热稳定法拉第旋转TbYbBiIG磁光单晶及性能

采用高温溶液法，以Ｂｉ２Ｏ３／Ｂ２Ｏ３为助熔剂成功地生长出掺铋复合稀土铁石榴石（ＴｂＹｂＢｉ）３Ｆｅ５Ｏ１２（简称ＴｂＹｂＢｉＩＧ）晶体。晶体外形规则，最大尺寸为７×６×４ｍｍ３，Ｘ射线衍射分析证实，生长的晶体为ＴｂＹｂＢｉＩＧ单相单晶体，扫描电镜能谱分析其组成为Ｔｂ２．０６Ｙｂ０．４６Ｂｉ０．４８Ｆｅ５Ｏ１２。在１．０μｍ～１．７μｍ波段测量出晶体法拉第旋转谱和光吸收谱。当λ＝１．５５μｍ时，在１０°Ｃ～８０°Ｃ温度范围内测得法拉第旋转θＦ的温度系数为ｄθＦ／ｄＴ＝－２．３×１０－２ｄｅｇ·ｍｍ－１Ｋ－１。研究结果表明，ＴｂＹｂＢｉＩＧ单晶体在近红外波段θＦ约为ＹＩＧ单晶的３倍，温度系数小，是制作高性能光隔离器的一种好材料     

高山宇宙线粒子电磁簇射的研究

在海拔３２００ ｍ高山,用一台有效体积为４５×４５×１４ｃｍ３的多板云室,测量了宇宙线贯穿粒子的电磁簇射几率,传递能量范围为 ０．４－２ ＧｅＶ．获得了８０１个有用事例,得到选入的高山宇宙线粒子在 １．２５ ｃｍ厚铅层中产生电磁簇射的平均几率是［４．６２±０．７６］×１０－3 ,大于由理论和加速器实验数据推出的μ,Ρ。π±的电磁簇射几率．用统计方法对实验结果进行了分析．     

分光光度法测定烟叶中镁的研究

在ｐＨ＝ ７．０ ＮＨ４Ａｃ 缓冲介质中,苦氨酸偶氮－Ｈ－酸（ＰＨＡ）与镁反应生成２∶１ 蓝紫色络合物,λｍ ａｘ＝６３０ｎｍ ,ε＝ １．１６×１０４Ｌ·ｍ ｏｌ－ １·ｃｍ － １,镁的含量在０．５－ ４０μｇ／２５ｍ Ｌ内符合比尔定律,本方法用于烟草样品中镁的测定,结果令人满意。     

Tl—1223超导体及其复Ag带的制备

研究了用产中分熔化法制备Ｔｌ－１２２３超导体的工艺。样品的名义组成为（Ｔｌ０．５Ｐｂ０．５）（Ｓｒ０．８Ｂａ０．２）Ｃａ２Ｃｕ３Ｏｙ。经熔化退火的样品，其磁化电流的７７Ｋ和１Ｔ下大于２×１０＾４／ｃｍ＾２。用熔化－退火的超导粉作原料制得的复Ａｇ带短样，Ｊｃ达１．６－１．７×１０＾４Ａ／ｃｍ＾２（７７ｋ，０Ｔ）。采用烧结后的超导粉作原料，在制备复Ａｇ带的工艺中，如用熔化－退火的热处理制度，可以免除…     

关于地球电场,电荷和电势状况

本文根据国内外资料，讨论了地球电场、电荷和电势的状况．指出：地球与大气层间组成了一个球壳“电容器”，其电容为 １．６７Ｆ，地面带负电 ３．０ × １０５Ｃ，大气层带正电３．０×１０５Ｃ，以大气层为零电势的话，地面电势则为－ ５．０ × １０５Ｖ．地面平均场强为－ １２０Ｖ／ｍ．分析了地面与大气层间电势差稳定的原因，它们之间存在着复杂的电荷交换，但始终维持电荷分布的动态平衡．     

一种新型铂电阻温度计及其性能研究

中国计量科学研究院同云南仪表厂合作研制一种新型的套管铂电阻温度计，并对其作为较为详细的实验研究，研究结果如下：在水三相点，温度计的稳定性优于±０．３ｍＫ，在一周之内，复现性优于±０．１ｍＫ，１ｍＡ测量电流下自热不超过１ｍＫ，温度计在４．２Ｋ温度下的电阻比Ｗ小于５．９×１０＾－４，其标准偏差的绝对值不大于３×１０＾－８；而非一致性在８３Ｋ以上稍大，而在１７Ｋ－８３Ｋ间小于０．４ｍＫ，在其余温度范围均     

