    Confocal LIBS imaging system
    Fig. 5. Confocal LIBS imaging system
    Spatial resolution experimental results. (a) Axial focusing ability; (b) spatial resolution
    Fig. 6. Spatial resolution experimental results. (a) Axial focusing ability; (b) spatial resolution
    Relationship between spatial resolution and LIBS intensity. (a) Ablation craters under different energy pulse lasers; (b) ablation craters' diameter, depth, volume and LIBS intensity under different energy pulse lasers; (c) ablation craters by pulse laser at different defocus distances; (d) ablation craters' diameter, depth, volume and LIBS intensity by pulsed laser at different defocus distances
    Fig. 7. Relationship between spatial resolution and LIBS intensity. (a) Ablation craters under different energy pulse lasers; (b) ablation craters' diameter, depth, volume and LIBS intensity under different energy pulse lasers; (c) ablation craters by pulse laser at different defocus distances; (d) ablation craters' diameter, depth, volume and LIBS intensity by pulsed laser at different defocus distances
    Agate ore sample. (a) White light image of the tested sample; (b) LIBS spectrum of the tested sample (480-600 nm)
    Fig. 8. Agate ore sample. (a) White light image of the tested sample; (b) LIBS spectrum of the tested sample (480-600 nm)
    3D fusion maps. (a)CCD image; (b)-(f) 3D maps of Ba, Ti, Ca, Cu, Fe
    Fig. 9. 3D fusion maps. (a)CCD image; (b)-(f) 3D maps of Ba, Ti, Ca, Cu, Fe
    Results of pulsed energy
    Fig. 10. Results of pulsed energy
    Results of laser focusing
    Fig. 11. Results of laser focusing
    Results of pulsed energy
    Fig. 12. Results of pulsed energy
    TypeDiameterfocal lengthRadius of curvatureCenter thicknessEdge thickness
    LA472525.475.334.54.42
    LA438025.4100.346.03.82
    LA423625.4125.457.53.42
    Table 1. Parameters of three different types of plano-convex quartz lensesunit: mm
    TypeRadiusAverage radius
    A or CB
    LA4725617.8384.8501.3
    LA4380731.4650.3690.8
    LA4236901.4921.4911.4
    Table 2. RMS radius of the focus spot for three different types of plano-convex lensesunit: μm
    Weihua Huang, Chunjing He, Weiqian Zhao, Lirong Qiu. Development of Confocal LIBS Microscope[J]. Acta Optica Sinica, 2020, 40(24): 2430002
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