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Semiconducting Graphene on Silicon from First-Principles Calculations

机译:从第一性原理计算硅上的半导体石墨烯

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Graphene is a semimetal with zero band gap, which makes it impossible to turn electric conduction off below a certain limit. Transformation of graphene into a semiconductor has attracted wide attention. Owing to compatibility with Si technology, graphene adsorbed on a Si substrate is particularly attractive for future applications. However, to date there is little theoretical work on band gap engineering in graphene and its integration with Si technology. Employing first-principles calculations, we study the electronic properties of monolayer and bilayer graphene adsorbed on clean and hydrogen (H)-passivated Si (111)/Si (100) surfaces. Our calculation shows that the interaction between monolayer graphene and a H-passivated Si surface is weak, with the band gap remaining negligible. For bilayer graphene adsorbed onto a H-passivated Si surface, the band gap opens up to 108 meV owing to asymmetry introduction. In contrast, the interaction between graphene and a clean Si surface is strong, leading to formation of chemical bonds and a large band gap of 272 meV. Our results provide guidance for device designs based on integrating graphene with Si technology.
机译:石墨烯是具有零带隙的半金属,这使得不可能在特定极限以下关闭导电。石墨烯向半导体的转变已引起广泛关注。由于与硅技术的兼容性,吸附在硅基板上的石墨烯对于未来的应用特别有吸引力。但是,迄今为止,关于石墨烯中的带隙工程及其与Si技术的集成的理论研究还很少。使用第一性原理计算,我们研究了吸附在干净的氢(H)钝化的Si(111)/ Si(100)表面上的单层和双层石墨烯的电子性能。我们的计算表明,单层石墨烯和H钝化的Si表面之间的相互作用较弱,带隙仍然可以忽略不计。对于吸附在H钝化的Si表面上的双层石墨烯,由于引入了不对称性,带隙打开至108 meV。相反,石墨烯和干净的Si表面之间的相互作用很强,导致形成化学键和272 meV的大带隙。我们的结果为基于石墨烯与Si技术集成的器件设计提供了指导。

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