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石墨烯-镍界面:综述

Graphene-nickel interfaces: a review.

作者信息

Dahal Arjun, Batzill Matthias

机构信息

Department of Physics, University of South Florida, Tampa, FL 33620, USA.

出版信息

Nanoscale. 2014 Mar 7;6(5):2548-62. doi: 10.1039/c3nr05279f. Epub 2014 Jan 30.

DOI:10.1039/c3nr05279f
PMID:24477601
Abstract

Graphene on nickel is a prototypical example of an interface between graphene and a strongly interacting metal, as well as a special case of a lattice matched system. The chemical interaction between graphene and nickel is due to hybridization of the metal d-electrons with the π-orbitals of graphene. This interaction causes a smaller separation between the nickel surface and graphene (0.21 nm) than the typical van der Waals gap-distance between graphitic layers (0.33 nm). Furthermore, the physical properties of graphene are significantly altered. Main differences are the opening of a band gap in the electronic structure and a shifting of the π-band by ∼2 eV below the Fermi-level. Experimental evidence suggests that the ferromagnetic nickel induces a magnetic moment in the carbon. Substrate induced geometric and electronic changes alter the phonon dispersion. As a consequence, monolayer graphene on nickel does not exhibit a Raman spectrum. In addition to reviewing these fundamental physical properties of graphene on Ni(111), we also discuss the formation and thermal stability of graphene and a surface-confined nickel-carbide. The fundamental growth mechanisms of graphene by chemical vapor deposition are also described. Different growth modes depending on the sample temperature have been identified in ultra high vacuum surface science studies. Finally, we give a brief summary for the synthesis of more complex graphene and graphitic structures using nickel as catalyst and point out some potential applications for graphene-nickel interfaces.

摘要

镍上的石墨烯是石墨烯与强相互作用金属之间界面的典型例子,也是晶格匹配系统的一个特殊情况。石墨烯与镍之间的化学相互作用是由于金属d电子与石墨烯的π轨道杂化。这种相互作用导致镍表面与石墨烯之间的间距(0.21纳米)小于石墨层之间典型的范德华间隙距离(0.33纳米)。此外,石墨烯的物理性质也发生了显著变化。主要差异在于电子结构中出现了带隙,且π带在费米能级以下移动了约2电子伏特。实验证据表明,铁磁性镍会在碳中诱导出磁矩。衬底诱导的几何和电子变化改变了声子色散。因此,镍上的单层石墨烯不表现出拉曼光谱。除了回顾镍(111)上石墨烯的这些基本物理性质外,我们还讨论了石墨烯和表面受限碳化镍的形成及热稳定性。还描述了通过化学气相沉积法生长石墨烯的基本机制。在超高真空表面科学研究中已确定了取决于样品温度的不同生长模式。最后,我们简要总结了以镍为催化剂合成更复杂的石墨烯和石墨结构的情况,并指出了石墨烯 - 镍界面的一些潜在应用。

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