Wide bandgap semiconductor from a hidden 2D incommensurate graphene phase
arXiv:1610.02114 · doi:10.1021/acs.nanolett.6b04196
Abstract
Producing a usable semiconducting form of graphene has plagued the development of graphene electronics for nearly two decades. Now that new preparation methods have become available, graphene's intrinsic properties can be measured and the search for semiconducting graphene has begun to produce results. This is the case of the first graphene "buffer" layer grown on SiC(0001) presented in this work. We show, contrary to assumptions of the last forty years, that the buffer graphene layer is not commensurate with SiC. The new modulated structure we've found resolves a long standing contradiction where ab initio calculations expect a metallic buffer, while experimentally it is found to be a semiconductor. Model calculations using the new incommensurate structure show that the semiconducting -band character of the buffer comes from partially hybridized graphene incommensurate boundaries surrounding unperturbed graphene islands.
arXiv comment17 pages, 4 figures, 1 table, 47 references, supplemental material: 15 pages, 4 figures
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Cited by in corpus (7)
- The structure and evolution of semiconducting buffer graphene grown on SiC(0001)
- Graphene: Free electron scattering within an inverted honeycomb lattice
- Dirac Fermion Cloning, Moir Flat Bands and Magic Lattice Constants in Epitaxial Monolayer Graphene
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- Edge states and ballistic transport in zig-zag graphene ribbons: the role of SiC polytypes
- The effects of Moire lattice on the electronic properties of graphene
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