Issue 4, 2014

Experimentally determined model of atmospheric pressure CVD of graphene on Cu

Abstract

We investigate the critical methane concentration (CMC) during the atmospheric-pressure chemical vapor deposition (AP-CVD) of graphene on Cu from CH4. Above the CMC, graphene both nucleates and grows; below the CMC, it etches; while at the CMC, carbon intermediate species attach and detach from graphene at equal rates. By studying how the CMC varies with [H2] and temperature, we determine the reaction mechanism and the intermediates. We find that the CMC scales with [H2]3/2 and determine a single Arrhenius temperature dependence close to the expected equilibrium value. For [CH4] > CMC, the radial growth rate is proportional to the “building unit” supersaturation indicating that graphene growth occurs under capture-limited kinetics through an intermediate hydrocarbon that is first-order dependent on [CH4] and proportional to [H2]−3/2. We develop a CH4 decomposition and capture model which is consistent with all measurements indicating that the intermediate is CH. We find that uniform monolayer graphene can only be achieved in AP-CVD near the CMC, with a nucleation density that varies 5 orders of magnitude from 880 to 1075 °C. Thus, our work also provides a roadmap for growing uniform graphene at atmospheric pressure on Cu over a broad range of experimental conditions.

Graphical abstract: Experimentally determined model of atmospheric pressure CVD of graphene on Cu

Supplementary files

Article information

Article type
Paper
Submitted
04 Sep 2013
Accepted
22 Nov 2013
First published
25 Nov 2013

J. Mater. Chem. C, 2014,2, 744-755

Experimentally determined model of atmospheric pressure CVD of graphene on Cu

N. S. Safron and M. S. Arnold, J. Mater. Chem. C, 2014, 2, 744 DOI: 10.1039/C3TC31738B

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