Design and analysis of 532 nm Doppler wind lidar with Fabry-Perot etalon

被引:3
作者
Wang G. [1 ,2 ]
Sun D. [3 ]
Du H. [2 ]
Kang J. [4 ]
Tang L. [1 ]
Shu Z. [1 ]
Hu D. [1 ]
Xu W. [1 ]
Dong J. [1 ]
机构
[1] Key Laboratory of Atmospheric Composition and Optical Radiation, Anhui Institute of Optics and Fine Mechanics, Chinese Acad. of Sci.
[2] Artillery Academy of PLA
[3] School of Earth and Space Sciences, University of Science and Technology of China
[4] The Unit of 65553, PLA
来源
Qiangjiguang Yu Lizishu/High Power Laser and Particle Beams | 2011年 / 23卷 / 04期
关键词
Doppler shift; Fabry-Perot etalon; Mie scattering; Rayleigh scattering; Wind lidar;
D O I
10.3788/HPLPB20112304.0949
中图分类号
学科分类号
摘要
A 532 nm wind lidar system based on a tetrad Fabry-Perot(FP) etalon using steady frequency YAG laser as laser radiation source was designed. In this paper, the fundamental theory of the Doppler wind lidar is introduced, major parameters of emission system, receiver system, emission and receiver optics system and control system were presented. The parameters of the bandwidth and free spectrum range(FSR) width and the width of peak values of outboard double channels based on molecule backscattered signals are designed and analyzed, the parameters of inboard double channels based on aerosols are also designed. The velocity and signal noise ratio of the whole system is simulated. When the value of full width at half maximum is 1.75 GHz, the values of range peaks of the tetrad FPI etalon is 1.1, 1.75, 1.1 GHz, respectively, the system based on outboard double channels may be substituted for boundary atmosphere to lower troposphere wind detection by the system based on inboard double channels. The wind detection of boundary atmosphere to troposphere based on a system may be achieved.
引用
收藏
页码:949 / 953
页数:4
相关论文
共 13 条
[1]  
Gentry B., Chen H., Profiling tropospheric winds with the goddard lidar observatory for winds, Proc of the 21st Int Laser Radar Conf, (2002)
[2]  
Dehring M., Nardell C., Pavlich J., Et al., Performance and comparison of 532nm and 355nm ground winds lidars, Proc of SPIE, 489, pp. 337-347, (2003)
[3]  
Souprayen C., Garnier A., Hertzog A., Et al., Rayleigh-Mie Doppler wind lidar for atmospheric measurements: II. Mie scattering effect, theory, and calibration, Appl Opt, 38, 12, pp. 2422-2431, (1999)
[4]  
Liu Z., Wu D., Liu J., Et al., Low-altitude atmospheric wind measurement from the combined Mie and Rayleigh backscattering by Doppler lidar with an iodine filter, Appl Opt, 41, 33, pp. 7079-7086, (2002)
[5]  
Liu Z., Liu B., Wu S., Et al., High spatial and temporal resolution mobile incoherent Doppler lidar for sea surface wind measurements, Opt Lett, 33, 13, pp. 1485-1487, (2008)
[6]  
Shen F., Cha H., Sun D., Et al., Low tropospheric wind measurement with Mie Doppler lidar, Opt Rev, 15, 4, pp. 204-209, (2008)
[7]  
Shen F., Cha H., Sun D., Et al., Design and performance simulation of a molecular Doppler wind lidar, Chin Opt Lett, 7, 7, pp. 593-597, (2009)
[8]  
Mckay J.A., Modeling of direct detection Doppler wind lidar: II. The fringe imaging technique, Appl Opt, 37, 27, pp. 6487-6493, (1998)
[9]  
Korb C.L., Gentry B.M., Li S.X., Et al., Theory of the Double-Edge Technique for Doppler Lidar Wind Measurement, Appl Opt, 37, 15, pp. 3097-3104, (1998)
[10]  
Hays P.B., Killeen T.L., Kennedy B.C., The Fabry-Perot interferometer on dynamics explorer, Space Sci Instrum, 5, pp. 395-416, (1981)