单层和双层手征介质球域中并矢格林函数理论及其应用研究

本文应用散射迭加法，首先给出了单层和双层手征介质球域中的并矢格林函数，分析了点偶极天线分别位于手征介质球心和球罩内任意位置处的辐射场特性，并组给出辐射阻抗随手征介质球尺寸的变化规律，特别考虑了手征导纳的影响；研究表明，通过改变手征介质球罩的厚度和波长之比，可以任意调节罩外辐射场的极化状态，因此，手征介质在天线工程中有广阔的应用前景。     

单层和双层手征介质柱域的并矢格林函数理论及其应用

本文应用散射叠加法，分别导出了单层和双层手征介质圆柱区域中的并矢格林函数。由此分析了位于手征介质圆柱和手征介质圆柱罩中心轴线上点偶极天线的辐射特性。结果表明，通过改变手征介质圆柱的尺寸和手征介质圆柱罩的厚度，可以任意调节辐射场的极化特性。另外，本文给出的并矢格林函数公式还可用于分析柱形手征微带天线的辐射特性。     

单层和双层手征介质柱域的并矢格林函数理论及其应用

本文应用散射叠加法,分别导出了单层和双层手征介质圆柱区域中的并矢格林函数。由此分析了位于手征介质圆柱和手征介质圆柱罩中心轴线上点偶极天线的辐射特性。结果表明,通过改变手征介质圆柱的尺寸和手征介质圆柱罩的厚度,可以任意调节辐射场的极化特性。另外,本文给出的并矢格林函数公式还可用于分析柱形手征微带天线的辐射特性。     

双层手征介质板中电偶极天线的辐射特性

本文首先给出电流源激励下双层手征介质中的并矢格林函数表达式，应用鞍点积分法，导出了有金属板衬底的双层手征介质中电偶极天线的辐射场表达式，分析了有、无空气隙时手征导纳对电偶极天线的方向图，θ＝０°方向的最大强和谐振频率的影响程度，结果表明，通过改变手征导纳参数，可以有效地调节电偶极天线的辐射特性。     

双层手征介质板中电偶极天线的辐射特性

本文首先给出了电流源激励下双层手征介质中的并矢格林函数表达式。应用鞍点积分法,导出了有金属板衬底的双层手征介质中电偶极天线的辐射场表达式。分析了有、无空气隙时手征导纳对电偶极天线的方向图,＝0方向的最大场强和谐振频率的影响程度。结果表明,通过改变手征导纳参数,可以有效地调节电偶极天线的辐射特性。     

手征球壳的低频电磁屏蔽效应分析

分析了手征介质球壳的低频电磁屏蔽效应，给出了一组手征电磁屏蔽球壳的设计曲线。比较了手征材料的一般电、磁屏蔽材料的不同之处，重点说明了该材料的特殊性。理论计算表明，这种新型材料是一种非常有前途的电磁屏蔽材料。     

手征Ω介质偶极子天线研究

本文首先探讨了用手征Ω介质作为微带天线基片的可能性。应用广义谱域指数矩阵方法,分析了单层和双层手征Ω介质中所有Ω单元的三种不同取向对偶极子天线辐射特性的影响,以及偶极子方向图随手征Ω介质损耗正切的变化情况。     

圆偏振光在手征负折射材料表面的反射和极化特性研究

从理论上分析了圆偏振光入射到手征负折射材料表面的反射与透射特性,给出了归一化反射透射功率与入射角的关系曲线以及布儒斯特角与手征参数之间的关系曲线.当入射角大于两个本征波的临界角时,全内反射现象发生.由于手征负折射介质中的一个本征波发生了负折射,右旋或左旋圆偏振光入射时反射波的极化态有着与常规介质完全不同的特性,以布儒斯特角入射时反射光都为线偏振波但极化方向并不相同.     

无介质基片直线渐变式槽缝天线辐射特性的分析

根据电磁场的等效原理，基于半无限大导电平面上磁流元的并矢格林函数，给出了无介质基片直线渐变式槽缝天线（TEM－LTSA）远区辐射场的主极化及交叉极化分量的理论公式，各极化分量只需计算一维的数值积分。分析天线张角、天线长度的各种结构的TEM－LTSA的交叉极化辐射特性，给出了对角平面内辐射场主极化辐值电平与交叉极化幅值电平的关系曲线。     

多层单轴手征类复合材料中的双重手征结构和特性

应用广义谱域指数矩阵技术，研究具有双重手征性结构的多层单轴复合手征介质层对任意极化入射平面电磁波的反射和透射特性。用数值方法分析了光轴取向、损耗、手征和非互易参数对反射和透射系数的影响。特别是交叉极化转换效应。结果表明，双各向异性单轴手征介质在新型模式极化转换器的研制等方面有重要的应用价值。     

