influence du potentiel rugueux crée par l'interférence entre l'ondé evanescente et lalumì ere diffusée par la surface du diélectrique. Le lecteur y trouvera en particulier la généralisation de l'approche de RAYLEIGHàRAYLEIGH`RAYLEIGHà une interface diélectrique?vide ( § III) dont nous nous servons pour calculer le champ lumineux diffusé. Dans l'article, nous nous concentrons sur l'approximation scalaire pour le champ lumineux. A l'annexe § B, nous donnons le champ lumineux diffusé en tenant compte de la polarisation, p.1160, 1997. ,
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89 5.2.1 La condition de réflexion pour, p.92 ,
103 6.2.1 Incidence normale ,
176 8.2.1 Calcul de la figure de diffraction, 176 8.2.2 Equivalencè a un réseau de phase mince . . . . . . . . . . . . 178 ,
183 8.3.1 Formulation dans l'esprit de l'optique géométrique, p.186 ,
C Les phases des amplitudes de diffraction : différence par rapportàrapport`rapportà l'approximation, p.230 ,
238 9.2.1 Calcuì a l'intérieur des ordres fortement couplés, p.239 ,
258 10.3.1 Calcul perturbatif des amplitudes de diffraction, p.261 ,
267 11.1.2 Le mécanisme de la diffraction, p.293 ,
293 Introduction, p.300 ,
329 13.1.1 Le profile de surface, Ergodicité, p.337 ,
359 14.2.1 Le coefficient de réflexion moyen, p.362 ,
370 15.1.1 L'interaction de VAN DER WAALS en présence de rugosité ,