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通过包覆介电层实现银纳米粒子的可调偶极表面等离子体共振

Tunable Dipole Surface Plasmon Resonances of Silver Nanoparticles by Cladding Dielectric Layers.

作者信息

Liu Xiaotong, Li Dabing, Sun Xiaojuan, Li Zhiming, Song Hang, Jiang Hong, Chen Yiren

机构信息

1] State Key Laboratory of Luminescence and Applications, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, People's Republic of China [2] University of Chinese Academy of Sciences, Beijing 100039, People's Republic of China.

State Key Laboratory of Luminescence and Applications, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, People's Republic of China.

出版信息

Sci Rep. 2015 Jul 28;5:12555. doi: 10.1038/srep12555.

DOI:10.1038/srep12555
PMID:26218501
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4517390/
Abstract

The tunability of surface plasmon resonance can enable the highest degree of localised surface plasmon enhancement to be achieved, based on the emitting or absorbing wavelength. In this article, tunable dipole surface plasmon resonances of Ag nanoparticles (NPs) are realized by modification of the SiO2 dielectric layer thicknesses. SiO2 layers both beneath and over the Ag NPs affected the resonance wavelengths of local surface plasmons (LSPs). By adjusting the SiO2 thickness beneath the Ag NPs from 5 nm to 20 nm, the dipole surface plasmon resonances shifted from 470 nm to 410 nm. Meanwhile, after sandwiching the Ag NPs by growing SiO2 before NPs fabrication and then overcoating the NPs with various SiO2 thicknesses from 5 nm to 20 nm, the dipole surface plasmon resonances changed from 450 nm to 490 nm. The SiO2 cladding dielectric layer can tune the Ag NP surface charge, leading to a change in the effective permittivity of the surrounding medium, and thus to a blueshift or redshift of the resonance wavelength. Also, the quadrupole plasmon resonances were suppressed by the SiO2 cladding layer because the dielectric SiO2 can suppress level splitting of surface plasmon resonances caused by the Ag NP coupling effect.

摘要

基于发射或吸收波长,表面等离子体共振的可调谐性能够实现最高程度的局域表面等离子体增强。在本文中,通过改变SiO₂介电层厚度实现了银纳米颗粒(NPs)的可调谐偶极表面等离子体共振。银纳米颗粒下方和上方的SiO₂层均会影响局域表面等离子体(LSPs)的共振波长。通过将银纳米颗粒下方的SiO₂厚度从5nm调整至20nm,偶极表面等离子体共振从470nm移至410nm。同时,在制造纳米颗粒之前通过生长SiO₂将银纳米颗粒夹在中间,然后用5nm至20nm的各种SiO₂厚度覆盖纳米颗粒后,偶极表面等离子体共振从450nm变为490nm。SiO₂包层介电层可以调节银纳米颗粒表面电荷,导致周围介质有效介电常数发生变化,从而使共振波长发生蓝移或红移。此外,SiO₂包层会抑制四极等离子体共振,因为介电SiO₂可以抑制由银纳米颗粒耦合效应引起的表面等离子体共振的能级分裂。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/e0283d0be86f/srep12555-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/c15b8cf491ef/srep12555-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/3b73fe823e7d/srep12555-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/43267c5879a7/srep12555-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/e0283d0be86f/srep12555-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/c15b8cf491ef/srep12555-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/3b73fe823e7d/srep12555-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/43267c5879a7/srep12555-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f8e/4517390/e0283d0be86f/srep12555-f4.jpg

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