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N -layered glass-anisotropic metamaterial-semiconductor cylinder model and designations  

N -layered glass-anisotropic metamaterial-semiconductor cylinder model and designations  

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We present here dependencies of scattered and absorbed powers of incident perpendicularly and parallel polarized microwaves by a multilayered cylinder. We consider here the normal (angle θ=90∘) and oblique (angles θ=60∘,30∘,5∘) incidence of microwave on the cylinder. The one consists of a glass core that is coated by the six anisotropic metamateria...

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Context 1
... equations for the multilayer cylinder was carried out by the partial area method [12][13][14]. The central core of the multi- layered cylinder was made of glass material. The glass core is coated by a sandwich semiconductor-metamaterial cover. The multilayered cylinder consists of seven concentric sur- faces with radii R j , j = 1, 2, . . . , N (Fig. 1). The every j th region is filled with a material having the permittivity ε j and the permeability μ j . Numbering of layers is going from the outside layer to the inner one. Thus, R 1 is the outside radius of the cylinder. In our calculations N = 7, i.e., the glass core with radius R 7 is coated with 6 layers of metamaterial and n- Si ...
Context 2
... in the plane x0z and the direction of microwave propagation is described by an angle θ between the z-axis and the wave vector k (Fig. 1). Here, E 0 is the amplitude of the electric field of an incident microwave. The vector E 0 determines the polarization of the incident microwave. The direction of vector E 0 is defined by the angle ψ that is between the vector E 0 and the y-axis. The EM wave has the parallel polarization when the angle ψ is equal to 90 • ...

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