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首页> 外文期刊>Applied optics >Direct-detection Doppler wind measurements with a Cabannes-Mile lidar: A. Comparison between iodine vapor filter and Fabry-Perot interferometer methods
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Direct-detection Doppler wind measurements with a Cabannes-Mile lidar: A. Comparison between iodine vapor filter and Fabry-Perot interferometer methods

机译:使用Cabannes-Mile激光雷达直接检测多普勒测风:A.碘蒸气过滤器和Fabry-Perot干涉仪方法之间的比较

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摘要

Atmospheric line-of-sight (LOS) wind measurement by means of incoherent Cabannes-Mie lidar with three frequency analyzers with nearly the same maximum transmission of similar to 80% that could be fielded at different wavelengths is analytically considered. These frequency analyzers are (a) a double-edge Fabry-Perot interferometer (FPI) at 1064 nm (IR-FPI), (b) a double-edge Fabry-Perot interferometer at 355 nm (UV-FPI), and (c) an iodine vapor filter (IVF) at 532 nm with two different methods, using either one absorption edge, single edge (se-IVF), or both absorption edges, double edge (de-IVF). The effect of the backscattered aerosol mixing ratio, R-b, defined as the ratio of the aerosol volume backscatter coefficient to molecular volume backscatter coefficient, on LOS wind uncertainty is discussed. Assuming a known aerosol mixing ratio, R-b, and 100,000 photons owing to Cabannes scattering to the receiver, in shot-noise-limited detection without sky background, the LOS wind uncertainty of the UV-FPI in the aerosol-free air (R-b = 0), is lower by similar to 16% than that of de-IVF, which has the lowest uncertainty for R-b between 0.02 and 0.08; for R-b > 0.08, the IR-FPI yielded the lowest wind uncertainty. The wind uncertainty for se-IVF is always higher than that of de-IVF, but by less than a factor of 2 under all aerosol conditions, if the split between the reference and measurement channels is optimized. The design flexibility, which allows the desensitization of either aerosol or molecular scattering, exists only with the FPI system, leading to the common practice of using IR-FPI for the planetary boundary layer and using UV-FPI for higher altitudes. Without this design flexibility, there is little choice but to use a single wavelength IVF system at 532 ran for all atmospheric altitudes. (C) 2007 Optical Society of America.
机译:分析性地考虑了通过不相干的Cabannes-Mie激光雷达与三个频率分析仪的大气视线(LOS)风测量,该分析仪具有几乎相同的最大透射率,近似于可以在不同波长下获得的80%。这些频率分析仪是(a)1064 nm的双边缘Fabry-Perot干涉仪(IR-FPI),(b)355 nm的双边缘Fabry-Perot干涉仪(UV-FPI)和(c )用两种不同的方法在532 nm的碘蒸气滤光片(IVF)上使用一个吸收边缘(单边缘)(se-IVF),或两个吸收边缘(双IVF)。讨论了后向散射气溶胶混合比R-b(对气溶胶体积向后散射系数与分子体积向后散射系数之比)对LOS风不确定性的影响。假设已知的气溶胶混合比Rb和由于卡巴内斯散射到接收器而产生的100,000个光子,在无天空背景的散粒噪声限制检测中,无气溶胶空气中UV-FPI的LOS风不确定性(Rb = 0 ),比de-IVF低约16%,后者的Rb不确定性最低,介于0.02和0.08之间;当R-b> 0.08时,IR-FPI产生的风不确定性最低。如果优化了参考通道和测量通道之间的比例,se-IVF的风不确定性始终高于de-IVF,但在所有气溶胶条件下都小于2倍。仅FPI系统具有设计灵活性,允许对气溶胶或分子散射进行脱敏处理,这导致了将IR-FPI用于行星边界层和将UV-FPI用于更高海拔的常规做法。没有这种设计灵活性,除了在所有大气高度使用532纳米的单波长IVF系统外,别无选择。 (C)2007年美国眼镜学会。

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