近中红外与1.06μm和1.54μm激光兼容隐身光子晶体研究

为实现飞行器高温部分的红外与激光兼容伪装,设计了一种基于一维光子晶体的近中红外与1.06μm和1.54μm激光兼容隐身材料。基于薄膜的传输矩阵法和异质结构理论,拓展了光子晶体的禁带宽度,使之覆盖近中红外波段;随后,利用掺杂原理,在光子晶体周期结构中引入了两种缺陷。结果显示,在1~5μm的带隙中出现了波长分别为1.06μm和1.54μm的缺陷模,反射率分别为1.21%和1.79%,这种具有"光谱挖空"特性的光子晶体可以实现近中红外与1.06μm和1.54μm激光兼容隐身。     

基于小波变换及多尺度分析的星点检测方法

为提高从包含复杂天空背景的红外图像中检测出星点目标的能力,提出了一种基于小波变换及多尺度分析的星点检测算法。在对图像进行小波变换的基础上,利用多尺度分析方法,确定图像自适应阈值,实现图像小波域的去噪,达到星点目标检测的目的。实验表明,该方法能有效地检测出红外图像中的星点目标,检测能力较普通背景预测方法提高近40%。     

高性能近贴式像增强器的调制传递函数分析

为了提升微光夜视系统中高性能近贴式像增强器极限分辨力,在归纳近贴式像增强器及其部件调制传递函数模型的基础上,结合高性能超二代和超三代像增强器的结构和电参量以及典型产品性能值,研究分析了像增强器及其部件调制传递函数分布特性参数,及它们对像增强器极限分辨力和综合评价参量-信道宽度的影响.研究结果表明:进一步提升像增强器性能需要提升荧光屏的性能或改善调制传递函数分布特征;信道宽度参量可作为评价像增强器调制传递函数曲线分布特征的有效参量.研究结论对于进一步提升高性能像增强器的性能具有理论指导意义.     

p-i-nInP/In_(0.53)Ga_(0.47)As/InP探测器结构优化

利用半导体仿真工具Silvaco对p-i-n InP/In_(0.53)Ga_(0.47)As/InP近红外光探测器进行优化仿真.参考实际器件对红外探测器进行建模,并将其暗电流、光谱响应仿真结果与实验结果进行拟合,保证仿真结果的有效性.以减小探测器的暗电流为目的,优化其结构.针对探测器吸收层厚度和吸收层掺杂浓度对暗电流、光响应的影响进行研究,发现当吸收层厚度大于0.3μm后,暗电流不再上升,但光响应随着吸收层厚度的增加而增大;当吸收层掺杂浓度不断上升时,器件暗电流不断降低,当掺杂浓度上升到2×1017/cm3时,暗电流达到最低值.本文还研究了p-i-n型探测器的瞬态响应,探究了响应速度与反偏电压之间的关系,发现提高反偏电压能减小探测器响应时间.     

甚高精度星敏感器的点扩散函数检测技术

为了研制精确的星点定位误差补偿算法,得到星像轮廓面的形貌信息,研究了检测星敏感器点扩散函数(PSF)的方法。在高精度测量平台上进行光电采样,获取星像像素灰度值分布,根据扩展Nijboer-Zernike理论进行PSF拟合重建。噪声仿真实验证明,该算法能够在星像信噪比较低的情况下准确地得到Zernike系数,从而快速地重建甚高精度星敏感器的空域PSF。基本满足自动检测甚高精度星敏感器星像轮廓面的要求。     

共面线多阳极大面积光电倍增管的研制

提出了一种新型的基于共面线结构的多阳极光电倍增管(CPWMA-PMT),可实现大的工作面积、反射式光电阴极和近贴式聚焦方式。阐述了CPWMA-PMT的工作原理,分析了设计与研制中的关键问题。对所研制的CPLMA-PMT进行了参量测试,验证了在近贴聚焦工作条件下采用共面线多阳极结构的可行性,并提出了进一步的改进方向。     

Near-ultraviolet Upconversion Luminescence in CaF2∶ Yb3+, Er3 + Nanocrystals

研究了Er3+和Yb3+共掺杂的CaF2纳米材料的制备及其紫外上转换发光性质.在980 nm二极管激光器激发下,该材料可发出相对较强的紫外和绿色双色上转换发光.研究了敏化离子Yb3+以及发光中心离子Er3+掺杂量对该材料紫外上转换发光相对强度的影响,并进一步对该材料紫外上转换发光增强的可能机制进行了探讨.     

The Wigner distribution function of a super Lorentz–Gauss SLG_(11) beam through a paraxial ABCD optical system

An orthonormal beam family of super Lorentz-Gauss （SLG） beam model is proposed to describe the higher-order mode beams with high divergence, which are generated by a high power diode laser. Here we consider the simplest case of the SLG beams, where there are four mutually orthogonal SLG beams, namely SLG00, SLG01, SLG10, and SLGll beams. The SLG00 beam is just the Lorentz-Gauss beam. Based on the Collins integral formula and the Hermite-Gaussian expansion of a Lorentz function, an analytical expression for the Wigner distribution function （WDF） of an SLG11 beam through a paraxial ABCD optical system is derived. The properties of the WDF of an SLG11 beam propagating in free space are demonstrated. The normalized WDFs of an SLG11 beam at the different spatial points are depicted in several observation planes. The influence of the beam parameter on the WDF of an SLGI 1 beam in free space is analyzed at different propagation distances. The second-order moments of the WDF of an SLG11 beam in free space are also examined. This research reveals the propagation properties of an SLGll beam from another perspective. The WDFs of SLG01 and SLG10 beams can be easily obtained by using the WDFs of Lorentz-Gauss beam and the SLG11 beam.     

EVALUATION OF SINGULAR AND NEARLY SINGULAR INTEGRALS IN THE BEM WITH EXACT GEOMETRICAL REPRESENTATION＊

The geometries of many problems of practical interest are created from circular or ellip- tic arcs. Arc boundary elements can represent these boundaries exactly, and consequently, errors caused by representing such geometries using polynomial shape functions can be removed. To fully utilize the geometry of circular boundary, the non-singular boundary integral equations （BIEs） and a general nonlinear transformation technique available for arc elements are introduced to remove or damp out the singular or nearly singular proper- ties of the integral kernels. Several benchmark 2D elastostatic problems demonstrate that the present algorithm can effectively handle singular and nearly singular integrals occur- ring in the boundary element method （BEM） for boundary layer effect and thin-walled structural problems. Owing to the employment of exact geometrical representation, only a small number of elements need to be divided along the boundary and high accuracy can be achieved without increasing other more computational efforts.