Epitaxial growth of mono- and (twisted) multilayer graphene on SiC(0001)
cond-mat.mtrl-sci, cond-mat.mes-hall
Submitted: 2024-11-18
Updated: 2024-11-18
Comments: 14 + 1 pages, 9 + 1 figures
Journal ref: Phys. Rev. Materials 9, 044003 (2025)
DOI: 10.1103/PhysRevMaterials.9.044003
License: http://creativecommons.org/licenses/by-sa/4.0/
The gist: To take full advantage of twisted bilayers of graphene or other two-dimensional materials, it is essential to precisely control the twist angle between the stacked layers, as this parameter
Terminology
Abstract
To take full advantage of twisted bilayers of graphene or other two-dimensional materials, it is essential to precisely control the twist angle between the stacked layers, as this parameter determines the properties of the heterostructure. In this context, a growth routine using borazine as a surfactant molecule on SiC(0001) surfaces has been reported, leading to the formation of high-quality epitaxial graphene layers that are unconventionally oriented, i.e., aligned with the substrate lattice (G- R0) [Bocquet et al. Phys. Rev. Lett. 125, 106102 (2020)]. Since the G- R0 layer sits on a buffer layer, also known as zeroth-layer graphene (ZLG), which is rotated 30 with respect to the SiC substrate and still covalently bonded to it, decoupling the ZLG- R30 from the substrate can lead to high-quality twisted bilayer graphene (tBLG). Here we report the decoupling of ZLG- R30 by increasing the temperature during annealing in a borazine atmosphere. While this converts ZLG- R30 to G- R30 and thus produces tBLG, the growth process at elevated temperature is no longer self-limiting, so that the surface is covered by a patchwork of graphene multilayers of different thicknesses. We find a 20% coverage of tBLG on ZLG, while on the rest of the surface tBLG sits on one or more additional graphene layers. In order to achieve complete coverage with tBLG only, alternative ways of decoupling the ZLG, e.g., by intercalation with suitable atoms, may be advantageous.
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