99 research outputs found
The exact theory for scattering of waves by thick holes in a slab and other objects with non-separable geometries
The theory for scattering of electromagnetic waves is developed for scattering objects for which the natural modes of the field inside the object do not couple one-to-one with those outside the scatterer. Key feature of the calculation of the scattered fields is the introduction of a new set of modes. As an example, we calculate the reflected and transmitted fields generated by an electromagnetic plane wave that impinges upon a multilayer slab of which the layers are stacked perpendicular to the boundary planes. As this is the geometry of a thick plate with slits our theory encompasses the exact scattering theory of electromagnetic waves by a thick plate with slits.
Quasi Normal Modes description of transmission properties for Photonic Band Gap structures
In this paper, we use the 'Quasi Normal Modes' (QNM) approach for discussing
the transmission properties of double-side opened optical cavities: in
particular, this approach is specified for one dimensional (1D) 'Photonic Band
Gap' (PBG) structures. Moreover, we conjecture that the density of the modes
(DOM) is a dynamical variable which has the flexibility of varying with respect
to the boundary conditions as well as the initial conditions; in fact, the e.m.
field generated by two monochromatic counter-propagating pump waves leads to
interference effects inside a quarter-wave (QW) symmetric 1D-PBG structure.
Finally, here, for the first time, a large number of theoretical assumptions on
QNM metrics for an open cavity, never discussed in literature, are proved, and
a simple and direct method to calculate the QNM norm for a 1D-PBG structure is
reported.Comment: 43 pages, 10 figures, submitted to JOSA
On the Reconstruction of a Weak Phase-Amplitude Object. I
In this paper we consider the reconstruction of a weak amplitude-phase object. We mean by this reconstruction of the wave function in a plane directly behind the object. The program is carried through with the aid of two measurements of the contrast, corresponding to different values of the defocusing
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