Method and device for realizing wave absorbing of graphene at visible light waveband
A graphene and visible light technology, applied in optics, optical components, instruments, etc., can solve the problems of sensitivity to incident angle changes, low light absorption efficiency, narrow light absorption bandwidth, etc.
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Embodiment 1
[0039] Example 1: Broadband absorption of graphene in the visible light band based on a multi-groove structure
[0040] A multi-groove structure is used to design a graphene broadband absorber in the visible light band. A cell of the multi-groove structure is composed of five narrow metal grooves with the same width and different depths. The metal grooves and their tops are filled with dielectric materials. layer, and graphene is deposited over the dielectric material capping layer. For TM polarized incident light, due to the cavity resonance effect of metal grooves, grooves with different depths correspond to different light absorption wavelengths of graphene. The combination of five grooves with different depths can enhance the interaction between light and graphene in the visible light band. Further, the broadband light absorption enhancement of graphene in the visible light band can be realized.
[0041] The selected design band is the visible light band (400-800nm), and ...
Embodiment 2
[0042] Example 2: A method for regulating graphene light absorption channels based on a single groove structure
[0043] Compared with the multi-groove structure, there is only one metal groove in a primitive cell of the single-groove structure. By changing the depth of the metal groove in the single groove structure, the light wavelength corresponding to the cavity resonance of the metal groove is changed, thereby changing the position of the light absorption channel of the graphene. Therefore, for the single groove structure, by selecting different groove depths, the selective light absorption enhancement of graphene can be achieved at different wavelength positions.
[0044] Under the condition of keeping the structure parameters of multi-groove unchanged, the five grooves in the original cell are reduced to one groove, and the width w of the groove remains unchanged, that is, the structural parameters are: Λ=300nm, t=5nm, w=30nm, D=100nm, using FDTD method, combined with ...
Embodiment 3
[0045] Example 3: Angle-insensitive broadband light absorption based on multi-groove structure graphene
[0046] Based on Example 1, under the condition of keeping the structural parameters unchanged, that is, Λ=300nm, t=5nm, w=30nm, D=100nm, d 1 =20nm, d 2 =35nm, d 3 = 50nm, d 4 =80nm, d 5 =90nm, adopt the FDTD method, and in conjunction with formula (4), calculate the influence of incident angle variation on the graphene absorption spectrum curve of multi-groove structure, get Figure 4 . From Figure 4 It can be seen that the graphene broadband absorber based on the multi-groove structure has a very high angle tolerance because the change of the incident angle has little effect on the cavity resonance effect. When the incident angle increases from 0° to 60°, graphene still has Excellent broadband light absorption effect, this feature has extremely high application value.
[0047] In practical applications, the metal can be deposited on the substrate by means of elect...
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