表面具有分形结构金属劈边缘绕射系数的提取

本文提出了一种计算数值绕射系数有有效方法，并将之用于提取表面具有分形结构金属劈的绕射系统，利用时域有限差分法提供的散射场，根据几何绕射理论建立含有绕射系数未知量的方程组，通过联立方程组的求解，得到散射体边缘的数值绕射系数。具体计算例子表明，该算法是有效的。     

电小尺寸凹槽的远区数值绕射系数

应用时域有限差分（FDTD）方法和时域加窗技术从物体的时域散射场中分离出劈和凹槽一类散射中心的贡献,计算其远区数值绕射系数。对于电小尺寸凹槽的远区数值绕射系数,结合微扰法给出了其计算结果。     

一种新的等效电磁流边缘分量表达式

增量长度绕射系数是目前用于计算边缘绕射场的一种方法,但对给定的入射波方向,在某此观察方向上,该方法会呈现出某些奇性.为消除上述奇异性,Michaeli推出了等效电磁流边缘分量的另外一种表达式,该表达式除存在Ufimtsev奇点外在所有观察方向上均不发生奇异.然而Michaeli的表达式不是增量长度绕射系数的推广,在增量长度绕射系数不奇异的情况下,两者的计算结果可能会有较大的差别.本文提出了一种新的等效电磁流边缘分量表达式.与Michaeli的同类表达式相比,新表达式既能有效克服增量长度绕射系数(ILDC)方法中的某些奇异性困难,又能与ILDC保持很好的一致性,因此更具实际应用价值.     

压缩天线测试场反射器的设计

应用几何绕射理论的结果,分析、介绍了两种压缩天线测试场(简称压缩场)反射器—滚边反射器和锯齿边反射器。导出了锯齿边反射器的边缘轮廓线方程,并根据J.B.凯勒的口径角点绕射系数公式,介绍了角点绕射场的计算式。给出了平面反射器模型的实验结果。     

由散射数据计算数值绕射系数

本文研究数值一致性绕射系数的提取方法。在建立散射模型并确认其散射中心后，用ＦＤＴＤ方法计算散射场，并通过电流加窗方法或联立方程组方法以提取所关心散射中心的一致性绕射系数。金属板边缘的例子验证了这一途径的可行性。最后，用这种方法获得了涂层金属板的一致性统射系数，其结果与阻抗劈的ＵＴＤ结果一致。     

涂层金属平板绕射系数的计算

本文介绍了一种计算目标绕射系数的通用数值方法－－根据时域有限差分（ＦＤＴＤ）方法提供的散射场，通过联立方程组求解绕射系数，所述方法对二维ＴＭ、ＴＥ波均适用，有无涂层情况下金属条板绕射系数的计算例子表明该方法是可行的。     

任意多边形导体板的高频散射分析

结合微分长度绕射系数和一致性等放电磁流推导得到了微分边缘绕射系数，将任意观察方向上的远区散射场与任意方向入射的平面波以绕第三者数形式联系起来，得到一种实用简便的高频散射计算方法。并以多边形平板为例验证了该方法。     

基于ILDC理论的平面结构电磁散射计算

增量长度绕射系数理论(ILDC)是对电大尺寸复杂目标进行边缘绕射计算的有效方法之一。本文基于散射总场、表面光学场和边缘绕射场三者之间的关系,针对几何建模的特点,从另一个角度推导出了ILDC在平表面结构中的应用形式,并验证了该方法的正确性,为目标电磁特性的研究提供了一种可行的计算方法。     

理想导体半圆柱TE波散射的混合法解

本文应用混合技术分析了在TE平面波激励下,理想导体半圆柱的双站散射。该混合技术是把半圆柱劈附近的电流表示为未知数,圆柱曲面上的一阶电流应用Fock理论求解,高阶绕射电流表示为含有未知系数的Fock型函数。圆柱平面上的一阶电流用物理光学近似和曲劈的一致性几何绕射理论得到。劈的二阶绕射电流表示为含有未知系数的GTD形式。然后通过磁场积分方程,运用简单矩量法求得劈附近的电流和未知的绕射系数。最后计算了理想导体半圆柱的双站散射截面,结果与矩量法的结果吻合得相当好。     

基于ILDC理论的平面结构电磁散射计算

增量长度绕射系数理论(ILDC)是对电大尺寸复杂目标进行边缘绕射计算的有效方法之一。本文基于散射总场、表面光学场和边缘绕射场三者之间的关系，针对几何建模的特点，从另一个角度推导出了ILDC在平表面结构中的应用形式，并验证了该方法的正确性，为目标电磁特性的研究提供了一种可行的计算方法。     

PTD analysis of impedance structures

Based on an approximate dyadic diffraction coefficient, equivalent currents (ECs) are derived for computing the scattering by a finite-length impedance wedge of arbitrary angle. The derived equivalent currents are implemented in a standard general purpose physical theory of diffraction (PTD) code and results are presented demonstrating the accuracy of the formulation for a number of impedance and (dielectrically) coated structures. These include typical shapes such as plates, finite-length cones, and cylinders which have been partially or fully coated. The PTD implementation requires a dyadic physical optics diffraction coefficient which is presented in the appendix     

