• Acta Optica Sinica
  • Vol. 40, Issue 17, 1706002 (2020)
Li Wang, Yang Chen, Jianping Suo, Rui Pan, Dong Wang, Fei Gao, and Dengxin Hua*
Author Affiliations
  • Faculty of Mechanical and Precision Instrument Engineering, Xi'an University of Technology, Xi'an, Shaanxi 710048, China
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    DOI: 10.3788/AOS202040.1706002 Cite this Article Set citation alerts
    Li Wang, Yang Chen, Jianping Suo, Rui Pan, Dong Wang, Fei Gao, Dengxin Hua. Quasi Single Mode Design and Implementation of Doppler Lidar Frequency Discrimination System Based on Multimode Fiber Mach-Zehnder Interferometer[J]. Acta Optica Sinica, 2020, 40(17): 1706002 Copy Citation Text show less
    Spot distributions of different modes. (a) LP02 mode; (b) LP31 mode
    Fig. 1. Spot distributions of different modes. (a) LP02 mode; (b) LP31 mode
    Quasi-single-mode emitting spot and energy distribution curve. (a) Emitting spot; (b) energy distribution curve
    Fig. 2. Quasi-single-mode emitting spot and energy distribution curve. (a) Emitting spot; (b) energy distribution curve
    Loss curve of fundamental mode in fiber
    Fig. 3. Loss curve of fundamental mode in fiber
    Diagram of quasi single mode realization system of multimode fiber MZI
    Fig. 4. Diagram of quasi single mode realization system of multimode fiber MZI
    Output light spots after light coupling into optical fiber and propagating with different incident angles. (a) Incident angle is 0.81°; (b) incident angle is 1.43°; (c) incident angle is 2.02°
    Fig. 5. Output light spots after light coupling into optical fiber and propagating with different incident angles. (a) Incident angle is 0.81°; (b) incident angle is 1.43°; (c) incident angle is 2.02°
    Spot energy distribution of emitting light at different incident angles, and energy proportion in full width at half-maximum at different incident angles. (a) Spot energy distribution of emitting light at different incident angles; (b) energy proportion in full width at half-maximum at different incident angles
    Fig. 6. Spot energy distribution of emitting light at different incident angles, and energy proportion in full width at half-maximum at different incident angles. (a) Spot energy distribution of emitting light at different incident angles; (b) energy proportion in full width at half-maximum at different incident angles
    Output faculae at different number of disturbance mode circles when diameter of disturbance mode is 6.6 cm. (a) 0 circle; (b) 1 circle; (c) 2 circles; (d) 3 circles
    Fig. 7. Output faculae at different number of disturbance mode circles when diameter of disturbance mode is 6.6 cm. (a) 0 circle; (b) 1 circle; (c) 2 circles; (d) 3 circles
    Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 6.6 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Fig. 8. Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 6.6 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Output faculae under different number of disturbance mode circles when diameter of disturbance mode is 4.8 cm. (a) 1 circle; (b) 2 circles; (c) 3 circles
    Fig. 9. Output faculae under different number of disturbance mode circles when diameter of disturbance mode is 4.8 cm. (a) 1 circle; (b) 2 circles; (c) 3 circles
    Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 4.8 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Fig. 10. Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 4.8 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Output faculae at different number of disturbance mode circles when diameter of disturbance mode is 3.0 cm. (a) 1 circle; (b) 2 circles; (c) 3 circles
    Fig. 11. Output faculae at different number of disturbance mode circles when diameter of disturbance mode is 3.0 cm. (a) 1 circle; (b) 2 circles; (c) 3 circles
    Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 3.0 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Fig. 12. Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 3.0 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Output faculae at different number of disturbance mode circles when diameter of disturbance mode is 2.2 cm. (a) 1 circle; (b) 2 circles; (c) 3 circles; (d) 4 circles
    Fig. 13. Output faculae at different number of disturbance mode circles when diameter of disturbance mode is 2.2 cm. (a) 1 circle; (b) 2 circles; (c) 3 circles; (d) 4 circles
    Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 2.2 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Fig. 14. Normalized energy distribution curves under different number of disturbance mode circles when diameter of disturbance mode is 2.2 cm, and variation of normalized energy with number of disturbance mode circles. (a) Normalized energy distribution curves under different number of disturbance mode circles; (b) variation of normalized energy with number of disturbance mode circles
    Comparison of energy curves and normalized output energy under different disturbance mode diameters when number of disturbance mode circle is 1. (a) Energy curve comparison; (b) normalized output energy
    Fig. 15. Comparison of energy curves and normalized output energy under different disturbance mode diameters when number of disturbance mode circle is 1. (a) Energy curve comparison; (b) normalized output energy
    Comparison of energy curves and normalized output energy under different disturbance mode diameters when number of disturbance mode circles is 2, and normalized output energy. (a) Energy curve comparison; (b) normalized output energy
    Fig. 16. Comparison of energy curves and normalized output energy under different disturbance mode diameters when number of disturbance mode circles is 2, and normalized output energy. (a) Energy curve comparison; (b) normalized output energy
    Comparison of energy curves and normalized output energy under different disturbance mode diameters when number of disturbance mode circles is 3, and normalized output energy. (a) Energy curve comparison; (b) normalized output energy
    Fig. 17. Comparison of energy curves and normalized output energy under different disturbance mode diameters when number of disturbance mode circles is 3, and normalized output energy. (a) Energy curve comparison; (b) normalized output energy
    Energy proportion in full width at half-maximum under different disturbance mode diameters varies with number of disturbance mode circles
    Fig. 18. Energy proportion in full width at half-maximum under different disturbance mode diameters varies with number of disturbance mode circles
    Detection SNR of Doppler lidar system at night versus detection height
    Fig. 19. Detection SNR of Doppler lidar system at night versus detection height
    ParameterValue
    Core diameter /μm200
    Cladding outer diameter /μm220
    NA0.22
    Wavelength /nm400--900
    Splitting ratio (650 nm)50%/50%
    Table 1. Parameters of 2×2 step refractive index multimode fiber coupler (FG200UEA)
    ParameterMultimode fiber
    Core diameter /μm200
    Cladding outer diameter /μm220
    NA0.22
    Wavelength /nm190--1200
    Transmittance at 632.8 nm /%≥99.7
    Table 2. Parameters of multimode fiber (ultraviolet quartz double-cladding fiber)
    Li Wang, Yang Chen, Jianping Suo, Rui Pan, Dong Wang, Fei Gao, Dengxin Hua. Quasi Single Mode Design and Implementation of Doppler Lidar Frequency Discrimination System Based on Multimode Fiber Mach-Zehnder Interferometer[J]. Acta Optica Sinica, 2020, 40(17): 1706002
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