Spectral tunability of the spacer layer in metasurface absorbers (Presentation Recording)

Kai Liu, N. Zhang, Dengxin Ji, Haomin Song, Xie Zeng, Qiaoqiang Gan
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Abstract

Potential solar energy applications of metamaterial absorbers require spectrally tunable resonance to ensure the overlap with intrinsic absorption profiles of active materials. Although those resonance peaks of metamaterial absorbers can be tuned precisely by lithography-fabricated nanopatterns with different lateral dimensions, they are too expensive for practical large-area applications. In this work, we will report another freedom to tune the spectral position of the super absorbing resonance, i.e. the spacer thickness. The structure was fabricated by evaporating an optically opaque metallic ground plate, a dielectric spacer layer, and a top metallic thin film followed by thermal annealing processes to form discrete nanoparticles. As the spacer thickness increases from 10-90 nm, two distinct shifts of the absorption peak can be observed [i.e. a blue-shift for thinner (10-30 nm) and a red-shift for thicker spacer layers (30-90 nm)]. To understand the physical mechanism, we characterized effective optical constants of top nanopattern layer and loaded them into numerical simulation models. A good agreement with experimental data was only observed in the thick spacer region (i.e. 30-90 nm). The optical behavior for thinner spacers cannot be explained by effective medium theory and interference mechanism. Therefore, a microscopic study has to be performed to reveal strongly coupled modes under metallic nanopatterns, which can be interpreted as separate antennas strongly coupled with the ground plate. Since the resonant position is sensitive to the spacer thickness, a tunable super absorbing metasurface is realizable by introducing spatial tunable materials like stretchable chemical/ biomolecules.
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超表面吸收器中间隔层的光谱可调性(报告记录)
超材料吸收器的潜在太阳能应用需要光谱可调共振,以确保与活性材料的本征吸收曲线重叠。虽然这些超材料吸收器的共振峰可以通过光刻制造的具有不同横向尺寸的纳米图案来精确调谐,但它们对于实际的大面积应用来说过于昂贵。在这项工作中,我们将报道另一个调节超吸收共振光谱位置的自由度,即间隔层厚度。该结构是通过蒸发一个光学不透明的金属接地板、一个介电间隔层和一个顶部金属薄膜,然后通过热退火过程形成离散的纳米颗粒来制造的。当间隔层厚度从10- 90nm增加时,可以观察到吸收峰的两个明显的位移[即较薄的间隔层(10- 30nm)的蓝移和较厚的间隔层(30- 90nm)的红移]。为了了解其物理机制,我们表征了顶部纳米图案层的有效光学常数,并将其加载到数值模拟模型中。仅在厚间隔区(即30-90 nm)观察到与实验数据吻合良好。较薄间隔片的光学特性不能用有效介质理论和干涉机理来解释。因此,必须进行微观研究以揭示金属纳米模式下的强耦合模式,这可以解释为与接地板强耦合的单独天线。由于共振位置对间隔层厚度敏感,因此可以通过引入可拉伸化学/生物分子等空间可调材料来实现可调超吸收超表面。
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