Zhou S Y, Gweon G-H, Fedorov A V, First P N, de Heer W A, Lee D-H, Guinea F, Castro Neto A H, Lanzara A
Department of Physics, University of California, Berkeley, California 94720, USA.
Nat Mater. 2007 Oct;6(10):770-5. doi: 10.1038/nmat2003. Epub 2007 Sep 9.
Graphene has shown great application potential as the host material for next-generation electronic devices. However, despite its intriguing properties, one of the biggest hurdles for graphene to be useful as an electronic material is the lack of an energy gap in its electronic spectra. This, for example, prevents the use of graphene in making transistors. Although several proposals have been made to open a gap in graphene's electronic spectra, they all require complex engineering of the graphene layer. Here, we show that when graphene is epitaxially grown on SiC substrate, a gap of approximately 0.26 eV is produced. This gap decreases as the sample thickness increases and eventually approaches zero when the number of layers exceeds four. We propose that the origin of this gap is the breaking of sublattice symmetry owing to the graphene-substrate interaction. We believe that our results highlight a promising direction for bandgap engineering of graphene.
石墨烯作为下一代电子器件的主体材料已展现出巨大的应用潜力。然而,尽管它具有引人入胜的特性,但石墨烯作为电子材料使用的最大障碍之一是其电子光谱中缺乏能隙。例如,这使得石墨烯无法用于制造晶体管。虽然已经提出了几种在石墨烯电子光谱中打开能隙的方案,但它们都需要对石墨烯层进行复杂的工程处理。在此,我们表明,当石墨烯在碳化硅衬底上外延生长时,会产生约0.26电子伏特的能隙。这个能隙会随着样品厚度的增加而减小,当层数超过四层时最终趋近于零。我们认为这个能隙的起源是由于石墨烯与衬底的相互作用导致亚晶格对称性的破坏。我们相信我们的结果为石墨烯的带隙工程突出了一个有前景的方向。