Spherical-multipole analysis of scattering by finite and semi-infinite elliptic cones

S. Blume, L. Klinkenbusch
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Abstract

The interest in scattering by elliptic cones is mainly motivated by the role which the diffraction coefficients play in asymptotic high frequency theories like the GTD (geometrical theory of diffraction) or the uniform theory of diffraction. Since the elliptic cone possesses a two-parametric tip, the pertinent field must contain the information of a very general tip diffraction coefficient (TDC). This TDC is obtained by analysis of the field scattered by a semi-infinite elliptic cone and is then validated by comparing the exact field scattered by a finite elliptic cone with the corresponding complete GTD-result (including the TDC). By applying the spherical-multipole technique the exact solutions for the scattering of EM waves by a finite as well as by a semi-infinite perfectly conducting elliptic cone are deduced. The vector problems are reduced to scalar problems. Products of spherical Bessel functions and so-called Lame products, the vector spherical-multipole functions can be derived, which form a complete base to construct any EM field outside the sources. The boundary-value problem for the finite elliptic cone is formulated as a standard two-domain problem. In each domain the EM field is described by an appropriate spherical multipole expansion, while the corresponding multipole amplitudes are found by enforcing the boundary- and continuity conditions of the field and by employing the orthogonality relations of the vector spherical-multipole functions. The problem of plane wave scattering by a semi-infinite elliptic cone is solved via the pertinent dyadic Green's function. Suitable sequence transformations are applied which enforce the convergence and yield the limiting value for these series.
有限和半无限椭圆锥散射的球-多极分析
对椭圆锥散射的兴趣主要是由于衍射系数在渐近高频理论中所起的作用,如GTD(几何衍射理论)或均匀衍射理论。由于椭圆锥具有双参数尖端,相关场必须包含一个非常一般的尖端衍射系数(TDC)的信息。通过对半无限椭圆锥散射场的分析,得到了该TDC,然后通过将有限椭圆锥散射场的精确场与相应的完整gtd结果(包括TDC)进行比较,验证了该TDC的正确性。应用球多极技术,导出了有限完全导电椭圆锥和半无限完全导电椭圆锥对电磁波散射的精确解。向量问题被简化为标量问题。由球面贝塞尔函数的积和所谓的Lame积,可以导出矢量球多极函数,它构成了构造源外任何电磁场的完整基础。将有限椭圆锥的边值问题表述为标准的二域问题。在每个域中,电磁场用适当的球面多极展开来描述,而相应的多极幅值则通过加强场的边界条件和连续性条件以及利用矢量球多极函数的正交关系来求得。利用相应的并矢格林函数求解了半无限椭圆锥的平面波散射问题。利用适当的序列变换来增强这些级数的收敛性并得到它们的极限值。
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