1990
DOI: 10.1016/0003-4916(90)90172-k
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Enhanced backscattering of light from a random grating

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Cited by 389 publications
(203 citation statements)
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“…Our rigorous calculation method is based upon the exact integral equations formulation of the above mentioned scattering problem. 15,[36][37][38][39] This formulation can be briefly summarized as follows. On the basis of the Helmholtz equations satisfied by the field in the upper U ␤ Ͼ (r, )(zϾ ) and lower U ␤ Ͻ (r, )(zϽ ) semi-infinite half-spaces, and by applying the Green's theorem and recalling the radiation conditions at infinity, we are led to the following four integral equations,…”
Section: Em Scattering Theorymentioning
confidence: 99%
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“…Our rigorous calculation method is based upon the exact integral equations formulation of the above mentioned scattering problem. 15,[36][37][38][39] This formulation can be briefly summarized as follows. On the basis of the Helmholtz equations satisfied by the field in the upper U ␤ Ͼ (r, )(zϾ ) and lower U ␤ Ͻ (r, )(zϽ ) semi-infinite half-spaces, and by applying the Green's theorem and recalling the radiation conditions at infinity, we are led to the following four integral equations,…”
Section: Em Scattering Theorymentioning
confidence: 99%
“…By means of a quadrature scheme the surface is truncated to a length L consisting of N sampling points. 36 In practice, for every realization of the random surface, it reduces to solving a system of 2N complex linear equations for the source functions, followed by a vectormatrix multiplication to obtain the scattered field at each position in the vacuum half-space. Furthermore, when statistical quantities such as ensemble averages ͑͗•••͒͘ or probability density functions ͑PDF͒ are needed, the procedure is repeated for a sufficiently large number N r of surface profile realizations ͑ergodicity is assumed͒.…”
Section: ͑23b͒mentioning
confidence: 99%
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“…The GO approximation is a commonly used approximation in rough surface scattering theory, [2][3][4][5][6] due to its relatively simple numerical implementation and the reduced computational requirements compared to the numerical integration techniques needed for rigorous electromagnetic wave analysis. [7][8][9][10][11] The approximation is a ray-tracing approach, where energy bundles are traced throughout their interactions with the surface until they leave it. The approximation is regarded as valid when the normalized correlation length, / , as well as the normalized rms roughness, / , are larger than unity ͑ being the wavelength of the light involved͒.…”
Section: Introductionmentioning
confidence: 99%
“…We make use here of the formally exact formulation for the scattering of EM waves in the form of surface integral equations by means of the Green's theorem. [35][36][37] This formulation has been used to investigate the EM field scattered from one-dimensional, randomly rough metal surfaces with arbitrarily large roughness. 22,38 Furthermore, by invoking the approximation ͑1͒, numerical results for the near-field enhancements at the pump frequency have been used to infer SERS enhancement factors.…”
Section: A Scattering Equationsmentioning
confidence: 99%