多光束等倾干涉圆环的实验研究

根据多光束干涉理论,推导出等倾干涉圆环直径的计算公式,进一步得出相邻两等倾干涉圆环的直径的平方差是常数,结果与实验相符合。用Ｆａｂｒｙ Ｐｅｒｏｔ 干涉仪观察钠双线的等倾干涉圆环,操作比较复杂,难度较大,提出一种简捷的调节方法,所测的钠双线波长差值与标准值的误差很小。     

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.     

Carbon nanotubes as a support for Pt-and Pt-Ru-catalysts of reactions proceeding in fuel cells

Comparative study of two types of single-wall carbon nanotubes and standard carbon black Vulcan XC-72 as supports for catalysts of reactions proceeding in fuel cells is carried out. The nanotubes were prepared by arc method; they differed in the degree of their purifying from amorphous carbon and metal impurities. The structure and hydrophobic-hydrophilic properties of these carbon supports are studied by etalon porosimetry. The effect of the supports’ specific surface area on the deposited catalyst particles size and specific surface area is studied. The catalysts (Pt-Ru and Pt) were deposited from aqueous solutions of their salts. Platinum was also deposited by thermal decomposition of ethoxy clusters. It is shown that in methanol oxidation reaction at the Pt-Ru catalysts the current values per unit true surface area do not depend on the support nature, provided the catalyst loading is equal and the particle size is similar. When oxygen is reduced at platinum deposited onto purified nanotubes and the carbon black Vulcan XC-72, specific kinetic currents also are close to each other. It is shown that the degree of nanotubes purification and their structure affect the kinetics of this reaction significantly.     

一种高准确度光纤光栅波长解调系统

为了消除F-P滤波器的温度特性对光纤光栅波长解调系统准确度的影响,提出了一种采用F-P标准具作为波长参考计算波长的方法,设计了一种高准确度波长解调系统,并采用虚拟仪器开发平台LabWindows/CVI实现了光谱数据的滤波、寻峰及波长计算算法.测试结果表明,该系统的重复性误差小于1.56 pm,稳定性误差小于1.13 pm.     

一种机械扫描式精密相移测长方法

以相移干涉测长为应用背景,提出了一种基于“机械扫描”的相移测长方法。利用超高弹性石英材料研制出了干涉测长所需的单体3路相移装置,并利用该相移装置建成了相移测长装置,成功地将位移传感器的量值在线溯源到光学频率标准,从而实现了对3路相移的准确测量。介绍了一种引入步长控制误差的“新五幅相移”实现相位解算方法,算法准确度达到0.01%。对不确定度的定量分析结果表明,基于该机械扫描式相移技术构建的绝对长度测量系统准确度可达0.5 nm。     

复杂激光系统中平板光学元件的调频-调幅效应的研究

为了抑制大口径光学元件中的受激Brillouin散射效应,并满足打靶过程中束匀滑的要求, 目前高能激光驱动器大都采用了正弦相位调制脉冲.然而,这类脉冲在复杂激光系统中传输时, 会出现明显的调频-调幅(FM-to-AM)效应.研究这种效应的来源,对提升激光系统的整体输出性能至关重要. 对复杂激光系统中一直被人们所忽视的平板光学元件带来的FM-to-AM效应进行了理论研究和数值模拟. 数值模拟结果表明,通过平板光学元件的次数越多调制深度越大,呈线性递增趋势,当通过次数为10次时, 调制深度高达22.2%;并且平板光学元件对各谱线的过滤也各不相同,当前端选用的中心波长为1054 nm时, 平板光学对各谱线的过滤作用非常小.提出通过改变中心波长来减小FM-to-AM效应, 这对于复杂激光系统的设计具有重要的指导意义.     

在乙醇水溶液中组装三维胶体光子晶体薄膜

近几年来，用垂直沉积法制备胶体晶体得到了人们的广泛关注。用乙醇水溶液为溶剂，用垂直沉积法制备了二氧化硅胶体晶体薄膜。用这种方法一次制备的样品厚度可达20微米以上，并且将较大微球组装成了有序性较好的胶体晶体薄膜。用扫描电镜（SEM）和光学方法检测了样品的质量和厚度。     

Design of a planar,high-gain,substrate-integrated Fabry–Perot cavity antenna at terahertz frequency

This paper presents an optimum design of a substrate-integrated cavity-type antenna for use in the terahertz frequency range. The antenna was designed with a frequency-selective surface (FSS) and a planar feeding structure that are both patterned on a high-permittivity gallium-arsenide substrate. The FSS, printed on the bottom side of the substrate, is made of a circular hole array that acts as a partially reflecting mirror. Meanwhile, the planar feeding structure, printed on the top side of the substrate, is a center-fed, open-ended slotline whose ground plane acts as a perfect reflective mirror; thus, it forms a Fabry–Perot resonator. The optimized antenna produced a maximum boresight gain of 14.3 dBi, a radiation efficiency of 62%, and side-lobe levels of −15.1 dB and −15.0 dB for the E- and H-planes, respectively, at a resonance frequency of 320 GHz. The proposed design exhibits compactness, planarity, and light weight compared with the substrate lens-coupled antenna design.     

A high-finesse fiber optic Fabry–Perot interferometer based magnetic-field sensor

A high-finesse extrinsic Fabry–Perot interferometric sensor for the measurement of weak dc magnetic fields is demonstrated. The Fabry–Perot cavity is formed by aligning the fiber end-face and the TbDyFe rod end-face, and each end-face is coated by a mirror with a micro-lens. The length of the TbDyFe rod is changed by the variation of an applied dc magnetic field, leading a change of the Fabry–Perot cavity length. By interrogating the white-light interferometric spectrum, the wavelength of the resonant peak is tracked and the length of the Fabry–Perot cavity is obtained. The sensor exhibits a high sensitivity of 1510 nm/mT with a magnetic resolution of 25 nT.     

体积全息图机制的再认识

提出了一种有关体积全息图机制的新看法，与以往的布拉格衍射模型不同，认为体积全息图由法布里－珀罗干涉仪构成，多光束干涉的优点是形成体积全息图特征的基础，基于这种新看法的计算机模拟给出了非常好的反射全息图的衍射光谱。