Oostinga Jeroen B, Heersche Hubert B, Liu Xinglan, Morpurgo Alberto F, Vandersypen Lieven M K
Kavli Institute of Nanoscience, Delft University of Technology, PO Box 5046, 2600 GA, Delft, The Netherlands.
Nat Mater. 2008 Feb;7(2):151-7. doi: 10.1038/nmat2082. Epub 2007 Dec 2.
The potential of graphene-based materials consisting of one or a few layers of graphite for integrated electronics originates from the large room-temperature carrier mobility in these systems (approximately 10,000 cm2 V(-1) s(-1)). However, the realization of electronic devices such as field-effect transistors will require controlling and even switching off the electrical conductivity by means of gate electrodes, which is made difficult by the absence of a bandgap in the intrinsic material. Here, we demonstrate the controlled induction of an insulating state--with large suppression of the conductivity--in bilayer graphene, by using a double-gate device configuration that enables an electric field to be applied perpendicular to the plane. The dependence of the resistance on temperature and electric field, and the absence of any effect in a single-layer device, strongly suggest that the gate-induced insulating state originates from the recently predicted opening of a bandgap between valence and conduction bands.
由一层或几层石墨构成的石墨烯基材料在集成电子学方面的潜力源于这些系统中较大的室温载流子迁移率(约10,000 cm2 V(-1) s(-1))。然而,诸如场效应晶体管等电子器件的实现将需要通过栅电极来控制甚至关闭电导率,而本征材料中不存在带隙使得这变得困难。在此,我们通过使用一种双栅器件结构证明了在双层石墨烯中可控地诱导出绝缘态——电导率大幅抑制,该结构能够垂直于平面施加电场。电阻对温度和电场的依赖性以及单层器件中不存在任何效应,强烈表明栅极诱导的绝缘态源于最近预测的价带和导带之间带隙的打开。