A uniform geometrical theory of diffraction for an edge in a perfectly conducting surface

A compact dyadic diffraction coefficient for electromagnetic waves obliquely incident on a curved edse formed by perfectly conducting curved ot plane surfaces is obtained. This diffraction coefficient remains valid in the transition regions adjacent to shadow and reflection boundaries, where the diffraction coefficients of Keller's original theory fail. Our method is based on Keller's method of the canonical problem, which in this case is the perfectly conducting wedge illuminated by plane, cylindrical, conical, and spherical waves. When the proper ray-fixed coordinate system is introduced, the dyadic diffraction coefficient for the wedge is found to be the sum of only two dyads, and it is shown that this is also true for the dyadic diffraction coefficients of higher order edges. One dyad contains the acoustic soft diffraction coefficient; the other dyad contains the acoustic hard diffraction coefficient. The expressions for the acoustic wedge diffraction coefficients contain Fresenel integrals, which ensure that the total field is continuous at shadow and reflection boundaries. The diffraction coefficients have the same form for the different types of edge illumination; only the arguments of the Fresnel integrals are different. Since diffraction is a local phenomenon, and locally the curved edge structure is wedge shaped, this result is readily extended to the curved wedge. It is interesting that even though the polarizations and the wavefront curvatures of the incident, reflected, and diffracted waves are markedly different, the total field calculated from this high-frequency solution for the curved wedge is continuous at shadow and reflection boundaries.     

介质涂敷导电凸曲面上磁振子辐射场一致性几何绕射理论

本文研究了介质涂敷导电凸曲面上磁振子辐射与绕射一致性高频渐近理论。文中在典型曲面辐射场一致性高频近似解基础上发展了介质涂敷导电凸曲面上磁振子辐射与绕射的一致性几何绕射理论,导出了涂敷导电凸曲面上磁流源高频电磁辐射场的一致性几何绕射理论公式。在这个公式中,辐射与绕射场用四个广义Ｆｏｃｋ型函数表示,深光区这些函数退化为几何光学场,暗区场则表示为不同模式爬行波的叠加。     

理想导电凸曲面上振子电磁辐射UTD解的并矢格林函数方法

P.H.Pathak,Wang Nan等人在研究典型问题几何绕射理论之后,于1981年发表了任意导电凸曲面振子天线高频电磁辐射一致性几何绕射理论近似解。本文应用并矢格林函数方法,通过典型曲面高频电磁辐射一致性近似解的研究和推广,导出了理想导电凸曲面上电、磁振子电磁辐射场在高频近似下一致性几何绕射理论近似解。与P.H.Pathak,Wang Nan等人的结果相比,主项并矢转移函数除个别系数外完全相同,高阶并矢转移函数在几何光学区略有差异。     

Diffraction d’une onde rampante par une ligne de discontinuité du plan tangent

This article is devoted to the study of the problem of diffraction of a creeping wave by a line of discontinuity of the tangent plane forming a salient edge. The author proposes a method based on the usual postulates of the Geometrical Theory of Diffraction. He exposes the principle of the method as well as the steps leading to the expressions of the dyadic diffraction coefficients.     

A simplified expression of the dyadic Green's function for a conducting half-sheet

Simple analytical expressions of the dyadic Green's function for a conducting half-sheet have been derived. These expressions involve some finite integrals which can be easily calculated by a digital computer and are much simpler than those involving the vector mode function expansion. Input impedances of monopole antennas on and near an edge of a conducting half-sheet and the impedance of a notch antenna have been obtained, and the usefulness of these simplified expressions has been proved. The present results can be applied to check the limits of the applicability of the asymptotic theories, e.g., the geometrical theory of diffraction (GTD) and the uniform asymptotic theory of diffraction (UAT).     

UTD propagation model in an urban street scene for microcellularcommunications

A three-dimensional propagation model for microcellular communications in an urban street scene is presented. The model is based on the uniform theory of diffraction (UTD) and takes into account multiple wall-to-wall, wall-to-ground, and ground-to-wall reflections, the diffraction from corners of buildings, and subsequent reflections from such diffracted signals. The ray geometry is made extremely complex by the presence of ground reflections and the many combinations of sequences of reflections or diffractions from walls, edges, and ground. At each reflection or diffraction point, the local ray-fixed coordinate system or edge-fixed coordinate system is used together with appropriate dyadic reflection or diffraction coefficient matrices. The theoretical results for the signal path loss along the streets are compared with measurements done in New York and Tokyo for various values of the propagation parameters. Agreement with these measurements indicates that the UTD formulation is a good model for such urban communication applications     

并元序列研究

对并元码偶作出进一步研究,首先提出了一类新的区组设计——并元加集偶的概念,研究了并元加集偶的一些特性。然后给出了并元加集偶与并元码偶的等价关系,应用这一等价关系给出了并元码偶存在的必要条件,也为并元加集偶的构造提供了理论依据。最后还研究了并元码偶的Walsh谱特性和重量分布特性。通过这些问题的研究,展示了Walsh变换新的应用。这些存在条件在这类码的理论研究和计算机搜索中有重要的作用。