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Generalized soft-and-hard surface

机译:广义的软硬表面

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摘要

Soft-and-hard surface (SHS) is a mathematical idealization of the tuned corrugated boundary. The boundary conditions are defined by a single real vector parallel to the corrugations. The SHS boundary was recently generalized by replacing the real vector by a complex vector and its conjugate (see Lindell, I.V., Proc. Inst. Elect. Eng. Microw. Antenna Propagat., vol.147, p.495-9, 2000). The SHS boundary is generalized one step further by defining it in terms of two complex vectors tangential to the surface. It is shown that, analogous to the previous special cases, there exist two eigenpolarizations, TE and TM with respect to the two vectors for plane waves of any angle of incidence. These two specially polarized waves see the boundary as a simple perfect magnetic or electric conductor surface, respectively. Because the same is true for TE and TM parts of fields radiated by finite sources, it is possible to apply the classical image theory for the computation of fields in the presence of a planar generalized SHS boundary. A principle of realization of such a boundary is briefly discussed. If the two vectors defining the boundary can be realized in practice, a device transforming any given polarization to any other polarization in reflection appears feasible.
机译:软硬表面(SHS)是调整后的波纹边界的数学理想化。边界条件由平行于波纹的单个实矢量定义。 SHS边界最近通过用复数向量及其共轭物替换实向量进行了泛化(请参阅Lindell,IV,Proc。Inst。Elect。Eng。Microw。Antenna Propagat。,第147卷,第495-9页,2000年) 。通过根据与曲面相切的两个复数向量定义SHS边界,将其进一步推广了一步。结果表明,与以前的特殊情况类似,对于任意入射角的平面波,两个向量都存在两个本征极化TE和TM。这两个特殊极化的波分别将边界视为简单的理想磁或电导体表面。因为对于有限源辐射的TE和TM部分场也是如此,所以可以在存在平面广义SHS边界的情况下将经典图像理论应用于场的计算。简要讨论了实现这种边界的原理。如果定义边界的两个向量可以在实践中实现,则将任何给定偏振转换为反射中任何其他偏振的设备似乎都是可行的。

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