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可视化低折射率介质纳米粒子中的米氏共振。

Visualizing Mie Resonances in Low-Index Dielectric Nanoparticles.

机构信息

Department of Electrical Engineering and Computer Science, The University of Michigan, Ann Arbor, Michigan 48109, USA.

State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, 500 Yutian Road, Shanghai 200083, China.

出版信息

Phys Rev Lett. 2018 Jun 22;120(25):253902. doi: 10.1103/PhysRevLett.120.253902.

Abstract

Resonant light scattering by metallic and high-index dielectric nanoparticles has received enormous attention and found many great applications. However, low-index dielectric nanoparticles typically do not show resonant scattering behaviors due to poor light confinement caused by small index contrast. This Letter describes a simple and effective approach to drastically enhance the resonance effect of the low-index particles by partial metal dressing. Mie resonances of low-index nanoparticles can now be easily visualized by scattered light. This scattering peak depends on sphere size and has a reasonable linewidth. A size difference as small as 8 nm was resolved by a peak shift or even by color change. The scattering peak is attributed to the enhanced TE_{11} Mie resonance of the low-index nanospheres. The metal dress not only provides a high-reflection boundary, but also functions as an antenna to couple the confined light power to the far field, leading to scattering maxima in the spectra. Additionally, the enhanced TE_{11} Mie resonance in low-index nanoparticles features a considerable magnetic response due to the strong circulating displacement currents induced by the intensified E field despite of a low permittivity (hence low index) of the particles. The enhanced Mie resonances could be used to sense minute changes in size or refractive index of low-index nanoparticles and benefit a wide range of applications.

摘要

金属和高折射率介质纳米粒子的共振光散射引起了人们的极大关注,并找到了许多重要的应用。然而,由于小的折射率对比度导致光限制较差,低折射率介质纳米粒子通常不表现出共振散射行为。本信描述了一种简单而有效的方法,通过部分金属修饰来显著增强低折射率粒子的共振效应。现在可以通过散射光很容易地观察到低折射率粒子的米氏共振。这个散射峰取决于球体的大小,并且具有合理的线宽。通过峰位移甚至颜色变化,就可以分辨出小至 8nm 的尺寸差异。散射峰归因于低折射率纳米球的增强的 TE_{11}米氏共振。金属修饰不仅提供了一个高反射边界,而且还作为一个天线将受限光功率耦合到远场,从而在光谱中产生散射最大值。此外,由于被加强的 E 场引起的强循环位移电流,尽管粒子的介电常数(因此折射率)较低,但低折射率纳米粒子中的增强的 TE_{11}米氏共振具有相当大的磁响应。增强的米氏共振可用于感测低折射率纳米粒子的尺寸或折射率的微小变化,并有益于广泛的应用。

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