2014
DOI: 10.1016/j.progsurf.2014.08.001
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Transition metals on the (0 0 0 1) surface of graphite: Fundamental aspects of adsorption, diffusion, and morphology

Abstract: In this article, we review basic information about the interaction of transition metal atoms with the (0001) surface of graphite, especially fundamental phenomena related to growth. Those phenomena involve adatomsurface bonding, diffusion, morphology of metal clusters, interactions with steps and sputter-induced defects, condensation, and desorption. General traits emerge which have not been summarized previously. Some of these features are rather surprising when compared with metal-on-metal adsorption and gro… Show more

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Cited by 64 publications
(70 citation statements)
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References 115 publications
(215 reference statements)
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“…As in our study of Cu/HOPG, analyses of N(θ) and the ISD can be powerful tools for identifying the correct model. We conclude that metal cluster growth on smooth graphite terraces-a simple and common observation in the literature [6] -must be interpreted with care, certainly for graphite and possibly for other carbon-rich surfaces as well.…”
Section: Discussionmentioning
confidence: 72%
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“…As in our study of Cu/HOPG, analyses of N(θ) and the ISD can be powerful tools for identifying the correct model. We conclude that metal cluster growth on smooth graphite terraces-a simple and common observation in the literature [6] -must be interpreted with care, certainly for graphite and possibly for other carbon-rich surfaces as well.…”
Section: Discussionmentioning
confidence: 72%
“…It is noteworthy that our calculations incorporate the dispersion forces that bind the carbon sheets in graphite. DFT shows that a Cu atom adsorbs atop a C atom with no C atom in the layer beneath (the graphite β site [6]), and the adsorption energy (E ads ) is 0.589 eV. A Cu atom diffuses between β sites along C-C bonds, with an associated energy barrier (E diff ) of 0.020 eV.…”
Section: Experimental and Computational Resultsmentioning
confidence: 99%
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“…Following the early categorization and description of 3D (Volmer-Weber) film growth by Bauer [31], recent studies of metal-film and nanostructure growth on graphite [32], graphene [4], and other 2D materials [5,6] have explained experimentally observed growth morphologies as a function of the ratio between the adsorption energy (E ads ) of metal atoms on the substrate and the bulk-metal cohesive energy (E coh ); the lower the E ads /E coh ratio, the stronger the tendency toward 3D growth. Intuitively, this can be understood as the metal atoms being more weakly bound to the substrate, which facilitates their ascent onto the first layer of an island by either direct hopping or an exchange mechanism [33].…”
Section: Introductionmentioning
confidence: 99%
“…These facets have been suggested to facilitate growth of AlSn alloy films on weakly interacting substratesincluding amorphous-C, SiO 2 , NaCl, and mica [3,[45][46][47]-by providing pathways for accelerated mass transport between the base and the upper layer of 3D atomic islands. Moreover, facet formation has been experimentally observed during the deposition of metal films on graphene and graphite surfaces [4,32]. Hence, in the context of 3D growth beyond the second layer, the absence of steps may allow adatoms to ascend multiple layers by encountering a terrace diffusion barrier [E s in Fig.…”
Section: Introductionmentioning
confidence: 99%