Nat Mater. 2010 Apr;9(4):315-9. doi: 10.1038/nmat2710. Epub 2010 Mar 14.
Graphene, a single layer of graphite, has recently attracted considerable attention owing to its remarkable electronic and structural properties and its possible applications in many emerging areas such as graphene-based electronic devices. The charge carriers in graphene behave like massless Dirac fermions, and graphene shows ballistic charge transport, turning it into an ideal material for circuit fabrication. However, graphene lacks a bandgap around the Fermi level, which is the defining concept for semiconductor materials and essential for controlling the conductivity by electronic means. Theory predicts that a tunable bandgap may be engineered by periodic modulations of the graphene lattice, but experimental evidence for this is so far lacking. Here, we demonstrate the existence of a bandgap opening in graphene, induced by the patterned adsorption of atomic hydrogen onto the Moiré superlattice positions of graphene grown on an Ir(111) substrate.
石墨烯是单层石墨,由于其显著的电子和结构特性以及在许多新兴领域(如基于石墨烯的电子器件)的潜在应用,最近引起了相当大的关注。石墨烯中的电荷载流子表现得像无质量的狄拉克费米子,并且石墨烯表现出弹道电荷输运,使其成为制造电路的理想材料。然而,石墨烯在费米能级周围缺乏带隙,这是半导体材料的定义概念,对于通过电子手段控制电导率至关重要。理论预测,通过周期性调制石墨烯晶格,可以设计出可调谐的带隙,但到目前为止,这方面的实验证据还很缺乏。在这里,我们通过原子氢在生长在 Ir(111)衬底上的石墨烯的莫尔超晶格位置上的图案化吸附,证明了石墨烯中带隙的开启。