...
首页> 外文期刊>Applied optics >Aerosol and cloud backscatter at 1.06, 1.54, and 0.53 by airborne hard-target-calibrated Nd:YAG/methane Raman lidar
【24h】

Aerosol and cloud backscatter at 1.06, 1.54, and 0.53 by airborne hard-target-calibrated Nd:YAG/methane Raman lidar

机译:机载硬目标校准的Nd:YAG /甲烷拉曼激光雷达在1.06、1.54和0.53处的气溶胶和云向后散射

获取原文
获取原文并翻译 | 示例

摘要

A lidar instrument was developed to make simultaneous measurements at three distinct wavelengths in the visible and near infrared at 0.532, 1.064, and 1.54 μm with high cross-sectional calibration accuracy. Aerosol and cloud backscatter cross sections were acquired during November and December 1989 and May and June 1990 by the NASA DC-8 aircraft as part of the Global Backscatter Experiment. The instrument, methodology, and measurement results are described. A Nd:YAG laser produced 1.064-and 0.532-p,m energy. The 1.54-μm transmitted pulse was generated by Raman-shifted downconversion of the 1.064-μm pulse through a Raman cell pressured with methane gas. The lidar could be pointed in the nadir or zenith direction from the aircraft. A hard-target-based calibration procedure was used to obtain the ratio of the system calibration between the three wavelengths, and the absolute calibration was referenced to the 0.532-μm lidar molecular backscatter cross section for the clearest scattering regions. From the relative wavelength calibration, the aerosol backscatter cross sections at the longer wavelengths are resolved for values as small as 1% of the molecular cross section. Backscatter measurement accuracies are better than l0 ↑(9)(msr) ↑(1) at l.064 and l.54 μm. Results from the Pacific Ocean region of the multiwavelength backscatter dependence are presented. Results show extensive structure and variation for the aerosol cross sections. The range of observed aerosol cross section is over 4 orders of magnitude, from less than 10 ↑(9) (m sr) ↑(1) to greater than 10 ↑(5) (m st) ↑(1). # 1997 Optical Society of America
机译:开发了一种激光雷达仪器,可以以高横截面校准精度同时在可见光和近红外中的三个不同波长下以0.532、1.064和1.54μm进行同时测量。作为全球反向散射实验的一部分,NASA DC-8飞机在1989年11月和12月以及1990年5月和1990年6月获得了气溶胶和云反向散射截面。描述了仪器,方法和测量结果。一台Nd:YAG激光器产生1.064-和0.532-p,m的能量。通过对1.064μm脉冲进行拉曼位移下转换,通过一个用甲烷气体加压的拉曼电解池产生1.54μm透射脉冲。激光雷达可以从飞机指向天底或天顶方向。使用基于硬目标的校准程序来获得三个波长之间的系统校准比率,并且绝对校准以最清晰的散射区域为参考的0.532-μm激光雷达分子背向散射截面。通过相对波长校准,可以解析较长波长的气溶胶反向散射截面,其值仅为分子截面的1%。反向散射测量精度在l.064和l.54μm处优于l0↑(9)(msr)↑(1)。给出了太平洋地区多波长反向散射依赖性的结果。结果显示气溶胶横截面的广泛结构和变化。观测到的气溶胶横截面范围超过4个数量级,从小于10↑(9)(m sr)↑(1)到大于10↑(5)(m st)↑(1)。 #1997美国眼镜学会

著录项

相似文献

  • 外文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号