Nouvelles conditions aux limites exactes pour les champs électromagnétiques à la surface des matériaux absorbants
Recent experiments using laser light by Langlois et al. have shown for the first time that actual diffraction patterns from edges do depend on the material and ridge shape of the scatterer, as well as on the polarization of the incident wave. These results have brought out the inadequacy of the scalar diffraction theory for diffraction angles larger than about 1°. Farther out one must use exact electromagnetic theory, with the attendant requirement that exact boundary conditions be known for the fields on the surface of the scattering object. These boundary conditions are well known for perfect conductors (Neumann's or Dirichlet's conditions) or even for good conductors (Leontovich's conditions). However, in the visible range one finds that copper is not a good conductor. Therefore, we develop in the present paper new exact boundary conditions, which generalize those of Leontovieh. In actual fact our new boundary conditions have enabled us to perform edge diffraction calculations for a considerably larger range of complex refraction indices covering the materials used. More generally one may claim that our boundary conditions do apply for all usual materials (copper, aluminium, ebonite … ), in as much as they are absorbing and the local ridge curvature of the scattering objects is far larger than the wavelength.