SEG Technical Program Expanded Abstracts 1997 1997
DOI: 10.1190/1.1885751
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Generalized form of Snell's law in anisotropic media: A practical approach

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Cited by 2 publications
(3 citation statements)
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“…Inspired by [ 27 ], the unit in the middle of the metasurface is taken as the origin and coordinates are defined as mn , − mn , and so on when expanding in different directions on both sides of the origin unit. The formula for far-field scattering is shown in Equation (8) according to the relevant conventional phased array antenna theory [ 28 ] and generalized Snell’s law [ 29 ]. where and are the pitch and azimuth angles of the scattered field, is the far-field of the unit, is the propagation constant, and are the amplitude and phase of the excitation current in the unit located at the coordinates ( x m , y n ), respectively.…”
Section: Theoretical Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…Inspired by [ 27 ], the unit in the middle of the metasurface is taken as the origin and coordinates are defined as mn , − mn , and so on when expanding in different directions on both sides of the origin unit. The formula for far-field scattering is shown in Equation (8) according to the relevant conventional phased array antenna theory [ 28 ] and generalized Snell’s law [ 29 ]. where and are the pitch and azimuth angles of the scattered field, is the far-field of the unit, is the propagation constant, and are the amplitude and phase of the excitation current in the unit located at the coordinates ( x m , y n ), respectively.…”
Section: Theoretical Analysismentioning
confidence: 99%
“…Inspired by [27], the unit in the middle of the metasurface is taken as the origin and coordinates are defined as mn, −mn, and so on when expanding in different directions on both sides of the origin unit. The formula for far-field scattering is shown in Equation (8) according to the relevant conventional phased array antenna theory [28] and generalized Snell's law [29].…”
Section: Graphene-based Metasurface Codingmentioning
confidence: 99%
“…Вектора медленности отраженных и преломленных волн находятся из закона Снеллиуса для анизотропных сред [Slawinski et al, 2000], который в данном случае заключается в равенстве проекций векторов медленности на ось X падающей, отраженных и преломленных волн. Вектора поляризации находятся путем нахождения собственных векторов соответствующей матрицы Кристоффеля.…”
Section: расчет коэффициентов отражения от границы азимутально-анизотропных средunclassified