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

被引:71
作者
Kinyanjui, M. K. [1 ]
Kramberger, C. [2 ]
Pichler, T. [2 ]
Meyer, J. C. [1 ]
Wachsmuth, P. [1 ]
Benner, G. [3 ]
Kaiser, U. [1 ]
机构
[1] Univ Ulm, Cent Facil Electron Microscopy, D-89081 Ulm, Germany
[2] Univ Vienna, Fac Phys, A-1090 Vienna, Austria
[3] Carl Zeiss NTS GmbH, D-73447 Oberkochen, Germany
基金
奥地利科学基金会;
关键词
ELECTRON-ENERGY-LOSS; DEPENDENCE; GRAPHITE;
D O I
10.1209/0295-5075/97/57005
中图分类号
O4 [物理学];
学科分类号
0702 ;
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 pi plasmons in free-standing graphene monolayers at the momentum range of 0 <= vertical bar q vertical bar <= 0.5 angstrom(-1) and parallel to the Gamma-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 pi 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 pi plasmon response. Copyright (C) EPLA, 2012
引用
收藏
页数:6
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