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Volumn 9, Issue 7, 2009, Pages 2654-2660

Electronic structure of few-layer epitaxial graphene on Ru(0001)

Author keywords

[No Author keywords available]

Indexed keywords

ANGLE RESOLVED PHOTOELECTRON SPECTROSCOPY; BI-LAYER; ELECTRONIC COUPLING; EPITAXIAL GRAPHENE; FERMI ENERGY; GRAPHENE; GRAPHENE LAYERS; GRAPHENE SHEETS; RU(0001); TRILAYER;

EID: 67650361320     PISSN: 15306984     EISSN: None     Source Type: Journal    
DOI: 10.1021/nl901040v     Document Type: Article
Times cited : (246)

References (46)
  • 16
    • 12844286241 scopus 로고    scopus 로고
    • Kresse, G.; J, H. Phys. Rev. B 1993, 47, 558.
    • Kresse, G.; J, H. Phys. Rev. B 1993, 47, 558.
  • 29
    • 84869362375 scopus 로고    scopus 로고
    • We used the nearest-neighbor Hamiltonian by Reich et al.30 with parameters ε2p, ED as noted in the text, γ0, 3.28 eV, and overlap s0, 0.03
    • We used the nearest-neighbor Hamiltonian by Reich et al.30 with parameters ε2p ) ED as noted in the text, γ0 )-3.28 eV, and overlap s0 ) 0.03.
  • 42
    • 84869364476 scopus 로고    scopus 로고
    • We have probed the impact of choosing the LDA by performing generalized gradient approximation calculations with the PBE functional43 for selected cases. For the split registry, the local bond lengths are essentially the same, but the binding energy is reduced to 0.6 eV, still indicative of significant bond formation. For the BC case, the interaction becomes slightly repulsive and the total energy as a function of Ru-graphene spacing no longer shows a well-defined minimum. This agrees with recent calculations performed with the PBE functional examining a 12 × 12 graphene layer on an 11 × 11 Ru(0001) slab supercell.44 While LDA-based calculations overestimate binding for weakly interacting layered systems (graphite c-axis lattice parameter too small, PBE-based calculations generally give no binding for such systems (graphitic layers are not bound, Thus, interface interaction suggests that the graphene regions near BC registry in the moire' may be somewhat further s
    • We have probed the impact of choosing the LDA by performing generalized gradient approximation calculations with the PBE functional43 for selected cases. For the split registry, the local bond lengths are essentially the same, but the binding energy is reduced to 0.6 eV, still indicative of significant bond formation. For the BC case, the interaction becomes slightly repulsive and the total energy as a function of Ru-graphene spacing no longer shows a well-defined minimum. This agrees with recent calculations performed with the PBE functional examining a 12 × 12 graphene layer on an 11 × 11 Ru(0001) slab supercell.44 While LDA-based calculations overestimate binding for weakly interacting layered systems (graphite c-axis lattice parameter too small), PBE-based calculations generally give no binding for such systems (graphitic layers are not bound). Thus, interface interaction suggests that the graphene regions near BC registry in the moire' may be somewhat further (say 0.1 Å) from the Ru surface than our LDA calculations indicate (2.20 Å), although lateral strain interactions may enhance the buckling.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.