Electronic properties of graphene

被引：287
|
作者：
Novoselov, K. S.
Morozov, S. V.
Mohinddin, T. M. G.
Ponomarenko, L. A.
Elias, D. C.
Yang, R.
Barbolina, I. I.
Blake, P.
Booth, T. J.
Jiang, D.
Giesbers, J.
Hill, E. W.
Geim, A. K.
机构：
[1] Univ Manchester, Sch Phys & Astron, Manchester M13 9PL, Lancs, England
[2] Inst Microelect Technol, Chernogolovka 142432, Russia
[3] Univ Manchester, Manchester Ctr Mesosci & Nanotechnol, Manchester M13 9PL, Lancs, England
[4] TSC, Lancaster OL10 1DS, England
[5] Graphene Ind Ltd, Manchester M60 1QD, Lancs, England
[6] Radboud Univ Nijmegen, High Feild Magnet Lab, NL-6525 ED Nijmegen, Netherlands
[7] Univ Manchester, Sch Comp Sci, Manchester M13 9PL, Lancs, England
来源：
PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS | 2007年 / 244卷 / 11期
关键词：
D O I：
10.1002/pssb.200776208
中图分类号：
O469 [凝聚态物理学];
学科分类号：
070205 ;
摘要：
Graphene is the first example of truly two-dimensional crystals - it's just one layer of carbon atoms. It turns out that graphene is a gapless semiconductor with unique electronic properties resulting from the fact that charge carriers in graphene obey linear dispersion relation, thus mimicking massless relativistic particles. This results in the observation of a number of very peculiar electronic properties - from an anomalous quantum Hall effect to the absence of localization. It also provides a bridge between condensed matter physics and quantum electrodynamics and opens new perspectives for carbon-based electronics. (c) 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.
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收藏
页码：4106 / 4111
页数：6
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