Počet záznamů: 1  

High-quality PVD graphene growth by fullerene decomposition on Cu foils

  1. 1.
    0483656 - ÚFCH JH 2018 RIV US eng J - Článek v odborném periodiku
    Azpeitia, J. - Otero-Irurueta, G. - Palacio, I. - Martinez, J. I. - Ruiz del Arbol, N. - Santoro, G. - Gutiérrez, A. - Aballe, L. - Foerster, M. - Kalbáč, Martin - Valeš, Václav - Mompean, F. J. - Garcia-Hernandez, M. - Martín-Gago, J.A. - Munuera, C. - Lopez, M. F.
    High-quality PVD graphene growth by fullerene decomposition on Cu foils.
    Carbon. Roč. 119, AUG 2017 (2017), s. 535-543. ISSN 0008-6223. E-ISSN 1873-3891
    Grant CEP: GA MŠMT LL1301
    GRANT EU: European Commission(XE) 696656 - GrapheneCore1
    Institucionální podpora: RVO:61388955
    Klíčová slova: functional perturbation-theory * epitaxial graphene * copper substrate * pt(111) surface * raman-spectrum * cvd-graphene
    Obor OECD: Physical chemistry
    Impakt faktor: 7.082, rok: 2017

    We present a new protocol to grow large-area, high-quality single-layer graphene on Cu foils at relatively low temperatures. We use C-60 molecules evaporated in ultra high vacuum conditions as carbon source. This clean environment results in a strong reduction of oxygen-containing groups as depicted by X-ray photoelectron spectroscopy (XPS). Unzipping of C-60 is thermally promoted by annealing the substrate at 800 degrees C during evaporation. The graphene layer extends over areas larger than the Cu crystallite size, although it is changing its orientation with respect to the surface in the wrinkles and grain boundaries, producing a modulated ring in the low energy electron diffraction (LEED) pattern. This protocol is a self-limiting process leading exclusively to one single graphene layer. Raman spectroscopy confirms the high quality of the grown graphene. This layer exhibits an unperturbed Dirac-cone with a clear n-doping of 0.77 eV, which is caused by the interaction between graphene and substrate. Density functional theory (DFT) calculations show that this interaction can be induced by a coupling between graphene and substrate at specific points of the structure leading to a local sp(3) configuration, which also contribute to the D-band in the Raman spectra. (C) 2017 Elsevier Ltd. All rights reserved.
    Trvalý link: http://hdl.handle.net/11104/0278873

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