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Loss spectra of graphite-related systems: A multiwall carbon nanotube, a single-wall carbon nanotube bundle, and graphite layers

机译:石墨相关系统的损耗光谱:多壁碳纳米管,单壁碳纳米管束和石墨层

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The pi-electron excitations are studied for a multiwall carbon nanotube, a single-wall carbon nanotube bundle with finite nanotubes, and graphite layers. The loss spectra of the nanotube systems exhibit several plasmon peaks. The most prominent one is the pi plasmon, and the others are the interband plasmons. The latter are absent in graphite layers. The pi plasmon depends on the number of carbon nanotubes or graphite layers (N), the transferred momentum (q), and the transferred angular momentum (L). The intertube or interlayer Coulomb interactions clearly enhance pi-plasmon frequency and oscillator strength as N increases. A multiwall carbon nanotube can exhibit L-decoupled pi plasmons. For the L = 0 pi plasmon, the multiwall nanotube behaves like graphite layers, but not like a single-wall carbon nanotube bundle. The radius dependence is negligible for a multiwall nanotube, while it is strong for a single-wall nanotube bundle. Furthermore, the former exhibits stronger collective excitations, higher pi-plasmon frequency, and relatively rapid increase of plasmon frequency with q. The calculated results are compared with experimental measurements. [References: 56]
机译:研究了多壁碳纳米管,具有有限纳米管的单壁碳纳米管束和石墨层的π电子激发。纳米管系统的损耗光谱表现出几个等离激元峰。最突出的一个是pi等离子体激元,其他的是带间等离子体激元。后者在石墨层中不存在。 π等离子体激元取决于碳纳米管或石墨层的数量(N),传递的动量(q)和传递的角动量(L)。随着N的增加,管间或层间库仑相互作用明显增强了π等离子体频率和振荡器强度。多层碳纳米管可以表现出L解耦的π型等离激元。对于L = 0 pi等离子体激元,多壁纳米管的行为类似于石墨层,但不像单壁碳纳米管束。半径依赖性对于多壁纳米管可以忽略不计,而对于单壁纳米管束则很强。此外,前者表现出更强的集体激发,更高的π-等离激元频率以及随着q相对较快地增加了等离激元频率。将计算结果与实验测量值进行比较。 [参考:56]

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