不同激光分布下Nd∶GdVO4晶体热焦距分析

为了研究方形激光晶体Nd∶GdVO4在超高斯泵浦光分布下的热效应,采用半解析的分析方法,进行了理论分析和实验验证.结果表明：当使用输出功率为15 W的半导体激光器端面中心入射时,在抽运端面中心获得1.38 μm最大热形变量（超高斯阶次为2时）和220 mm的热焦距（超高斯阶次为5时）.     

New test and analysis of position-sensitive-silicon-detector

We have tested and analyzed the properties of two-dimensional Position-Sensitive-silicon-Detector （PSD） with new integrated preamplifiers. The test demonstrates that the best position resolution for 5.5 MeV α particles is 1.7 mm （FWHM）, and the best energy resolution is 2.1%, which are notably better than the previously reported results. A scaling formula is introduced to make the absolute position calibration.     

Studies of closed orbit correction and slow orbit feedback for the SSRF storage ring

Details of the active ways to suppress Closed Orbit Distortion （COD）, including bending magnet sorting and survey and alignment of the magnets, are discussed based on the studies of affections to the COD by the bending magnet field error and the misalignment of quadrupoles. The closed orbit correction and the Slow Orbit Feed Back （SOFB） system for the SSRF storage ring are presented in this paper. With these available methods, better results were obtained during the commissioning period with 3 GeV beam energy.     

一种基于畸变等效曲面的图像畸变校正

介绍了一种图像畸变的等效曲面模型,用于修正由于光学系统或图像传感器产生的畸变。分析了球形畸变模型的原理,推导出基于球形模型的畸变校正公式,并给出了基于球形模型的畸变校正的具体实现方法,通过实验对这种畸变校正的效果进行了验证。这种曲面畸变模型的校正具有实现简单,不需求解方程组等优点,并可以推广到其他曲面,具有比较广泛的实用性。     

斯特林制冷机驱动控制源电磁兼容分析与改进

介绍了斯特林制冷机驱动控制源的分类,讨论了不同的驱动方式对探测芯片产生的干扰形式,并给出了驱动控制源采取的改进措施.并对驱动控制源与斯特林制冷机联机实验所产生的干扰情况进行了分析,介绍了驱动控制源采取的有效改进措施.     

一种数字摄录一体机的畸变校准方法

畸变是评价光学成像系统像质的一个重要参数。在建立系统的畸变数学模型的基础上,利用计算机辅助方法,通过精确定位被测CCD摄录一体机光学中心的位置,由被测系统采集高精度目标靶的图像,并对数字图像进行处理,实现了对CCD摄录一体机畸变的测量。通过软件对系统进行畸变校正,可使被测系统的畸变测量的相对不确定度达到了0.11%。畸变校正技术可用于电视制导、航空测绘、飞船交汇对接等方面。     

水平场景无畸变折反射全景成像系统透镜畸变的消除

采用短焦距透镜设计水平场景无畸变折反射全景成像系统,会使系统更加小型化,然而短焦距透镜的畸变会对系统成像产生影响。为此建立了具有径向畸变的相机模型;根据这一相机模型,研究了采用短焦距摄像头的水平场景无畸变折反射全景成像系统中,透镜畸变对系统成像的影响,结果表明短焦距透镜的畸变会对系统成像产生严重影响;为了消除透镜畸变的影响,对反射镜的设计进行了改进,在反射镜面形微分方程中包含了透镜畸变消除的参量;按新的方法,设计了一套由短焦距摄像头组成的水平场景无畸变折反射全景成像系统。     

大视场多CCD拼接相机标定方法研究

介绍了一种多CCD拼接弹道相机的标定方法和步骤,以及标定系统的原理及组成。对相机的光学畸变和大视场拼接物像几何投影关系进行了分析,建立了相机数学模型,并采用最小二乘多元回归分析方法,通过测量相机的内方位元素计算畸变系数,确定了最佳条件下相机数学模型中的各个参数。实验表明利用该方法标定出相机精度方位角测角误差小于10″,高低角测角误差小于15″。     

Emissive or Nonemissive? A Theoretical Analysis of the Phosphorescence Efficiencies of Cyclometalated Platinum(II) Complexes

We herein report a theoretical analysis based on a density functional theory/time‐dependent density functional theory (DFT/TDDFT) approach to understand the different phosphorescence efficiencies of a family of cyclometalated platinum(II) complexes: [Pt(NCN)Cl] ( 1 ; NCN=1,3‐bis(2‐pyridyl)phenyl^?), [Pt(CNN)Cl] ( 2 ; CNN=6‐phenyl‐2,2′‐bipyridyl^?), [Pt(CNC)(CNPh)] ( 3 ; CNC=2,6‐diphenylpyridyl^2?), [Pt(R‐CNN)Cl] ( 4 ; R‐CNN=3‐(6′‐(2′′‐naphthyl)‐2′‐pyridyl)isoquinolinyl^?), and [Pt(R‐CNC)(CNPh)] ( 5 ; R‐CNC=2,6‐bis(2′‐naphthyl)pyridyl^2?). By considering both the spin–orbit coupling (SOC) and the electronic structures of these complexes at their respective optimized singlet ground (S₀) and first triplet ( ) excited states, we were able to rationalize the experimental findings that 1) 1 is a strong emitter while its isomer 2 is only weakly emissive in CH₂Cl₂ solution at room temperature; 2) although the cyclometalated ligand of 3 has a higher ligand‐field strength than that of 1 , 3 is nonemissive in CH₂Cl₂ solution at 298 K; and 3) extension of π conjugation at the lateral aryl rings of the cyclometalated ligands of 2 and 3 to give 4 and 5 , respectively, leads to increased emission quantum yields under the same conditions. We found that Jahn–Teller and pseudo‐Jahn–Teller effects are operative in complexes 2 and 3 , respectively, on going from the optimized S₀ ground state to the optimized excited state, and thus lead to large excited‐state structural distortions and hence fast nonradiative decay. Furthermore, a strong‐field ligand may push the two different occupied d orbitals so far apart that the SOC effect is small and the radiative decay rate is slow. This work is an example of electronic‐structure‐driven tuning of the phosphorescence efficiency, and the DFT/TDDFT approach is demonstrated to be a versatile tool for the design of phosphorescent materials with target characteristics.     

直流磁控溅射Au膜的微观应变研究

采用直流磁控溅射技术在室温下制备了厚度为108.4和215.6 nm的Au膜,膜厚由椭偏仪测定.利用常规CBD扫描模式对Au膜微结构进行分析,并采用剖面分析直接法测定Au膜的微观应变.X射线衍射(XRD)分析表明,Au膜在平行于基片表面沿<111>方向择优生长;衍射线剖面的宽化主要由晶格畸变所致.厚度为215.6 nm Au膜的微观应变量为0.065,比108.4 nm Au膜(0.055)略大.