强激光在高Z等离子体中吸收的波长关系

利用“神光Ⅰ”输出的～５００Ｊ、１．０５μｍ，～２００Ｊ、０．５３μｍ激光和“星光Ⅱ”输出的～７０Ｊ、０．３５１μｍ激光，实验研究了激光与金圆盘靶作用产生的等离子体对激光的吸收，获得了激光１０°、４５°入射Ａｕ盘靶吸收的波长关系。实验结果与一维平面等离子体吸收模型计算的结果基本相符。     

单模光纤中Raman光放大

本文报道在单模光纤中，背向受激拉曼散射（ＢＳＲＳ）对通信光的光放大研究。所用泵浦源为声光０开关Ｎｄ￣（＋３）：ＹＡＧ激光器，工作波长１．０６４μｍ。信号源为ＩｎＧａＡｓＰ半导体激光器，工作波长１．３０μｍ。在１．３０μｍ处实现了Ｒａｍａｎ光放大，增益达１９．４ｄＢ以上，增益系数为２．３×１０￣（－１２）ｃｍ／ｗ。     

子午面大视场、孤矢面大孔径的耦合系统设计

本文提出了一套由４块柱面透镜组成的激光二极管阵列泵浦固体激光器的耦合系统，它可以将尺寸为４０ｍｍ×３．６ｍｍ的半导体激光二极管阵列的发光面所发出的子午面发散角±１０°，弧矢面发散角为±３０°的泵浦光耦合到接收面的系统可用于半导体激光二极管阵列泵浦固体激光器的研究。     

用低能电子衍射研究ⅢA—VA化合物{110}表面吸附Sb和Bi的表…

用低能电子衍射研究了Ｓｂ和Ｂｉ吸附在ＩｎＰ｛１１０｝和ＧａＡｓ｛１１０｝表面上表面结构。结果显示出：对Ｓｂ／ＩｎＰ｛１１０｝，表面原子层间距：ｄ１＝０．２７±０．２３Ａ（膨胀９．４％±０．０２Ａ）；旋转角ω１为－１０．７７°±２．２９°和ω２为１５．２６°±０．８２°；吸附键长ｌｃ１－Ａ＝２．８４±０．０５Ａ，ｌｃ２－Ｂ＝２．７５±０．０２Ａ，其键角α＝１０１．２１°±２．１°，β＝１０７．８６°     

Optimum design of aspheric collimation lenses for optical antenna system

Three kinds of aspheric collimation lenses for optical antenna have been design by optimization. The aspheric cylinder collimation lenses with aspheric surfaces (such as elliptic, hyperbolic and parabolic marginal profiles) have been researched for the semiconductor laser beam with the characteristic of dot emitting source. Based on genetic algorithm and the optimization toolbox of MTLAB, the divergence angle has been optimized. The collimation divergence angle is less than 115 μrad has been measured by laser beam analyzer. This optimum design laser beam collimation lenses as a pre-collimation system can be used for optical antenna system. And it can be widely used in modern space laser communication.     

基于伽利略结构的二级激光扩束系统的设计

针对高倍率扩束系统设计要求(即轴上和轴外像差都得到较好的校正),从三级像差理论出发,设计了一种新型的40^×高倍率激光扩束系统。该系统是基于简单的伽利略结构并通过二级扩束系统来实现的,系统包括4片透镜,通过引入2个二次非球面、 2个反射镜或1个棱镜来折叠光路。利用CODE V光学设计软件给出了该系统的光学结构参数和外形结构图,并进行了像质评价。结果表明：该系统结构简单,设计难度小,成本较低,像质好,性能优良,是一种可以被广泛采用的高倍率激光扩束系统。     

A novel prism beam-shaping laser diode bar end-pumped TEM<Subscript>00</Subscript> mode Nd:YVO<Subscript>4</Subscript> laser

A beam-shaping diode end-pumped TEM₀₀ mode CW Nd:YVO₄ laser is presented. A special beam-shaping element made up of isosceles right-angled prism pieces is adopted to realize beam symmetric. Two cylinder lenses are used to couple the shaped beam into a 3 × 3 × 9 mm Nd:YVO₄ crystal with 0.3 at % neodymium doping. By using this laser system, we have achieved 6.1 W CW laser operated in single transverse mode at 1064 nm with 95.2% reshaping efficiency and 25.6% optical-optical conversion efficiency.     

