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Direct probe of linearly dispersing 2D interband plasmons in a free-standing graphene monolayer

机译:在独立的石墨烯单层中线性分散二维带间等离子体激元的直接探针

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摘要

In low-dimensional systems, a detailed understanding of plasmons and their dispersion relation is crucial for applying their optical response in the field of plasmonics. Electron energy-loss spectroscopy is a direct probe of these excitations. Here we report on electron energy-loss spectroscopy results on the dispersion of the π plasmons in free-standing graphene monolayers at the momentum range of 0≤|q|≤0.5 ? ~(-1) and parallel to the Γ-M direction of the graphene Brillouin zone. In contrast to the parabolic dispersion in graphite and in good agreement with theoretical predictions of a 2D electron gas of Dirac electrons, linear π plasmon dispersion is observed. As with previous EELS results obtained from single-wall carbon nanotubes, this can be explained by local-field effects in the anisotropic 2D system yielding a significant contribution of the low-energy band structure on the high-energy π plasmon response.
机译:在低维系统中,对等离激元及其色散关系的详细了解对于将其光学响应应用于等离激元领域至关重要。电子能量损失谱是这些激发的直接探究。在这里,我们报告了在动能范围为0≤| q |≤0.5?时,π等离子体激元在自支撑石墨烯单层中的分散情况的电子能量损失谱结果。 〜(-1),且平行于石墨烯布里渊区的Γ-M方向。与石墨中的抛物线色散相反,并且与狄拉克电子的二维电子气的理论预测非常吻合,观察到了线性π等离子体激元色散。与以前从单壁碳纳米管获得的EELS结果一样,这可以通过各向异性2D系统中的局部场效应来解释,该效应会导致低能带结构对高能π等离子体激元响应产生重大影响。

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