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Titlebook: Electromagnetic Theory of Gratings; Roger Petit Book 1980 Springer-Verlag Berlin Heidelberg 1980 Gitter (Optik).diffraction.dispersion.ele

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https://doi.org/10.1007/978-3-030-72756-7mentalists, or recently discovered. They are grating anomalies, usually referred to as Wood anomalies, total absorption of a plane wave by a metallic grating (bare or coated with a thin dielectric layer) as well as the coupling of a laser beam into an optical waveguide by means of a holographic thin
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Creating a SQL Health Repository, We must lay stress on the fact that the properties described below are mainly those which cannot be found in classical optics text books because they are in fact consequences of the electromagnetic theory. After a lot of valuable experimental verifications, this theory is used to obtain numerous ef
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https://doi.org/10.1007/978-3-030-72756-7ions and the associated boundary conditions on the grating surface, without any wave impinging on the structure. It is the study of such a solution that we call the “homogeneous problem” and we wish to show how the resolution of the homogeneous problem can enlighten the study of the response of the
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The Homogeneous Problem,ions and the associated boundary conditions on the grating surface, without any wave impinging on the structure. It is the study of such a solution that we call the “homogeneous problem” and we wish to show how the resolution of the homogeneous problem can enlighten the study of the response of the
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0342-6793 e of thumb was generally sufficient to make good use of the optical gratings available about thirty years ago. Thanks to the spectacular improvements in grating978-3-642-81502-7978-3-642-81500-3Series ISSN 0342-6793
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Book 1980ity insofar as the diffracted wave vector can be deduced from the incident one by a specular reflexion on the large facet. Actually this rule of thumb was generally sufficient to make good use of the optical gratings available about thirty years ago. Thanks to the spectacular improvements in grating
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Differential Methods,quations, but, as outlined in Chap. 1, it is possible to solve directly these differential equations. The method related in this chapter is equivalent to, but slightly different from, the scheme previously described in Chap. 1. It takes a place among the so-called differential methods that we shall classify into three categories:
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