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New expressions for equivalent edge currents

机译:等效边沿电流的新表达式

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摘要

It is known that the results of incremental length diffraction coefficients (ILDC) (1) and the method of equivalent edge currents (MEC) (2) differ by terms due to the physical optics (PO) current. These PO components become infinite for certain aspects of observation and illumination, by the extraction of the PO contribution from MEC, ILDC, unlike MEC, predicts finite currents for certain directions of observation. However, as already observed by Mitzner (1), ILDC also displays infinities for certain combinations of observation and incidence directions, though the range of singular aspects reduced in comparison with the MEC. Michaeli (3) derived a set of expressions for the fringe current components of equivalent edge currents, those expressions are finite for all aspects of illumination and observation, except for the Ufimtsev singularity. However, for certain non-singular aspects of ILDC expressions, there is a wide divergence between Michaeli's results (3) and Mitzner's results (1).
机译:众所周知,由于物理光学(PO)电流,增量长度衍射系数(ILDC)(1)和等效边缘电流(MEC)(2)的方法各有不同。通过从MEC中提取PO的贡献,这些PO分量对于观察和照明的某些方面变得无穷,ILDC与MEC不同,它预测了在某些观察方向上的有限电流。然而,正如Mitzner(1)所观察到的那样,尽管与MEC相比,单数方面的范围有所减小,但ILDC也显示了观察和入射方向的某些组合的无穷大。 Michaeli(3)为等效边缘电流的边缘电流分量导出了一组表达式,这些表达式对于照明和观察的所有方面都是有限的,除了Ufimtsev奇异性。但是,对于ILDC表达式的某些非奇异方面,Michaeli的结果(3)和Mitzner的结果(1)之间存在很大差异。

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