Abstract:IntroductionElectrodynamical structures which contain semi-infinite sequences of discontinuities are of interest for a long time. Such structures have a significant feature compared to the infinite ones: they allow to describe the field scattered by the edge of a real finite grating.The approach which supposes that the full field is defined as a superposition of fields scattered by each element with unknown coefficients is widely used in diffraction problems by semi-infinite gratings [1], [2], [3]. Then the co… Show more
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