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Plasmons in nanotube bundles

机译:纳米管束中的等离激元

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摘要

The collective electronic excitation (plasmon) modes of carbon nanotube bundles aligned in both two-and three-dimensional superiattices have been calculated. The series of modes obtained can be viewed as combination of three contributions: (i) a one-tubule contribution, (ii) a uniform 2D or 3D buk contribution, and (iii) a contribution related to the lattice structure. The one-tubule contribution is dominant for plasmon wavelenths small compared to intertubule distance a i.e.for aq 1. For large wavelenths aq1, however, thev then to those of the 2D or 3D uniform electron gas. The lattice contribution is dominant for intermediate wavelenths.
机译:计算了二维和三维超晶格排列的碳纳米管束的集体电子激发(等离激元)模式。可以将获得的一系列模式视为三个贡献的组合:(i)单管贡献,(ii)统一的2D或3D buk贡献和(iii)与晶格结构有关的贡献。与小管间距离a(即aq >> 1)相比,小等离激元波长的单管贡献占主导地位。但是,对于大波长aq << 1,则其等于2D或3D均匀电子气的波长。对于中间波长,晶格的贡献是主要的。

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