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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Plasmonic Metasurfaces with Tunable Gap and Collective Surface Plasmon Resonance Modes
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Plasmonic Metasurfaces with Tunable Gap and Collective Surface Plasmon Resonance Modes

机译:具有可调差距和集体表面等离子体共振模式的等离子体元件

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摘要

Optical properties of a plasmonic metasurface made of a monolayer of gold nanoparticles in close proximity to an aluminum thin film were studied numerically and experimentally. Extinction spectra of the plasmonic metasurface were studied as functions of the thickness of a dielectric spacer between the monolayer of gold nanoparticles and the aluminum film in the visible wavelength range. The goal was to understand the excitation of a collective surface plasmon resonance (SPR) mode and a gap plasmon mode as well as their dependence on the spacer thickness, nanoparticles spacing, and their size. By using finite-difference-time-domain (FDTD) calculations, we find that the SPR extinction peak first red-shifts and then splits into two peaks. The first extinction peak is associated with the collective SPR mode of the monolayer, and it shifts to shorter wavelengths as the spacer layer decreases. As the spacer layer decreases from 35 to 7.5 nm, the second peak gradually appears in the extinction spectra of the metasurface. We assign the second peak to the gap mode. The gap mode first appears at around 620 nm or greater, and it shifts to larger wavelength for larger nanoparticle spacing and size. The FDTD simulations are confirmed by an experimental examination of the dispersion curves of a similar multilayer system. The computational results match the experimental results and confirm the excitation of the two modes.
机译:在数值和实验中研究由由铝薄膜紧密接近的金纳米颗粒的单层金纳米颗粒制成的等离子体元表面的光学性质。等离子体元表面的消光光谱作为介电间隔物在可见波长范围内的金纳米颗粒和铝膜之间的介电隔离物的厚度的函数。目标是了解集体表面等离子体谐振(SPR)模式的激励和间隙等离子体模式以及它们对间隔厚度,纳米粒子间距及其尺寸的依赖性。通过使用有限差分时域(FDTD)计算,我们发现SPR消光峰值首先换档,然后分成两个峰。第一消光峰与单层的集体SPR模式相关联,并且随着间隔层减小,它变为较短的波长。随着间隔层从35到7.5nm减小,第二峰值逐渐出现在元表面的消光光谱中。我们将第二个峰值分配给间隙模式。间隙模式首先出现在620nm或更大范围内,并且它转向较大的纳米颗粒间距和尺寸的更大波长。通过对类似多层系统的分散曲线的实验检查来确认FDTD模拟。计算结果与实验结果匹配并确认两种模式的激发。

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