posted on 2020-06-11, 21:14authored byAmirhossein Bayani, Karin Larsson
The
process of Au intercalation into a SiC/buffer interface has
been theoretically investigated here by using density functional theory
(DFT) and the nudged elastic band (NEB) method. Energy barriers were
at first calculated (using NEB) for the transfer of an Au atom through
a free-standing graphene sheet. The graphene sheet was either of a
nondefect character or with a defect in the form of an enlarged hexagonal
carbon ring. Defects in the form of single and double vacancies were
also considered. Besides giving a qualitative prediction of the relative
energy barriers for the corresponding SiC/buffer interfaces, some
of the graphene calculations also proved evidence of energy minima
close to the graphene sheet. The most stable Au positions within the
SiC/buffer interface were, therefore, calculated by performing geometry
optimization with Au in the vicinity of the buffer layer. Based on
these NEB and DFT calculations, two factors were observed to have
a great influence on the Au intercalation process: (i) energy barrier
and (ii) preferential bonding of Au to the radical C atoms at the
edges of the vacancies. The energy barriers were considerably smaller
in the presence of vacancies. However, the Au atoms preferred to bind
to the edge atoms of these vacancies when approaching the buffer layer.
It can thereby be concluded that the Au intercalation will only occur
for a nondefect buffer layer when using high temperature and/or by
using high-energy impacts by Au atoms. For this type of Au intercalation,
the buffer layer will become completely detached from the SiC surface,
forming a single layer of graphene with an intact Dirac point.