Accuracy Analysis of the Fabry–Perot Etalon Based Doppler Wind Lidar

A direct detection Doppler wind lidar with the dual Fabry–Perot technique has been built in Hefei, China, and the system is described in this paper. A dual, air-spaced Fabry–Perot etalon is designed as the frequency discriminator and the transmission characteristics are measured with a stabilized cw laser and a pulse laser. The experimental data are found to be in agreement with the designed parameters. The Doppler shift is measured by taking the ratio of the transmitted intensities from the dual etalon. Analysis of the accuracy of Doppler measurement is made by considering the factors of the number of iterations in converting the measured ratio to the Doppler shift, the laser intensity fluctuation and the signal-to-noise ratio. In the sufficient signal-to-noise ratio the velocity accuracy of the Doppler lidar system is estimated to be better than 0.5 m/s.     

塞曼效应实验系统评述

对塞曼效应实验系统各环节的作用、要求和关键作了分析和评述，指出了安排实验中应注意的问题，提出了观察不同谱线塞曼效应的建议．     

Measurement of absorption spectra for atmospheric methane by a lidar system with tunable emission wavelength in the range 1.41–4.24 μm

We have developed, built, and tested an automated differential lidar system for measuring low concentrations of atmospheric gases, based on an optical parametric oscillator tunable in the near IR region. We have calculated the spectral shift of the relative intensities of the individual lines in the ν₃ absorption band of methane. In comparing the measured and calculated spectra, we did not observe any shifts in the ν₃ absorption band of methane. At the same time, in the experimental spectra we observe broadening of the Q branch and the individual lines of the P branch. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 76, No. 2, pp. 285–290, March–April, 2009.     

薄膜多腔滤光片型梳状滤波器的设计

介绍了一种通过使用多个薄膜法布里—珀罗滤光片的叠加来实现密集波分复用中使用的梳状滤波器的设计的新方法。采用间隔层为熔融石英的薄膜法布里—珀罗滤光片作为基本结构的光学梳状滤波器可以比较容易地控制各腔的厚度,因而能精确地达到波分复用系统中波长间隔非常窄的要求。分析了如何确定间隔层厚度和各法布里—珀罗腔的反射镜的反射率以及它们之间的匹配问题,最后给出了与设计吻合较好的实验结果,制作的梳状滤波器在C波段的信道间隔为100GHz,相邻通道窜音小于-24dB,最小插入损耗约-0．4dB。     

用标准具测量微小频移的方法研究

针对光学系统表面反射激光和水中受激布里渊散射光通过F-P标准具后所形成的干涉环簇图样,提出了三种计算布里渊频移的方法,即小角度微分法、小角度差值法和环间距比例法。分别对其进行了理论推导,得出了相应的解析表达式,并通过实验进行了验证。使用这三种方法得出的结果分别为8.65GHz,8GHz和7.2GHz,其中由环间距比例法得出的结果与水中布里渊散射频移的理论值7.5GHz符合得最好。通过与已有方法进行比较,结果表明与环间距比例法相差1MHz。分析了各种方法的优缺点以及适用情况和条件。     

塞曼效应测光速实验中影响精度的因素分析

通常情况下该实验用以对电子的荷质比进行测量。笔者发现,如果进行逆向构思,把电子的荷质比作为已知量时,可重新进行理论推导从而得到真空中的光速值。基于该理论基础重新设计塞曼效应试验,就可以得到测量光速的一种新方法。本文主要就采用这一方法测光速时,对影响测量精度的主要因素进行了分析。     

Temperature–Light Dual‐Responsive Au@PNIPAm Core‐Shell Microgel‐Based Optical Devices

Au nanoparticle (AuNP) core particles coated with a poly(N‐isopropylacrylamide) (pNIPAm) shell (Au@pNIPAm) are synthesized by seed mediated free radical polymerization. Subsequently, a temperature–light‐responsive photonic device is fabricated by sandwiching the Au@pNIPAm particles between two thin layers of Au. The optical device exhibits visual color and characteristic multipeak reflectance spectra, where peak position is primarily determined by the distance between two Au layers. Dual responsivities of the photonic device are achieved by combining the photothermal effect of AuNPs core (localized surface plasmon resonance (LSPR) effect) and the temperature responsivity of the pNIPAm shell. That is, the pNIPAm shell collapses as the temperature is increased above pNIPAm's lower critical solution temperature, either by direct heat input or heat generated by AuNPs' LSPR effect. To investigate the effect of AuNPs distribution in the microgels on the devices' photothermal responsivity, the Au@pNIPAm microgel‐based etalon devices are compared with that fabricated by AuNP‐doped pNIPAm‐based microgels; in terms of response kinetics and optical spectrum homogeneity. The uniform Au@pNIPAm microgel‐based devices show a fast response and exhibit a comparatively homogeneous spectrum over the whole slide. These materials can potentially find use in drug delivery systems, active optics, and soft robotics.     

Gires-Tournois干涉镜补偿色散的自启动飞秒Cr4+:YAG激光器实验研究

利用一片GTI镜补偿腔内色散,并使用宽带半导体可饱和吸收片,实现了锁模自启动的飞秒Cr⁴⁺:YAG激光输出.在9W平均功率的1030nm激光抽运下,获得输出脉冲功率为95 mW,光谱半高全宽45 nm,中心波长1508 nm,实测脉冲宽度为65 fs.     

光纤光栅径向受力检测技术

对光纤布喇格光栅径向受力特性进行了理论与实验研究,给出了光纤布喇格光栅的径向受力灵敏度,并利用可调F-P标准具设计了一套解调光纤布喇格光栅反射峰劈裂值的实验系统.此系统消除了外界环境对F-P标准具初始腔长的干扰所引起的误差,系统的准确度达到了0.02 nm.     

正反馈选模和调Q技术

把一个由GaAs光电导开关和激光腔中的普克尔盒组成的正反馈回路,用于YAG激光器中,选单纵模和调Q,获得了稳定可靠的单纵模调Q脉冲.