Electronic states of coupled graphene nanoribbons

Electronic states of laterally coupled graphene nanoribbons (GNRs) have been calculated within a nearest-neighbor tight-binding approximation with varying inter-GNR coupling strength γ from γ = 0 to t (intra-GNR transfer integral). For a coupled zigzag-edge GNR array, both almost flat bands and anis...

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Bibliographic Details
Published inJapanese Journal of Applied Physics Vol. 56; no. 4; p. 45001
Main Authors Hashimoto, Futo, Mori, Nobuya, Kubo, Osamu, Katayama, Mitsuhiro
Format Journal Article
LanguageEnglish
Published The Japan Society of Applied Physics 01.04.2017
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Summary:Electronic states of laterally coupled graphene nanoribbons (GNRs) have been calculated within a nearest-neighbor tight-binding approximation with varying inter-GNR coupling strength γ from γ = 0 to t (intra-GNR transfer integral). For a coupled zigzag-edge GNR array, both almost flat bands and anisotropic Dirac cones appear near the Fermi level. For a coupled armchair-edge GNR array with a ribbon width N = 3n or 3n + 1, the system is semiconducting with a finite bandgap at γ = 0, which decreases as γ increases. For N = 3n, it becomes metallic with a zero bandgap only at γ = t. On the other hand, for N = 3n + 1, it becomes metallic when γ ≥ t/2. At γ = t/2, a peculiar energy dispersion emerges; the energy dispersion is parabolic perpendicular to the GNR axis and linear parallel to the GNR axis. When N = 3n + 2, the system is always metallic regardless of γ.
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content type line 23
ISSN:0021-4922
1347-4065
DOI:10.7567/JJAP.56.045001