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在 Cu(111)上通过化学气相沉积法制备和表征了取向和非共形的石墨烯/六方氮化硼杂化堆叠。

Chemical vapor deposition and characterization of aligned and incommensurate graphene/hexagonal boron nitride heterostack on Cu(111).

机构信息

Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland.

出版信息

Nano Lett. 2013 Jun 12;13(6):2668-75. doi: 10.1021/nl400815w. Epub 2013 May 14.

Abstract

Two limiting factors for a new technology of graphene-based electronic devices are the difficulty of growing large areas of defect-free material and the integration of graphene with an atomically flat and insulating substrate material. Chemical vapor deposition (CVD) on metal surfaces, in particular on copper, may offer a solution to the first problem, while hexagonal boron nitride (h-BN) has been identified as an ideal insulating substrate material. The bottom-up growth of graphene/h-BN stacks on copper surfaces appears therefore as a promising route for future device fabrication. As an important step, we demonstrate the consecutive growth of well-aligned graphene on h-BN, both as single layers, by low-pressure CVD on Cu(111) in an ultrahigh vacuum environment. The resulting films show a largely predominant orientation, defined by the substrate, where the graphene lattice aligns parallel to the h-BN lattice, while each layer maintains its own lattice constant. The lattice mismatch of 1.6% between h-BN and graphene leads to a moiré pattern with a periodicity of about 9 nm, as observed with scanning tunneling microscopy. Accordingly, angle-resolved photoemission data reveal two slightly different Brillouin zones for electronic states localized in graphene and in h-BN, reflecting the vertical decoupling of the two layers. The graphene appears n-doped and shows no gap opening at the K[overline] point of the two-dimensional Brillouin zone.

摘要

对于基于石墨烯的电子器件的新技术,有两个限制因素:难以生长大面积无缺陷的材料,以及将石墨烯与原子级平整和绝缘衬底材料集成。化学气相沉积(CVD)在金属表面上,特别是在铜上,可能为第一个问题提供解决方案,而六方氮化硼(h-BN)已被确定为理想的绝缘衬底材料。因此,在铜表面上自下而上生长石墨烯/h-BN 堆叠似乎是未来器件制造的有前途的途径。作为一个重要步骤,我们在超高真空环境中通过低压 CVD 在 Cu(111)上展示了在 h-BN 上连续生长的良好排列的石墨烯,包括单层。所得薄膜显示出主要取向,由衬底定义,其中石墨烯晶格平行于 h-BN 晶格排列,而每个层保持其自己的晶格常数。h-BN 和石墨烯之间 1.6%的晶格失配导致莫尔图案,其周期约为 9nm,如扫描隧道显微镜观察到的。相应地,角分辨光发射数据显示出电子态在石墨烯中和 h-BN 中局部化的两个略有不同的布里渊区,反映了两层的垂直解耦。石墨烯呈现 n 掺杂,并且在二维布里渊区的 K[overline]点处没有打开间隙。

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