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arXiv 1012.2826cond-mat.mtrl-sci
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面内取向对Ir(111)表面单层石墨烯的电子结构、稳定性和拉曼散射的影响

In-plane orientation effects on the electronic structure, stability and Raman scattering of monolayer graphene on Ir(111)

Elena Starodub, Aaron Bostwick, Luca Moreschini, Shu Nie, Farid El Gabaly, Kevin F. McCarty, Eli Rotenberg

摘要:

我们采用角分辨光电子能谱(ARPES)研究了Ir(111)上外延单层石墨烯的两种旋转变体的电子结构。随着生长,更丰富的R 0变体几乎是电荷中性的,在费米能级附近的石墨烯和Ir带之间具有强杂交。石墨烯费米面及其复制品与Ir费米面中的Van Hove奇点完全重合。亚晶格对称性破缺在狄拉克交叉处引入了一个小的能隙诱导势,这是通过使用K原子对石墨烯进行n掺杂来揭示的。主带和复制带之间的能隙(源自石墨烯和Ir晶格之间的莫尔干涉图案)被示出为由于与Ir带的杂化而沿着微区边界是不均匀的。提出了一种电子介导的相互作用来解释R 0变体的稳定性。在平面内旋转30°的变体R30在生长时是p掺杂的,并且K掺杂显示在狄拉克交叉处没有带隙。在ARPES测量中没有发现复制带。R30变体的拉曼光谱表现出石墨烯的特征声子模式,而R 0光谱没有特征。这些结果表明,薄膜/基底的相互作用从化学吸附(R 0)转变为物理吸附(R30)与面内取向。最后,石墨烯覆盖的Ir的功函数低于清洁衬底,但高于石墨。

英文摘要:

We employ angle-resolved photoemission spectroscopy (ARPES) to investigate the electronic structures of two rotational variants of epitaxial, single-layer graphene on Ir(111). As grown, the more-abundant R0 variant is nearly charge-neutral, with strong hybridization between graphene and Ir bands near the Fermi level. The graphene Fermi surface and its replicas exactly coincide with Van Hove singularities in the Ir Fermi surface. Sublattice symmetry breaking introduces a small gap-inducing potential at the Dirac crossing, which is revealed by n-doping the graphene using K atoms. The energy gaps between main and replica bands (originating from the moiré interference pattern between graphene and Ir lattices) is shown to be non-uniform along the mini- zone boundary due to hybridization with Ir bands. An electronically mediated interaction is proposed to account for the stability of the R0 variant. The variant rotated 30° in-plane, R30, is p-doped as grown and K doping reveals no band gap at the Dirac crossing. No replica bands are found in ARPES measurements. Raman spectra from the R30 variant exhibit the characteristic phonon modes of graphene, while R0 spectra are featureless. These results show that the film/substrate interaction changes from chemisorption (R0) to physisorption (R30) with in-plane orientation. Finally, graphene-covered Ir has a work function lower than the clean substrate but higher than graphite.

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