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Negative refraction in Photonic Crystals: thickness dependence and Pendellösung phenomenon

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Abstract

We show that the refracted wave at the exit surface of a Photonic Crystal (PhC) slab is periodically modulated, in positive or in negative direction, changing the slab thickness. In spite of an always increasing literature, the effect of the thickness in negative refraction on PhC’s does not seem to be appropriately considered. However such an effect is not surprising if interpreted with the help of Dynamical Diffraction Theory (DDT), which is generally applied in the x-ray diffraction. The thickness dependence is a direct result of the so-called Pendellösung phenomenon. That explains the periodic exchange, inside the crystal, of the energy among direct beam (or positively refracted) and diffracted beam (or negatively refracted). The Pendellösung phenomenon is an outstanding example of the application of the DDT as a powerful and simple tool for the analysis of s electromagnetic interaction in PhC’s.

©2005 Optical Society of America

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Figures (4)

Fig. 1.
Fig. 1. Dispersion surfaces in crystal in the long wavelength limit: the medium can be considered as homogeneous (a). Decreasing the wavelength, the spheres approach and a Bragg gap appears (b).
Fig. 2.
Fig. 2. The crystal dispersion surface, which determines the permitted wavevectors in the structure for a given frequency is a hyperbola (thick line) close to the Bragg gap. In the figure are also shown dispersion surfaces in the air, which are spheres. The intersections of the hyperbola asymptotes in vacuum, the Lorentz point (Lo) and the Laue point (La) respectively, are also indicated.
Fig. 3.
Fig. 3. Electric field obtained via a FEM simulation in a 2D square lattice PhC with filling factor r/a=0.1. The cylinders have a real dielectric constant ε=3 embedded in vacuum. The polarization is chosen with the electric field (shown in the figure) parallel to the cylinder axis. The wavelength λ satisfies the Bragg law in vacuum with an incidence angle θi =60°, i.e. I0La in Fig. 2. (a) Slab thickness t=6a0/2: the maximum intensity is in the diffracted direction and exhibits negative refraction behavior. (b) t=12a0 ; (c) t=18a=3/2 Λ0 ; (d) t=24a=2Λ0. The Pendellösung exchange of energy between positive and negative refracted beam corresponds to the thickness period Λ0 as calculated from (2).
Fig. 4.
Fig. 4. FEM simulation of a PhC with the same characteristics as in Fig. 3 and a thickness t=6a. Square modulus of the electric field parallel to the cylinder axis for an incident angle θi =55° (a), and θi =65° (b). The detail (c) shows the modulus of the electric field inside the PhC.

Equations (2)

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X 0 X h = k 2 χ h χ h 4 ( 1 + χ 0 )
Λ 0 = λ cos θ B 1 + χ 0 χ h χ h
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