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hal.structure.identifierEcole Nationale Supérieure des Mines de St Etienne [ENSM ST-ETIENNE]
hal.structure.identifierLaboratoire Georges Friedel [LGF-ENSMSE]
dc.contributor.authorGRUY, Frédéric
hal.structure.identifierLaboratoire Ondes et Matière d'Aquitaine [LOMA]
hal.structure.identifierLaboratoire Ondes et Matière d'Aquitaine [LOMA]
dc.contributor.authorPERRIN, Mathias
hal.structure.identifierDépartement de Mathématiques et Applications - ENS Paris [DMA]
dc.contributor.authorRABIET, Victor
dc.description.abstractEnIn classical Physics, the Lippmann-Schwinger equation links the field scattered by an ensemble of particles-of arbitrary size, shape and material-to the incident field. This singular vectorial integral equation is generally formulated and solved in the direct space R n (typically, n = 2 or n = 3), and often approximated by a scalar description that neglects polarization effects. Computing rigorously the Fourier transform of the fully vectorial Lippmann-Schwinger equation in S (R 3), we obtain a simple expression in the Fourier space. Besides, we can draw an explicit link between the shape of the scatterer and the scattered field. This expression gives a general, tridimensional, picture of the well known Rayleigh-Sommerfeld expression of bidimensional scattering through small apertures.
dc.language.isoen
dc.title.enFourier transform of the Lippmann-Schwinger equation for 3D Vectorial Electromagnetic Scattering : a direct relationship between fields and shape
dc.typeDocument de travail - Pré-publication
dc.subject.halPhysique [physics]/Physique [physics]/Optique [physics.optics]
dc.subject.halPhysique [physics]/Physique mathématique [math-ph]
hal.identifierhal-03043716
hal.version1
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-03043716v1
bordeaux.COinSctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.au=GRUY,%20Fr%C3%A9d%C3%A9ric&PERRIN,%20Mathias&RABIET,%20Victor&rft.genre=preprint


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