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Multiple Dirac fermions from a topological insulator and graphene superlattice

机译:来自拓扑绝缘体和石墨烯超晶格的多个Dirac费米子

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摘要

Graphene and three-dimensional topological insulators are well-known Dirac materials whose bulk and surface states are governed by Dirac equations. They not only show good transport properties but also carry various quanta related to the geometrical phase such as charge, spin, and valley Hall conductances. Therefore, it is a great challenge to combine the two Dirac materials together, realizing multiple Dirac fermions. By using first-principles density-functional-theory calculations, we demonstrate such a system built from topological insulator-band insulator-graphene superlattice structures. Hexagonal boron nitride is proposed as an ideal band-insulating material in gluing graphene and topological insulators, providing a good substrate for graphene and a sharp interface with a topological insulator. The power factors for p-type doping are largely enhanced due to the charge-conducting channels through multiple Dirac cones. The systems characterized by the coexistence of the topologically protected interfacial and graphene Dirac cones can pave the way for developing integrated devices for electronics, spintronics and valleytronics applications.
机译:石墨烯和三维拓扑绝缘体是众所周知的Dirac材料,其体态和表面态由Dirac方程控制。它们不仅显示出良好的传输性能,而且还携带与几何相位有关的各种量子,例如电荷,自旋和谷底霍尔电导。因此,将两种狄拉克材料结合在一起,实现多种狄拉克费米子是一个巨大的挑战。通过使用第一性原理密度泛函理论计算,我们证明了这种由拓扑绝缘体-带状绝缘体-石墨烯超晶格结构构建的系统。六方氮化硼被认为是粘合石墨烯和拓扑绝缘体的理想带绝缘材料,可为石墨烯提供良好的基材,并提供与拓扑绝缘体的清晰界面。由于通过多个Dirac锥体的电荷传导通道,p型掺杂的功率因数大大提高。以拓扑受保护的界面和石墨烯Dirac锥锥共存为特征的系统可以为开发用于电子,自旋电子学和Valleytronics应用的集成设备铺平道路。

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