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使用超薄半导体光栅在可见光范围内实现近完美(>99%)的双波段吸收。

Near-perfect (>99%) dual-band absorption in the visible using ultrathin semiconducting gratings.

作者信息

Gong Tao, Munday Jeremy N

出版信息

Opt Express. 2022 Sep 26;30(20):36500-36508. doi: 10.1364/OE.470617.

Abstract

Electromagnetic perfect absorption entails impedance-matching between two adjacent media, which is often achieved through the excitation of photonic/plasmonic resonances in structures such as metamaterials. Recently, super absorption was achieved using a simple bi-layer configuration consisting of ultrathin lossy films. These structures have drawn rising interest due to the structural simplicity and mechanical stability; however, the relatively broadband absorption and weak angular dependence can limit its versatility in many technologies. In this work, we describe an alternative structure based on an ultrathin semiconducting (Ge) grating that features a dual-band near-perfect resonant absorption (99.4%) in the visible regime. An angular-insensitive resonance is attributed to strong interference inside the ultrathin grating layer, akin to the resonance obtained with a single ultrathin planar film, while an angular-sensitive resonance shows a much narrower linewidth and results from the diffraction-induced surface mode coupling. With an appropriately designed grating period and thickness, strong coherent coupling between the two modes can give rise to an avoided-crossing in the absorption spectra. Further, the angular-insensitive resonance can be tuned separately from the angularly sensitive one, yielding a single narrow-banded absorption in the visible regime and a broadband absorption resonance that is pushed into the near-infrared (NIR). Our design creates new opportunities for ultra-thin and ultra-compact photonic devices for application in technologies including image sensing, structural color-filtering and coherent thermal light-emission.

摘要

电磁完美吸收需要相邻两种介质之间实现阻抗匹配,这通常通过激发诸如超材料等结构中的光子/等离子体共振来实现。最近,利用由超薄损耗膜组成的简单双层结构实现了超吸收。由于结构简单和机械稳定性,这些结构引起了越来越多的关注;然而,相对较宽的吸收带宽和较弱的角度依赖性可能会限制其在许多技术中的通用性。在这项工作中,我们描述了一种基于超薄半导体(Ge)光栅的替代结构,该结构在可见光范围内具有双波段近完美共振吸收(99.4%)。角度不敏感共振归因于超薄光栅层内部的强干涉,类似于用单个超薄平面膜获得的共振,而角度敏感共振显示出窄得多的线宽,是由衍射诱导的表面模式耦合引起的。通过适当设计光栅周期和厚度,两种模式之间的强相干耦合可以在吸收光谱中产生避免交叉。此外,角度不敏感共振可以与角度敏感共振分开调谐,在可见光范围内产生单个窄带吸收,并将宽带吸收共振推至近红外(NIR)。我们的设计为超薄和超紧凑光子器件创造了新机会,可应用于包括图像传感、结构滤色和相干热发光等技术。

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