通过改变各向异性和粒子间相互作用嵌入电介质中的金纳米粒子的光谱调谐:形状与相互作用之间的数学关系

J. K. Majhi
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引用次数: 0

摘要

分别对各向异性非相互作用金纳米粒子(NPs)和嵌入介质基体的球形相互作用金纳米粒子的光吸收特性进行了理论研究。对于这些研究,我们考虑了一种改进的Garcia等人的模型,该模型依赖于Maxwell-Garnett (MG)理论,其中粒子的各向异性用参数β表示,称为形状参数,相互作用用参数K表示。对于各向异性粒子的OA谱的计算,β的值从0.05变化到1.0,考虑K = 0并保持粒子半径固定在R = 2 nm。各向异性Au NPs的OA光谱在500 ~ 832 nm范围内表现出表面等离子体共振(SPR)的大红移,与相同尺寸的球形非相互作用粒子在520 nm左右的红移相反。SPR峰值位置随β的增加呈指数型衰减。在相同粒径的球形Au NPs中,当相互作用参数K在20 ~ 80之间变化时,可以观察到OA光谱的相似性质和SPR峰随K减小的衰减行为。观测结果给出了参数β和K之间的相关性,这是不确定的。这种相关性对于各向异性金纳米粒子在等离子体、表面增强拉曼散射(SERC)、光子学、光电子学等领域的不同应用是必不可少的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spectral Tuning of Gold Nanoparticles Embedded in Dielectric by Changing Anisotropy and Interparticle Interaction: A Mathematical Correlation between the Shape and Interaction
The theoretical studies of optical absorption (OA) properties of anisotropic non-interacting Au nanoparticles (NPs) and the spherical interacting Au NPs embedded in dielectric matrix have been carried out separately. For the studies we have considered a modified Garcia et al. model depend on Maxwell-Garnett (MG) theory where anisotropy of the particles are represented by a parameter β known as shape parameter and interaction is represented by the parameter K. For calculation of OA spectra of anisotropic particles, the values of β is varied from 0.05 to 1.0, considering K = 0 and keeping particle radius fixed at R = 2 nm. The OA spectra of anisotropic Au NPs in the above range of β exhibit a large redshift of surface plasmon resonance (SPR) from 500 - 832 nm in contrary to what is observed for spherical non-interacting particle of same size at an around 520 nm. An exponential type decay of SPR peak position with increase of β has also been observed. The almost similar nature of OA spectra and the decay behavior of the SPR peak with decrease of K have also been observed for interacting spherical Au NPs by varying the interaction parameter K from 20 to 80 of same particle size. The observation gives a correlation between the parameter β and K which was not established. This correlation is essential and helpful for different applications of anisotropic Au nanoparticles in plasmonic, surface enhanced Raman scattering (SERC), photonics, optoelectronics, and others.
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