Denis Pablo A
Computational Nanotechnology, DETEMA, Facultad de Química, UDELAR, CC 1157, 11800 Montevideo (Uruguay).
Chemphyschem. 2014 Dec 15;15(18):3994-4000. doi: 10.1002/cphc.201402608. Epub 2014 Oct 27.
Herein, the effects of substitutional doping of graphene with Ga, Ge, As, and Se are shown. Ge exhibits the lowest formation energy, whereas Ga has the largest one. Ga- and As-doped graphene display a reactivity that is larger than that corresponding to a double vacancy. They can decompose H2 and O2 easily. Variation of the type and concentration of dopant makes the adjustment of the interlayer interaction possible. In general, doping of monolayer graphene opens a band gap. At some concentrations, Ga doping induces a half metallic behavior. As is the element that offers the widest range of gap tuning. Heyd-Scuseria-Ernzerhof calculations indicate that it can be varied from 1.3 to 0.3 eV. For bilayer graphene, the doped sheet induces charge redistribution in the perfect underneath sheet, which opens a gap in the range of 0.05-0.4 eV. This value is useful for developing graphene-based electronics, as the carrier mobility of the undoped sheet is not expected to alter.
在此展示了用Ga、Ge、As和Se对石墨烯进行替代掺杂的效果。Ge表现出最低的形成能,而Ga的形成能最大。Ga和As掺杂的石墨烯表现出比对应双空位更大的反应活性。它们能轻易分解H₂和O₂。掺杂剂类型和浓度的变化使得层间相互作用的调节成为可能。一般来说,单层石墨烯的掺杂会打开一个带隙。在某些浓度下,Ga掺杂会诱导半金属行为。As是提供最宽带隙调谐范围的元素。Heyd-Scuseria-Ernzerhof计算表明其带隙可在1.3至0.3 eV之间变化。对于双层石墨烯,掺杂的那一层会在理想的下层中诱导电荷重新分布,从而打开一个0.05 - 0.4 eV范围内的带隙。该值对于开发基于石墨烯的电子产品很有用,因为预计未掺杂层的载流子迁移率不会改变。