Author Affiliations
1Key Laboratory of Atmospheric Optics Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei, Anhui 230031, China2Science Island Branch of Graduate School, University of Science and Technology of China, Hefei, Anhui 230026, China3Jiangsu Province Intelligent Optoelectronic Devices and Measurement-Control Engineering Research Center, Department of Physics and Electronic Engineering, Yancheng Teachers University, Yancheng, Jiangsu 224002, China4Advanced Laser Technology Laboratory of Anhui Province, Hefei, Anhui 230037, Chinashow less
Fig. 1. Schematic of Doppler frequency measurement principle based on triple FPI
Fig. 2. Schematic of Rayleigh-Mie Doppler lidar system based on triple FPI
Fig. 3. Photos of verification system for Doppler lidar based on triple FPI
Fig. 4. PMT output pulse signal collected by high-speed A/D acquisition card
Fig. 5. Measured original transmittance data and the corresponding fitting curve when scanning the FPI cavity length
Fig. 6. FPI transmittance curves when emitted laser/Mie and Rayleigh scattering light are incident
Fig. 7. Total wind speed measurement sensitivities when Mie or Rayleigh scattering signals are incident on FPI-1 and FPI-2
Fig. 8. Five consecutive groups of radial wind speeds in the same direction. (a) Measuring profile; (b) measuring mean and variance
Fig. 9. Radial wind speed and error in East, South, West, and North with zenith angle of 27°. (a) Radial wind speed; (b) radial wind speed error
Fig. 10. Comparison results of Doppler lidar verification system and radiosonde on the afternoon of May 12,2020. (a) Horizontal wind speed; (b) horizontal wind direction
Fig. 11. Comparison results of Doppler lidar verification system and radiosonde on the night of May 18, 2020. (a) Horizontal wind speed; (b)horizontal wind direction
Fig. 12. Horizontal wind field difference measured by two detection devices on the night of May 18, 2020. (a) Horizontal wind speed difference; (b) horizontal wind direction difference
Parameter | Value | Parameter | Value |
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Emissionsystem | Nd∶YAG laserContinuum9030 | Wavelength /nm | 532 | Receivingsystem | Triple FPIET70 | FSR /GHz | 8 | | Pulse energy /mJ | 430 | FWHM /GHz | 1 | Frequency /Hz | 30 | FPI-1 and -2peak-to-peak /GHz | 3.48 | Pulse width /ns | 4--8 | Line width /MHz | 90 | FPI-1 and -Lpeak-to-peak /GHz | 1.16 | Beam diameter /mm | 9 | Divergenceangle /mrad | 0.5 | Peak transmittance /% | >60 | Caliber /mm | 80 | Beam expander | Magnification | 10 | Filter | Wavelength /nm | 532 | Transceiveropticalsystem | Cassegraintelescope | Caliber /mm | 300 | FWHM /nm | 0.5 | Focallength /mm | 2440 | Peak transmittance /% | 70 | Beam splitter | T/R | 90/10; 50/50;30/70 | Receivingfield /mrad | 0.08 | PMT detector | Model | R9880U-20 | Opticalefficiency /% | 85 | Operating mode | AD+PC | Fiber | Core diameter /mm | 0.2(edge)/0.1(lock) | Scanner | Scan range /(°) | 360×90 | Caliber /mm | 350 | NA | 0.11 | Opticalefficiency /% | 60 | Acquisition card | Sampling rate /(GHz/MHz) | 1000/20 |
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Table 1. Design parameters of verification system for Doppler lidar based on triple FPI