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3D multilayered plasmonic nanostructures with high areal density for SERS

机译:用于SERS的具有高面密度的3D多层等离子体纳米结构

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Enhancing light–matter interactions is essential to improving nanophotonic and optoelectronic device performance. In the present work, we developed a new design for 3D plasmonic nanostructures with enhanced near-field interactions among the plasmonic nanomaterials. The 3D plasmonic nanostructures consisted of multilayered bottom Ag/polydimethylsiloxane (PDMS) nanostructures, an alumina middle layer, and top Ag nanoparticles (NPs). High areal density PDMS nanoprotrusions were self-organized by a simple maskless plasma etching process. The conformal deposition of alumina using atomic layer deposition and Ag deposition produced 3D plasmonic nanostructures. These structures induced multiple near-field interactions between the ultrahigh-areal-density (1400 μm?2) top Ag NPs and the underlying Ag nanostructures, and among the top Ag NPs themselves. The high density of hot spots across the 3D space yielded highly efficient and widely tunable plasmonic responses across the entire visible range. The SERS signal enhancement measured at the 3D plasmonic nanostructures was 3.9 times the signal measured at the 2D multilayered structures and 48.0 times the signal measured at a Ag NP layer deposited onto a Si substrate. Finally, the 3D plasmonic nanostructures exhibited excellent uniformity with a variation of 6.8%, based on a microscale Raman mapping analysis. The excellent Raman signal uniformity can be attributed to the ultrahigh areal density of the Ag NPs and the uniform thickness of the alumina spacing layer.
机译:增强光与物质的相互作用对于改善纳米光子和光电器件的性能至关重要。在当前的工作中,我们开发了3D等离子体纳米结构的新设计,并增强了等离子体纳米材料之间的近场相互作用。 3D等离子体纳米结构由多层底部Ag /聚二甲基硅氧烷(PDMS)纳米结构,氧化铝中间层和顶部Ag纳米颗粒(NP)组成。高面密度PDMS纳米突起通过简单的无掩模等离子蚀刻工艺自组织。使用原子层沉积和Ag沉积的氧化铝共形沉积产生3D等离子体纳米结构。这些结构在超高面积密度(1400μm ?2 )顶部Ag NPs与下面的Ag纳米结构之间以及在顶部Ag NPs之间引起多个近场相互作用。他们自己。跨越3D空间的高密度热点在整个可见范围内产生了高效且可广泛调节的等离子体响应。在3D等离子体纳米结构上测量的SERS信号增强是2D多层结构上测量的信号的3.9倍,是在沉积到Si基板上的Ag NP层上测量的信号的48.0倍。最后,基于微尺度拉曼映射分析,3D等离子体纳米结构表现出出色的均匀性,变化为6.8%。出色的拉曼信号均匀性可归因于Ag NP的超高面密度和氧化铝间隔层的均匀厚度。

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