Design method for pure medium electromagnetic lens based on meta-surface
An artificial electromagnetic surface and electromagnetic lens technology, applied in electrical components, optics, instruments, etc., can solve the problems of sub-wavelength structure design, difficult processing, narrow working frequency band, difficult to apply, etc., and achieve easy design and implementation, working frequency The effect of simple bandwidth and design method
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Embodiment 1
[0032] The present invention considers that the ultimate goal of the artificial electromagnetic surface of the metal structure is to realize the phase mutation of the secondary Huygens source, and there is another means to realize the phase mutation——change the thickness of the electromagnetic wave propagation medium, and the present invention designs a pure medium electromagnetic lens. Its working principle is as follows: the present invention uses figure 1 (a) As an example, suppose a beam of TE electromagnetic wave with θ i Angular oblique incident to a certain unit of the lens, the unit can be regarded as the mnth unit in the two-dimensional plane, the period length is one-half of the wavelength (L=λ 0 / 2), incident plane xz ⊥mn . Assuming that each unit is a uniform plane dielectric layer, the present invention can obtain a two-port network model according to the transmission line theory, such as figure 1 Shown in (b), on (z=0), down (z=h mn ) surface TE wavefields c...
Embodiment 2
[0050] Such as Figure 6 As shown, the present invention provides a kind of design method based on the pure dielectric electromagnetic lens of artificial electromagnetic surface, and this method comprises the steps:
[0051] Step 1: Obtain the relationship between the phase change and the thickness of the medium according to the medium material used in the lens and the wavelength of the working electromagnetic wave;
[0052] According to the formula: Obtain the relationship between the electromagnetic wave phase change and the thickness of the medium, where β = ω ( ϵ r - sin 2 θ i ) ϵ 0 μ 0 , Z c ...
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