Dual-band visible light broadband absorption structure and preparation method thereof
An absorption structure and visible light technology, applied in optics, optical components, instruments, etc., can solve the problems of sensitivity to incident light angle, complex design structure, and inability to mass-produce, and achieve high absorption efficiency, wide application, and high absorption efficiency. small effect
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[0068] The cross-sectional structure of a dual-band visible light broadband absorbing structure involved in an embodiment of the present invention is as follows: figure 1 As shown, it includes a substrate 110 , a metal layer 111 , a metal grating layer 112 and a filling medium 113 . Wherein, the material of the base 110 is a transparent flexible material, such as polyester (PET), polycarbonate (PC), polyvinyl chloride (PVC), polymethyl methacrylate (PMMA) or polypropylene (BOPP). The metal layer 111 is located on the substrate 110 and its material is, for example, aluminum, silver, copper, tungsten, nickel, chromium or titanium. The metal layer 111 acts as a reflector. In order to ensure light reflection efficiency, the thickness d of the metal layer 111 is greater than the skin depth of visible light on the metal material. In one embodiment, the thickness of the metal layer 111 is 100nm. The metal grating layer 112 is located on the metal layer 111 and its material is, for ...
Embodiment 1
[0072] figure 2 and image 3 The relationship between the absorption spectrum of TM polarized light and TE polarized light of the broadband absorbing structure designed for the present invention, incident angle and incident wavelength. Wherein, p is 260nm, f is 0.25, h is 300nm, d is 100nm, the material of the metal layer and the metal grating layer is nickel, and the filling medium is silicon dioxide. The absorption characteristics and angle tolerance of broadband absorbing structures are analyzed by rigorous coupled wave theory (RCWA). Due to the coupling of surface plasmons excited by TM polarized light in the medium, a strong magnetic field resonance is formed to realize light energy capture, resulting in high-efficiency absorption. The mechanism of high absorption of TE polarized light lies in the formation of an open cavity between the filling medium and the metal walls on both sides, and the high absorption caused by cavity resonance. It can be found that both TM an...
Embodiment 2
[0074] Figure 4 and Figure 5 The relationship diagrams of the absorption spectra of the TM polarized light and the TE polarized light of the visible light broadband absorption structure with the period of the metal grating layer and the incident wavelength are respectively shown. In this embodiment, the period p of the metal grating is adjusted, and the influence of the change of p on the absorption spectrum of the structure is observed. Other structural parameters are the same as those in Embodiment 1, and the incident angle is 0 degree. It can be found that the period variation has a great influence on the TM light absorption, and preferably, the absorption bandwidth near the period of 250 nm is large and the efficiency is high. Period has little effect on TE polarized light.
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