二维理想导体角反射器电磁散射场的计算

报道了采用模式匹配技术计算电极化和磁极化平面波垂直入射时二维理想导体角反射器散射场的方法。推导出以散射场展开系数为未知量的线性方程组，由计算机求解线性方程组得到散射场的展开系数，从而计算散射场。还给出计算实例，并与矩量法计算结果比较，两者一致。     

大尺寸参数双球散射场展开系数的计算

利用矢量球谐函数,根据电磁场边界条件,建立相关方程,严格求解了双球粒子散射场展开系数.并将计算出的散射场与用散射传输矩阵法得到的结果进行了对比.结果显示:两者在小粒子情况下吻合很好.同时利用文中公式可数值计算出更广泛的算例.它也是解决更复杂条件粒子相关散射的基础.     

手征涂覆球对高斯波束的散射

在广义米理论的基础上,通过把入射高斯波束、散射场和内部场用适当的球矢量波函数展开,给出了一种求解手征涂覆球对高斯波束散射的解析方法。待定的展开系数可由从边界条件得到的线性方程组求出。对于波束的区域近似模型,给出了微分散射截面的数值结果。结果表明：与介质涂覆的情况相比,手征涂覆对微分散射截面和散色场的极化特性都产生了较大的影响。     

二维密集导体目标散射的数值模式匹配法

用数值模式匹配法(Numerical Mode Match,NMM)求解空间随机分布的二维任意形状导体柱目标的复合散射。每个目标的散射场在各自局部坐标系中用柱面波函数展开,外部空间的散射场由所有目标散射场的叠加共同贡献。在每个导体目标表面选取若干离散点数值匹配边界条件,得到关于展开系数的超定矩阵方程,用奇异值分解(Singular Value Decomposition,SVD)或最小二乘法获得其最佳逼近解。这样,空间的散射场可由级数展开解析计算。数值分析了展开级数的截断问题,与矩量法(Method of Moment,MoM)数值计算的结果比较和误差分析获得不同形状和不同尺寸目标的展开项数,并用多项式拟合了简单的函数式。最后,针对不同形状组合的多导体柱复合散射模型分析其双站散射计算,与MoM方法的结果比较表明:数值模式匹配法能快速准确地分析任意尺寸任意位置任意形状复合目标的散射计算。     

线源激励二维理想导体角反射器辐射场严格解

采用模式匹配法,对平行电流丝或磁流丝作用下二维理想导体角反射器的电磁辐射进行了严格地电磁场分布。推导出了以散射场展开系数为未知量的矩阵方程,给出了计算实例,其中张角为１８０℃（即平板）的计算结果与文献［４］的结果是一致的。     

随机球粒媒质的弹性多散射

从多散射场的基本积分方程出发,利用场的矢量球波函数展开及矢量球波函数的坐标变换迭加公式,导出了求解随机球粒媒质的弹性多散射场矢量球波函数展开系数的一组耦合线性方程,从而建立起一种新的分析随机球粒媒质的弹性多散射理论。不同于现有方法,本文方法得到了整个空间的多散射场。     

阻抗球涂覆均匀等离子体电磁散射的解析解

均匀无源各向异性等离子体介质中的电磁场是第一、第二类各向异性等离子体球矢量波函数的线性叠加,在阻抗球表面满足阻抗边界条件、等离子体与自由空间表面满足电磁场切向连续的边界条件,可得出各向异性等离子体涂覆阻抗球在平面波入射情况下,均匀等离子体介质中电磁场用各向异性等离子体球矢量波函数表示的系数满足的矩阵方程,进而得出散射场由球矢量波函数展开的展开系数和雷达散射截面.数值计算的结果表明:当阻抗球的半径趋于0时,其结果和均匀各向异性等离子体球对平面波的电磁散射结果相同.最后还给出了一些数值计算的结果.     

用复射线展开法计算目标散射场的误差特性分析

复射线展开法是计算目标散射场的一种简捷的方法,其可靠性有赖于对误差特性的系统研究。本文以平面波谱积分为散射场计算的参考标准,以L~2空间中由范数定义的距离作为复射线展开法计算结果的误差,从而得到了复射线展开法在目标散射场计算中的误差特性,找到了减小误差的方法并给出这一方法的适用范围。     

用复射线展开法计算目标散射场的误差特性分析

复射线展开法是计算目标散射场的一种简捷的方法，其可靠性有赖于对误差特性的系统研究，本文以平面波谱积分为散射计算的参考标准，以Ｌ＾２空间中由范数定义的距离作为复射线展开法计算结果的误差，从而得到了复射展开法在目标散射场计算中的误差特性，找到了减误差的方法并给出这一方法的适应范围。     

波导不连续问题分析中基函数对收敛性能影响的研究

提出了利用多种新的基函数系列展开波导不连续处的场并求解该不连续性的散射参量的方法.通常可结合不连续处的金属楔近旁的边缘条件,构造出满足该边缘条件的变形三角基函数用以展开不连续处的电磁场,匹配公共口面处的切向电磁场即可得到一个线性方程组,可得到极好的数值收敛;还进一步采用不同的多种基函数,也可以获得极好的数值收敛.对于一个不连续性,方程组的阶数与基函数的个数(几个甚至一个)相等,因而方程组保持了较低的阶数,极大地提高了计算效率.     

