纳米管表面等离子体耦合

O. Stéphan, D. Taverna, M. Kociak, L. Henrard, K. Suenaga, C. Colliex
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引用次数: 1

摘要

为了研究孤立的单壁碳纳米管(SWCNTs)的介电响应,使用扫描透射电子显微镜在近场几何结构中进行了空间分辨电子能量损耗谱测量。考虑到这些纳米结构的局部各向异性,我们将光谱与不同层数的多壁碳纳米管(MWCNTs)的光谱进行了比较,并在连续介质理论的框架内进行了模拟。对于薄的MWCNTs,在15和19 eV下确定了两种极化模式,分别为切向和径向表面等离激元模式,这是由于纳米管内外表面两种表面模式的耦合造成的。我们最后表明,在15 eV时,swcnts的介电响应呈现单一能量模式,在介电模型中可以理解为MWCNTs表面等离子激元激发的薄层极限。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Surface Plasmon Coupling in Nanotubes
To investigate the dielectric response of isolated Single‐Walled Carbon Nanotubes (SWCNTs), spatially‐resolved Electron Energy‐Loss Spectroscopy measurements have been carried out using a Scanning Transmission Electron Microscope in a near‐field geometry. Spectra have been compared with those acquired on Multi‐Walled Carbon Nanotubes (MWCNTs) made of different numbers of layers, and with simulations performed within the framework of the continuum dielectric theory, taking into account the local anisotropic character of these nanostructures. For thin MWCNTs, two polarisation modes have been identified at 15 and 19 eV, indexed as tangential and radial surface plasmon modes respectively, resulting from the coupling of the two surface modes on the internal and external surfaces of the nanotubes. We finally show that the dielectric response of a SWCNT, displaying a single energy mode at 15 eV, can be understood in the dielectric model as the thin layer limit of surface plasmon excitation of MWCNTs.
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