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用于表面增强拉曼光谱的介电二聚体阵列中的晶格共振和局部场增强

Lattice Resonances and Local Field Enhancement in Array of Dielectric Dimers for Surface Enhanced Raman Spectroscopy.

作者信息

Černigoj Jernej, Silvestri Fabrizio, Stoevelaar L Pjotr, Berzinš Jonas, Gerini Giampiero

机构信息

The Netherlands Organization for Applied Scientific Research, TNO, Optics Department, 2628CK, Delft, The Netherlands.

Eindhoven University of Technology, TU/e, Electromagnetics Group, 5600MB, Eindhoven, The Netherlands.

出版信息

Sci Rep. 2018 Oct 24;8(1):15706. doi: 10.1038/s41598-018-33941-7.

Abstract

In this paper, we propose the use of high refractive index dimers for the realization of a surface enhanced Raman spectroscopy substrate, with an average enhancement factor comparable to plasmonic structures. The use of low loss dielectric materials is favorable to metallic ones, because of their lower light absorption and consequently a much lower heating effect of the substrate. We combined two different mechanisms of field enhancement to overcome the main weakness of dielectric dimers: a low enhancement factor compared to the plasmonic ones. A first mechanisms is associated to surface lattice resonances. This generates a narrow-band high enhancement, which is exploited to enhance the excitation light. A second mechanism exploits the local field enhancement between the dimers' resonators, for the band where the molecule Raman emission spectrum is located. The fact that both field enhancements can be tuned by acting on separate geometric parameters, makes possible to optimize the design for many different molecules. The optimized structure and its performance is presented together with a discussion of the different enhancement mechanisms.

摘要

在本文中,我们提出使用高折射率二聚体来实现表面增强拉曼光谱基底,其平均增强因子与等离子体结构相当。使用低损耗介电材料优于金属材料,因为它们的光吸收较低,因此基底的热效应要低得多。我们结合了两种不同的场增强机制,以克服介电二聚体的主要弱点:与等离子体二聚体相比增强因子较低。第一种机制与表面晶格共振有关。这会产生窄带高增强,可用于增强激发光。第二种机制利用二聚体谐振器之间的局部场增强,用于分子拉曼发射光谱所在的波段。两种场增强都可以通过调整不同的几何参数来调节,这使得针对许多不同分子优化设计成为可能。本文展示了优化后的结构及其性能,并讨论了不同的增强机制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0cbf/6200810/bc45ae79acd0/41598_2018_33941_Fig1_HTML.jpg

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