Broadband THz metamaterial absorber based on multi-resonant absorption superposition
A metamaterial, terahertz technology, applied in the field of terahertz absorbers, can solve the problems of difficulty, complex process, narrow single-peak resonance absorption bandwidth, etc., to achieve the effect of improving the frequency bandwidth, easy preparation process, and high process difficulty
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Embodiment 1
[0045] A broadband terahertz metamaterial absorber based on multi-resonance absorption superposition, the absorber includes an upper patterned functional material layer 1, a middle dielectric layer 2 and a lower metal reflective layer 3. Among them, the upper patterned functional material layer 1 uses metal phase vanadium dioxide as the material, and the conductivity of the upper patterned functional material layer 1 is 2.7×10 5 S / m, the thickness of the upper patterned functional material layer 1 is 0.3um. The geometric dimensions of the metamaterial unit structure of the upper patterned functional material layer 1 are: the arm length x of the connecting arm 14 is 7.5um, the line width m of the metamaterial unit structure is 3um, and the width d of the parallel opening 13 is 5um; The lattice period a of the cell structure array is 29um. The intermediate dielectric layer 2 adopts polyimide with a thickness h of 13um; the lower metal reflective layer 3 adopts a conductivity o...
Embodiment 2
[0048] The simulation calculation conditions of this embodiment are roughly the same as those of Embodiment 1, except that graphite is used as the material for the upper patterned functional material layer 1, and its conductivity is 1×10 5 S / m, the width d of the parallel openings 13 of the metamaterial unit structure is 9um, and the lattice period a of the metamaterial unit structure array is 27um.
[0049] The absorber structure in this embodiment is simulated and calculated for the absorption rate of the terahertz wave by the commercial software CST Microwave Studio 2014 frequency domain solver. The terahertz wave is perpendicular to the surface of the metamaterial absorber, and the magnetic and electric field polarizations perpendicular to each other The direction is parallel to the vertical direction of the cross in the array unit. The absorption spectrum calculated by simulation is as follows Figure 12 As shown, the peak absorption rate of the metamaterial absorber re...
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