气溶胶散射光偏振度特性的理论研究

散射光偏振度在大气气溶胶、大气污染的遥感探测中有重要的应用价值。通过求解Mueller矩阵及偏振度,讨论了当激光器输出波长处于近红外波段806 nm时，散射介质的粒子数浓度对散射光偏振度的影响。给出了散射光的偏振度与散射介质的粒子数浓度之间的变化关系，为使用散射光偏振度研究大气遥感提供了新途径。     

TM scattering by a wedge with concaved edge

The TM scattering problem by a perfectly conducting wedge with concaved edge is formulated for a line source excitation using the mode-matching technique. The scattered and guided fields are represented in terms of an infinite series of radial waveguide modes with unknown coefficients. By applying the appropriate boundary conditions, the coefficients of scattered field are obtained. For small ka, the diffraction coefficient of concaved edge is derived from the scattered field     

高隔离度双极化微带天线直线阵的设计

本文介绍一种新型的1×16双极化微带天线直线阵的设计.该天线采用双极化角馈方形贴片单元,阵列的垂直极化端口采用共面馈电,水平极化端口采用口径耦合,并在馈电网络中应用反相馈电技术.实验结果表明,天线二端口驻波比小于1.5的相对带宽分别达到15％和13.5％,两端口之间的隔离度在频带内高于33dB,最大达到43dB.本直线阵可用作星载综合口径雷达系统的天线子阵,便于与有源收发器件结合.     

计算轴对称粒子光散射问题的简化T矩阵方法

首先给出了光散射计算中的T矩阵方法的推导过程,然后分析了轴对称粒子T矩阵的特点——方位模m的独立性。并由此特点对原始的T矩阵进行了简化和变形,去除了其中的零元素并将其分成关于方位模m的小矩阵。然后运用基于方位模m的独立方程求得散射场系数。最后以球形粒子为例得到散射场的仿真结果与用微元法有很好的吻合。     

Electromagnetic scattering from two adjacent objects

In the paper, the problem of electromagnetic scattering from two adjacent particles is considered and an iterative solution that accounts for multiple scattering up to second-order is proposed. The first-order solution can easily be obtained by calculating the scattered field of isolated particles when illuminated by a plane-wave. To get the second-order solution, the scattered field from one of the particles, with nonuniform phase, amplitude, and polarization, is considered as the illuminating wave for the other particle and vice versa. In the work, the second-order scattered field is derived analytically using a novel technique based on the reciprocity theorem. In specific, the analytical solution for bistatic specular scattering from a cylinder and sphere pair is discussed and the results are compared with numerical computations based on the method of moments     

Oblique scattering by a pair of conducting half planes: TM case

An exact series solution for the oblique scattering by a pair of infinitely long parallel edges of perfectly conducting half planes is formulated for a TM plane wave using the mode-matching technique (MMT). The scattered and guided fields are represented in terms of an infinite series of radial waveguide modes. By applying the appropriate boundary conditions, the coefficients of the scattered field are obtained. The diffraction coefficient of double edges is subsequently derived from the scattered field     

SEM representation of the early and late time fields scattered fromwire targets

In the communication, the singularity expansion method (SEM) is used to express the field scattered from an arbitrary thin-wire target. Explicit expressions are given for both the class-1 and class-2 representations of the scattered field due to step excitations. Numerical results are given for the early-time transient fields scattered from both a straight wire and a simple swept-wing aircraft model. The results of the SEM computations are compared to fields obtained by Fourier inversion techniques. It is shown that the class-2 representation yields a significant improvement over the class-1 result during the early-time interval, albeit at the expense of a more complex computation     

Wave diffraction by a right-angled interface between resistive half and whole planes

The interaction phenomenon of electromagnetic plane waves by a right angled interface between whole and half screens with different resistivities is studied. The construction, under examination, is considered in order to model various corner discontinuities between transmissive surfaces for indoor wireless communications. First of all, the initial waves, which occur in the absence of the diffracting edge, are determined. Then the scattered geometrical optics fields are obtained by subtracting the initial waves from the total geometrical optics fields. The diffracted field is constructed directly from the scattered geometrical optics wave by a new method. The resultant field expressions are examined numerically.     

Radar cross sections of dielectric or plasma coated conducting spheres and circular cylinders

Radar cross sections for a variety of spherical and cylindrical scatterers having homogeneous dielectric or plasma shells are obtained by using both the exact boundary value solutions and approximate, semi-empirical methods based on physical principles. The plasma is assumed to have the macroscopic properties of a lossless dielectric with a permittivity less than that of free space. A superposition approximation for the radar cross section of a dielectric coated conducting body is obtained by considering the scattered field to be the phasor sum of two principal components, the field scattered by the air-dielectric interface and the field scattered by an equivalent conducting body which differs from the actual body because of the lens action of the shell. This approximation yields very good agreement with the exact solutions for both spherical and cylindrical dielectric clad scatterers with radii in the Rayleigh region and in the resonant region, and for bistatic scattering as well as for backscatter. The echo area of a conducting sphere with nonconcentric spherical dielectric shell calculated by means of the superposition approximation is in excellent agreement with experimental measurements, thus demonstrating the validity of this method in a case for which the exact solution cannot be obtained.     

求解目标地波散射特性的方法研究

本文把求解半空间散射问题的FDTD技术与地波传播理论相结合，研究任意复杂目标的地波散特性。入射地波设置在FDTD计算区域中的总场边界上并在散射场输出边界面上提取散射近场数据，然后利用等效及镜像原理，计算无地波衰减时的远区散射场，通过引入地波衰减因子，把该远区散射场转换为远区地波散射场，文中给出了方法验证例子以及一个较复杂目标的单站RCS计算结果。