Controlling the interlayer coupling in two-dimensional
(2D) materials
generates novel electronic and topological phases. Its effective implementation
is commonly done with a transverse electric field. However, phases
generated by high displacement fields are elusive in this standard
approach. Here, we introduce an exceptionally large displacement field
by structural modification of a model system: AB-stacked bilayer graphene
(BLG) on a SiC(0001) surface. We show that upon intercalation of gadolinium,
electronic states in the top graphene layers exhibit a significant
difference in the on-site potential energy, which effectively breaks
the interlayer coupling between them. As a result, for energies close
to the corresponding Dirac points, the BLG system behaves like two
electronically isolated single graphene layers. This is proven by
local scanning tunneling microscopy (STM)/spectroscopy, corroborated
by density functional theory, tight binding, and multiprobe STM transport.
The work presents metal intercalation as a promising approach for
the synthesis of 2D graphene heterostructures with electronic phases
generated by giant displacement fields.