Hu Min, Novo Carolina, Funston Alison, Wang Haining, Staleva Hristina, Zou Shengli, Mulvaney Paul, Xia Younan, Hartland Gregory V
College of Optics and Photonics, CREOL & FPCE, University of Central Florida, Orlando, FL 32816-2700, USA.
J Mater Chem. 2008;18(17):1949-1960. doi: 10.1039/b714759g.
This article provides a review of our recent Rayleigh scattering measurements on single metal nanoparticles. Two different systems will be discussed in detail: gold nanorods with lengths between 30 and 80 nm, and widths between 8 and 30 nm; and hollow gold-silver nanocubes (termed nanoboxes or nanocages depending on their exact morphology) with edge lengths between 100 and 160 nm, and wall thicknesses of the order of 10 nm. The goal of this work is to understand how the linewidth of the localized surface plasmon resonance depends on the size, shape, and environment of the nanoparticles. Specifically, the relative contributions from bulk dephasing, electron-surface scattering, and radiation damping (energy loss via coupling to the radiation field) have been determined by examining particles with different dimensions. This separation is possible because the magnitude of the radiation damping effect is proportional to the particle volume, whereas, the electron-surface scattering contribution is inversely proportional to the dimensions. For the nanorods, radiation damping is the dominant effect for thick rods (widths greater than 20 nm), while electron-surface scattering is dominant for thin rods (widths less than 10 nm). Rods with widths in between these limits have narrow resonances-approaching the value determined by the bulk contribution. For nanoboxes and nanocages, both radiation damping and electron-surface scattering are significant at all sizes. This is because these materials have thin walls, but large edge lengths and, therefore, relatively large volumes. The effect of the environment on the localized surface plasmon resonance has also been studied for nanoboxes. Increasing the dielectric constant of the surroundings causes a red-shift and an increase in the linewidth of the plasmon band. The increase in linewidth is attributed to enhanced radiation damping.
本文综述了我们最近对单个金属纳米颗粒进行的瑞利散射测量。将详细讨论两种不同的系统:长度在30至80纳米之间、宽度在8至30纳米之间的金纳米棒;以及边长在100至160纳米之间、壁厚约为10纳米的中空金银纳米立方体(根据其确切形态称为纳米盒或纳米笼)。这项工作的目标是了解局域表面等离子体共振的线宽如何取决于纳米颗粒的尺寸、形状和环境。具体而言,通过研究不同尺寸的颗粒,确定了体相退相、电子 - 表面散射和辐射阻尼(通过与辐射场耦合导致的能量损失)的相对贡献。这种区分是可能的,因为辐射阻尼效应的大小与颗粒体积成正比,而电子 - 表面散射贡献与尺寸成反比。对于纳米棒,辐射阻尼是粗棒(宽度大于20纳米)的主导效应,而电子 - 表面散射是细棒(宽度小于10纳米)的主导效应。宽度介于这些极限之间的棒具有窄共振——接近由体相贡献确定的值。对于纳米盒和纳米笼,在所有尺寸下辐射阻尼和电子 - 表面散射都很显著。这是因为这些材料壁薄,但边长较大,因此体积相对较大。还研究了环境对纳米盒局域表面等离子体共振的影响。增加周围介质的介电常数会导致等离子体带发生红移并使线宽增加。线宽的增加归因于增强的辐射阻尼。