1. High-quality PVD graphene growth by fullerene decomposition on Cu foils
- Author
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José A. Martín-Gago, V. Vales, Mar García-Hernández, Carmen Munuera, Michael Foerster, Jon Azpeitia, José I. Martínez, Gonzalo Otero-Irurueta, Lucia Aballe, María Francisca López, Gonzalo Santoro, M. Kalbac, N. Ruiz del Árbol, Federico Mompean, Alejandro Gutiérrez, Irene Palacio, European Commission, Ministerio de Economía y Competitividad (España), European Research Council, and Fundação para a Ciência e a Tecnologia (Portugal)
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Materials science ,Fullerene ,Ultra-high vacuum ,Nanotechnology ,02 engineering and technology ,010402 general chemistry ,7. Clean energy ,01 natural sciences ,Article ,law.invention ,symbols.namesake ,X-ray photoelectron spectroscopy ,law ,General Materials Science ,Graphene oxide paper ,Low-energy electron diffraction ,Graphene ,General Chemistry ,021001 nanoscience & nanotechnology ,0104 chemical sciences ,13. Climate action ,Chemical physics ,symbols ,0210 nano-technology ,Raman spectroscopy ,Graphene nanoribbons - Abstract
We present a new protocol to grow large-area, high-quality single-layer graphene on Cu foils at relatively low temperatures. We use C60 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 C60 is thermally promoted by annealing the substrate at 800 °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 sp3 configuration, which also contribute to the D-band in the Raman spectra., Financial support from EU Horizon 2020 research and innovation program under grant agreement No. 696656 (GrapheneCore1-Graphene-based disruptive technologies) and Spanish MINECO (grants MAT2014-54231-C4-1-P,MAT2014-52405-C2-2-R, CSD2009-00013, MAT2015-64110) is acknowledged. JA and NR are supported by the FPI program from MINECO (BES-2012-058600 and BES-2015-072642, respectively). CM and JIM acknowledge the financial support by the “Ramón y Cajal” Program of MINECO (RYC-2014-16626 and RYC-2015-17730, respectively). JIM and GS acknowledge funding from the ERC-Synergy Program (grant ERC-2013-SYG-610256 Nanocosmos). JIM thanks CTI-CSIC for use of computing resources. MK and VV acknowledge funding from ERC-CZ (LL1301) project. GO-I acknowledges FCT for his grant (SFRH/BPD/90562/2012).
- Published
- 2017
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