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首页> 外文期刊>Physical review >Electronic structure and scanning tunneling microscopy images of heterostructures consisting of graphene and carbon-doped hexagonal boron nitride layers
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Electronic structure and scanning tunneling microscopy images of heterostructures consisting of graphene and carbon-doped hexagonal boron nitride layers

机译:由石墨烯和碳掺杂六边形硼层组成的异质结构的电子结构和扫描隧道显微镜图像

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摘要

We perform first-principles total-energy calculations within the framework of the density-functional theory to investigate electronic properties of graphene/C-doped hexagonal boron nitride (h-BN) heterostructures. We consider both the monolayer h-BN case and the trilayer h-BN case. From the electronic-structure analysis, it is found that substitutional doping of the C atom at the B site and that at the N site in underlying h-BN lead to asymmetric charge carrier concentrations in the graphene layer, indicating the importance of the impurity atom in the h-BN substrate and its polarity in the electronic transport properties of graphene/h-BN heterostructures. We also find that simulated scanning tunneling microscopy (STM) images of the graphene surface on the C-doped h-BN layer at the B site and that at the N site are considerably different from each other in both monolayer and trilayer h-BN cases. While the B site doping of the C atom in h-BN substrate layers essentially does not change the STM image of the graphene surface on the pristine h-BN, the C atom doped at the N site considerably modifies the STM image of graphene even in the case of the doping in the third layer of the trilayer h-BN. Therefore, when the graphene in used as a cover layer to the h-BN layered materials and thin films, the STM should be a useful tool to detect the acceptor C atoms in the h-BN not only at the topmost surface layer but also at second and third layers. We clarify the origin of these characteristic features of the STM images in terms of spatial distributions of the local density of states induced by the dopant C atom.
机译:我们在密度函数理论的框架内执行总能量计算,以研究石墨烯/ C掺杂六方氮化物(H-BN)异质结构的电子性质。我们考虑单层H-BN案例和三层H-BN案例。从电子结构分析中,发现B位点上的C原子的替代掺杂,并且在下面的H-BN中的N位点导致石墨烯层中的不对称电荷载体浓度,表明杂质原子的重要性在石墨烯/ H-BN异质结构的电子传输性质中的H-BN基材及其极性。我们还发现,在B位点的C掺杂的H-BN层上的石墨烯表面的模拟扫描隧道显微镜(STM)图像在单层和三层H-BN壳体中彼此相比彼此不同。虽然在H-BN衬底层中的C原子的B网站掺杂基本上不会在原始H-BN上改变石墨烯表面的STM图像,但在N个网站上掺杂的C原子显着地改变了石墨烯的STM图像三层H-Bn的第三层中掺杂的情况。因此,当石墨烯用作H-BN分层材料和薄膜的覆盖层时,STM应该是检测H-BN中的受体C原子的有用工具,而不仅在最顶部的表面层也是如此第二层和第三层。我们在掺杂剂C原子诱导的局部密度的空间分布方面阐明了STM图像的这些特征的起源。

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  • 来源
    《Physical review》 |2019年第12期|125403.1-125403.10|共10页
  • 作者单位

    Tokyo Inst Technol Dept Phys Meguro Ku 2-12-1 Oh Okayama Tokyo 1528551 Japan;

    Tokyo Inst Technol Dept Phys Meguro Ku 2-12-1 Oh Okayama Tokyo 1528551 Japan;

    Tokyo Inst Technol Dept Phys Meguro Ku 2-12-1 Oh Okayama Tokyo 1528551 Japan|Tokyo Inst Technol Adv Res Ctr Quantum Phys & Nanosci Meguro Ku 2-12-1 Oh Okayama Tokyo 1528551 Japan|Tokyo Inst Technol Mat Res Ctr Element Strategy Midori Ku 4259 Nagatsuta Cho Yokohama Kanagawa 2268503 Japan;

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