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首页> 外文期刊>Carbon: An International Journal Sponsored by the American Carbon Society >Rotation misorientated graphene moire superlattices on Cu (111): Classical molecular dynamics simulations and scanning tunneling microscopy studies
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Rotation misorientated graphene moire superlattices on Cu (111): Classical molecular dynamics simulations and scanning tunneling microscopy studies

机译:Cu(111)上旋转取向错误的石墨烯莫尔条纹超晶格:经典分子动力学模拟和扫描隧道显微镜研究

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Graphene on copper is a system of high technological relevance, as Cu is one of the most widely used substrates for the CVD growth of graphene. However, very little is known about the details of their interaction. One approach to gain such information is studying the superlattices emerging due to the mismatch of the two crystal lattices. However, graphene on copper is a low-corrugated system making both their experimental and theoretical study highly challenging. Here, we report the observation of a new rotational moire super-lattice of CVD graphene on Cu (111), characterized by a periodicity of (1.5 ± 0.05) nm and corrugation of (0.15 ±0.05) A, as measured by scanning tunneling microscopy (STM). To understand the observed superlattice we have developed a newly parameterized Abell-Tersoff potential for the graphene/Cu (111) interface fitted to nonlocal van der Waals density functional theory (DFT) calculations. The interfacial force field with time-lapsed classical molecular dynamics (CMD) provides superlattices in good quantitative agreement with the experimental results, for a misorientation angle of (10.4 ±0.5°), without any further parameter adjustment. Furthermore, the CMD simulations predict the existence of two non-equivalent high-symmetry directions of the moire pattern that could also be identified in the experimental STM images.
机译:铜上的石墨烯是具有高度技术相关性的系统,因为Cu是用于CVD生长石墨烯的最广泛使用的衬底之一。但是,关于它们的交互细节知之甚少。获取此类信息的一种方法是研究由于两个晶格不匹配而出现的超晶格。但是,铜上的石墨烯是一种低波纹系统,因此其实验和理论研究都极具挑战性。在这里,我们报告观察到的一种新的CVD石墨烯在Cu(111)上的旋转莫尔超晶格的观察,其特征是周期(1.5±0.05)nm和波纹(0.15±0.05)A,这是通过扫描隧道显微镜测量的(STM)。为了了解观察到的超晶格,我们为石墨烯/ Cu(111)界面开发了新参数化的Abell-Tersoff势,该势能适用于非局部范德华密度泛函理论(DFT)计算。界面力场具有时滞经典分子动力学(CMD),提供了与实验结果良好的定量一致性的超晶格,取向角为(10.4±0.5°),而无需任何进一步的参数调整。此外,CMD模拟可预测存在两个不相等的摩尔纹高对称方向,这也可以在实验STM图像中找到。

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