半导体激光器光波准直特性研究

分析了半导体激光器光波经准直透镜的传输特性,对影响准直光束质量的主要因素作了深入讨论,并在实验上利用小口径大数值孔径透镜获得了高准确直度的光束。     

8～12 μm波段折/衍混合反摄远系统消热差设计

设计了工作于8～12μm波段的折/衍混合消热差红外反摄远系统.该系统全视场为14°,有效焦距为100 mm,后工作距为113 mm,F/#2.0.系统采用锗和硒化锌两种材料,为三片镜结构.引入二元面和高次非球面,使结构简化,重量减轻,提高了成像质量.系统在－40℃～100 ℃的温度范围内性能稳定,适用于像元尺寸40μm,像元数640×480的现代非致冷式面阵探测器.大视场、长后工作距以及超宽工作温度范围,决定了系统可满足军用和民用领域的多种需求.     

Design and realization of active infrared imaging system based on power-over-fiber technique

We present an active infrared monitoring system based on the power-over-fiber technique. The system realizes the following main functions: the power supply via optical fibers, the laser lighting, the image acquisition and processing. In the demonstration system, the high-power laser light (at the wavelength of 808 nm) in the base station is transmitted to the remote unit via a 200-m long multi-mode fiber, whose core diameter is 200 µm. The remote unit includes an optical beam splitter, a power manager module behind a photovoltaic power converter (PPC) to ensure a quasi-maximum power-supply, a camera, a microcontroller, and an optical transmitter. As the laser beam enters the remote unit, it is divided into three parts by an optical beam splitter. The first part is converted by the PPC to provide the required electrical power of the remote unit. Besides, to improve the power-supply ability of PPC, a maximum power point tracking technique is applied, and more than 77% of PPC’s maximum output power can be obtained. The other two parts of the laser beam pass through respective beam-shaping lenses and are used directly for the infrared laser lighting. Therefore, the active infrared monitoring is achieved without extra laser lighting sources. The collected image data are transmitted via another single-mode fiber to the base station for further data processing. Experiment result shows an active and unnoticed image monitoring in the dark environment.     

新面型短程透镜的制备研究

根据解析理论新的精确公式进行设计并用单点金刚石超精切削加工制备,研制出一种优化的非球凹面短程透镜.透镜含光滑无奇点圆边,与平面连接的边缘曲率半径为无限大.样品制备在45×20×2.5mm3的LiNbO3衬底上,每片有两个孔径8mm、焦距8mm的无球差非球面短程透镜,利用670nm波长的半导体激光器端面耦合入样品一端,在另一端测得焦点光斑半宽度为2.9μm.     

Measurement of the chief ray angle of mobile phone camera

The chief ray angle (CRA) of a mobile phone lens is related to the acceptance angle of the IR cutoff filter and micro lens array. The CRA of a lens need to be within an allowed value, otherwise image blurring or vignetting occurs. However, because of the compact size of mobile phone camera lenses, it is not easy to measure the CRA accurately. In this paper, we suggest a new method to measure the CRA of high-quality mobile phone camera lenses accurately using a laser beam as a light source and a plane mirror to collimate the beam in a double pass configuration. When the plane mirror is tilted to the same angle as the lens CRA, the spot center does not change, irrespective of the longitudinal position of the plane mirror. We manufactured the reference optics, which consisted of four spherical lenses, to verify our method. We found that our new CRA measurement method has 0.65° of measurement uncertainty for 15° CRA, which satisfies phone camera makers’ requirements.     

Space-Incoherent Beam Combining of Rectangular Spot Using 18 Fiber-Transmitted Semiconductor-Laser Beams

Journal of Russian Laser Research - We report an 18×1 laser space-incoherent beam combiner with a rectangular spot used for laser heat treatment (LHT). A total of 18 semiconductor laser beams...