Radiation of an aperture antenna covered by a spherical-shellchiral radome and fed by a circular waveguide

This paper presents a full-wave analysis of the radiation characteristics of an aperture antenna that is flush-mounted on a ground plane and fed by a circular waveguide supporting the dominant TE₁₁ mode. The antenna is covered by a dielectric hemispherical chiral radome. Huygen's equivalence principle and the image theory are utilized to simplify the problem. The magnetic dyadic Green's function for the three-layered geometry is formulated and applied to analyze the radiated electromagnetic fields outside the chiral radome. Both the exact and approximate expressions of electric fields valid for the Fresnel and Fraunhofer zones are obtained using the spherical vector wave functions and their approximations in the far zone. Various chiral materials are assumed and computations of antenna parameters are carried out. The effects of the dielectric chiral radome on the radiation power patterns, sidelobe levels, and 3-dB beamwidths are also discussed numerically     

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。     

Radiation of elementary sources in a chiral medium

The classical problem of radiation of elementary sources is generalized to the case of a chiral medium. The electromagnetic fields of right- and left-hand polarized waves are expressed in terms of vector potentials, and formulas for the components of the fields radiated by a vertical electric dipole in a chiral medium are obtained.     

Exact solutions of electromagnetic fields in both near and farzones radiated by thin circular-loop antennas: a general representation

This paper presents an alternative vector analysis of the electromagnetic (EM) fields radiated from thin circular-loop antennas of arbitrary radius a. This method, which employs the dyadic Green's function in the derivation of the EM radiated fields, makes the analysis more general, compact, and straightforward than those two methods published recently by Werner (1996) and Overfelt (1996). Both near and far zones are considered so that the EM radiated fields are expressed in terms of the vector-wave eigenfunctions. Not only the exact solution of the EM fields in the near and far zones outside the region (where r>a) is derived by the use of the spherical Hankel function of the first kind, but also the closed-series form of the EM fields radiated in the near zone inside the region 0⩽r   

Optimal Radiated Waveforms From an Arbitrary UWB Antenna

Solutions are presented for the optimal electric field waveforms radiated by an arbitrary ultrawideband (UWB) antenna. Optimization criteria include maximization of the electric field amplitude at a particular time and location, or maximization of energy density over a specified time interval at a particular location. Assuming bandpass signals, constraints are placed on the total radiated energy, the Q of the antenna, and the size of the antenna. The solution is developed using a spherical mode expansion of the fields radiated by an arbitrary antenna enclosed by a spherical mathematical surface, and optimized using variational methods. A closed-form result is obtained for the case of amplitude maximization, while an integral equation must be solved numerically for the case of energy maximization in a time interval. An interesting result from these solutions is that the shapes of the optimal radiated field waveforms are largely independent of the size of the antenna. The solutions also indicate that the antenna characteristics that provide optimum field amplitude or energy in the transient case are identical to those associated with maximum gain in the CW case.     

Theory of a corner-driven loop antenna immersed in a warm plasma

A linearized hydrodynamic theory and potential function technique arc used to formulate the theory of a corner-driven loop antenna immersed in a warm plasma. The theory explains some of the experimental observations obtained from impedance measurement of a loop antenna on the Ariel 3 satellite. The far-zone fields and the normalized radiated power for different antenna sizes are calculated. The results suggest that much of the radiated energy is radiated in longitudinal plasma waves     

Shielding effect of hollow chiral sphere

The low-frequency shielding effect of a spherical layer is studied. The layer is made of a chiral material and it is electromagnetically characterized with three material parameters: permittivity, permeability, and chirality. Due to chirality, there is magnetoelectric coupling. The electric and magnetic shielding effects are derived and are shown to be functions of the three material parameters and also the relative thickness of the layer. Illustrations display the effects of the various parameters on the shielding, which is different for the magnetic and electric fields. Among the special effects is that the shielding increases rapidly as the chirality parameter approaches the refractive index of the shell. This makes chiral shells in principle effective shields, and in the future they may offer an alternative to conducting materials for novel shielding applications     

Mutual coupling between two circular waveguides

The problem of coupling between two circular waveguides is solved using the Wiener-Hopf technique. Expressions for the radiated, reflected, and the transmitted fields are obtained and are expressed by three terms. The first term in these expressions represents the solution for an open ended circular waveguide, while the other two are due to the interaction between the two waveguides. It is shown that, the radiated, reflected, and the transmitted fields can also be found from the reflection coefficient of an open ended circular waveguide and an evaluation of a semi-infinite integral involving the fourier transformed Green's function of the Weiner-Hopf equation. Exact solutions are used to generate the approximate solution of the ray theory of diffraction. This is achieved by expanding the exact solution and using the modified diffraction coefficient of Lee in conjunction with a spherical wave-factor.