Phosphaalkynes—Syntheses,Reactions, Coordination Behavior [New Synthetic Methods (73)]

Organophosphorus compounds have been applied in two ways in chemical synthesis. They can either be used as a reagent in a step of the synthesis (for example, in the Wittig reaction) or they can be incorporated directly into the target molecule. This second application, in particular, has expanded greatly in the last few years with the preparation of low-coordination phosphorus compounds. These include the phosphaalkynes, which are of great interest to organic and inorganic chemists. Phosphaalkynes have been employed in the synthesis of heterocyclic compounds, phosphaarenes and their valence isomers, and polycyclic compounds. Further applications have been the use of phosphaalkynes as new ligand systems in complex chemistry and their cyclooligomerization with organometallic reagents. While the chemical properties of phosphaalkynes have little in common with those of nitriles, they are in many ways very similar to those of the isoelectronic acetylenes.     

Multiple scattering in random media I. Restricted two-body additive approximation

We present a microscopic theory of the problem of finding the properties of a particle interacting with potentials located at random sites. The sites are governed by a general probability distribution. The starting point is the multiple scattering equations for the amplitude k ₁|T |k ₂ in terms of the individual scattering amplitudes k ₁|T |k ₂. We work with quantitiesA defined by k ₁|T |k ₂=k ₁|T |k ₂exp[i(k ₁–k ₂)R ]. The theory is based on a splitting of the fundamental equation forA into equations for the mean A and the fluctuationsAA . Neglect of the fluctuations yields the quasicrystalline approximation. We rearrange the equation forAA to isolate the collective part of the fluctuations. We then make the simplest microscopic truncation which is thatAA is a restricted two-body additive function of the site positions. With the contribution of the collective fluctuations, this yields results forA that are accurate to ordert ⁴.Work supported in part by the National Science Foundation under Contract No. NSF DMRWork supported in part by the National Science Foundation under Contract No. NSF DMR     

基于DRFM的脉冲多普勒雷达组合干扰及其效能评估

脉冲多普勒雷达具有较强的抗干扰能力，对其实施有效干扰有一定的困难。本文仿真研究了两种基于数字射频存储器的脉冲多普勒雷达组合干扰技术，并分别提出了脉冲多普勒雷达压制性干扰和欺骗性干扰的干扰效果度量方法，该方法在具体应用场合更贴近于干扰抗干扰的动态对抗过程。     

HFC网络中数字电视信号性能参数测试分析

光纤同轴混合(HFC)网是目前承载数字电视信号的主要传输媒质,HFC网络能否真正满足数字电视传输网络的要求,需要对HFC网络中数字电视信号性能参数进行测试分析.在讨论数字电视信号电平、误码率、调制误差比等主要性能参数的基础上,根据实际运营的有线数字电视HFC网络构建测试模型,测试了数字电视信号的性能参数,分析了数字电视信号在HFC网络中的传输情况.测试分析表明:在目前条件下,HFC网络能适应数字电视信号的传输,有一定的优越性.     

腔长失调对光腔衰荡法测量精度的影响

 只考虑腔长失调因素下建立了反射率模拟测量的理论模型。根据高斯光束传输规律分析了腔长失调对衰荡腔模式耦合的影响，推导了腔长失调与谐振腔输出脉冲信号、衰荡信号与反射率之间的关系，模拟了腔长失调在±10mm范围内的光脉冲衰荡现象。结果表明：对于光敏面直径为0.2mm的高速探测器，为了保证10^-6的测量精度，腔长的失调量应控制在±1mm之间。在光路调节中采用具有对数变换功能的示波器和动态范围较大的探测器，可以提高测量精度。     

激光微细加工中微小曝光区域的计算机温度测量系统

在半导体的激光微细加工技术里，微小曝光区域的温度分布是关键的工艺参数，必须得到精确的测量。而为了使温度测量不影响曝光区的温度分布，需采用不接触测量方法。研制了计算机温度测量系统，实现了微小激光曝光区温度的实时不接触测量。系统中，InGaAs／InP光探测器将微小高温区的温度信号转换为光电流．再经信号放大及模／数转换后输入计算机。结合温度定标实验，对测得的温度数据进行插值运算，在实验中可以实时显示出曝光区的温度值。系统的温度分辨率可达到0．2℃，测量区域的最小直径可达到18μm。同时设计了搜索算法，使温度数据采集和精密位移平台的移动相配合，实现了温度分布的测量和最高温度区的准确定位。     

分块镜扇形子镜驱动点位置优化计算

在光学综合孔径共相位检测微调系统中,分块镜子镜三自由度微动调节机构通常采用3个并联的微位移致动器来驱动各子镜,使单个分块镜具有独立的姿态调整能力,从而实现了光学共相位误差的纳米级精确校正。以理论力学原理作为切入点展开了分析,针对微动机构的稳定性、tilt-tip调节灵敏度等,根据所给定几何参数的子镜三驱动点位置对其进行了优化计算。经数学建模和仿真计算,得到了定参数子镜的三驱动点最佳位置坐标,进而归纳出了普遍适用的优化评价方法。     

夫琅和费衍射与大角度衍射

众所周知,夫琅和费衍射的解析强度分布和暗纹位置是在一系列近似情况下导出的。其中最重要的条件是观测点必须限制在傍轴附近,衍射角不能太大,否则得不到简单的解析公式,也就不能称之为夫琅和费衍射。最近发现有人发明错误的理论将夫琅和费衍射概念及其测量扩展到90°角,其结论与常识截然相反,因此,有必要把混淆的概念予以澄清。     

基于联合变换相关器的像移测量仿真分析

对基于联合变换相关器的像移测量数学原理进行了说明,介绍了面阵CCD的安装位置以及输入图像的获取方法,分析了低信噪比输入图像、相对转动位移对测量精度的影响。应用MATLAB对输入图像进行傅里叶变换得到联合功率谱,对二值化处理的功率谱进行傅里叶变换得到相关输出,用质量中心算法计算出像移量。分析得出,输入图像信噪比大于5dB,测量均方误差小于0.05像素;输入图像相对转动位移在0.1°的范围内,转动位移对测量精度和峰噪比的影响可以忽略不计。综合分析表明像移测量均方误差小于0.05像素。