18 Research focus and highlights – Synchrotron light
PSI Scientific Report 2008
Structure and trapping properties of corrugated monolayers – new results from across the SLS Domenico Martoccia, Matts Björck, Christian Schlepütz, Stephan Pauli, Bruce Patterson, Philip Willmott, Hugo Dil, Luc Patthey, Swiss Light Source (SLS), PSI; Jorge Lobo-Checa, Nanolab, University of Basel; Simon Berner, Thomas Brugger, Jürg Osterwalder, Thomas Greber, Physics Institute, University of Zurich
The physical properties of the isoelectronic, two-dimensional structures of graphene and hexagonal boron-nitride are complementary and may also in combination become technologically useful. On solid supports, both deviate from a perfectly flat honeycomb structure and provide the possibility to functionalize them as templates for nanoscaled arrays among other applications. Structural and electronic studies of these systems performed at the Swiss Light Source have provided new insights for their potential use in areas as diverse as molecular recognition, nanoarrays, and novel electronic device fabrication.
Graphene and hexagonal boron-nitride (h-BN) are honeycomb
this inconsistency. Only surface X-ray diffraction (SXRD) has
structures that can be grown as single layers, or “sheets”, on
the necessary resolution (approximately two parts in ten-
2
crystalline substrates. The bonding between these sp -hybrid-
thousand of an in-plane reciprocal lattice unit), and hence
ised, two-dimensional structures and the substrate varies
SXRD studies were performed on g/Ru at the Materials Science
periodically, due to a moiré-like interference caused by differ-
beamline of the SLS.
ences in their respective in-plane lattice constants. As a
Surprisingly, in-plane SXRD measurements showed that the
consequence, the atomic sheets become corrugated, resulting
moiré structure agrees with neither of those previously pro-
in features with periods of a few tens of Ångströms. They are
posed, but is in fact unambiguously 25-on-23, having a pe-
characterised by pronounced and separated triangular elevations on a hexagonal network in the case of graphene, but in h-BN the elevations are more hexagonal with wire-like connected rings, and is thus referred to as a “nanomesh”. Their future use as nanotemplates for molecular arrays and in recognition of macromolecules is a tantalizing prospect that can be better assessed only by a deeper understanding of their structures and electronic properties. With this in mind, studies of these systems have been performed at the Surface Diffraction Station and Surface and Interface Spectroscopy Beamline of the Swiss Light Source.
Graphene on Ruthenium Initial studies of graphene on Ru(0001) (g/Ru) using techniques such as scanning tunneling microscopy and low-energy electron-diffraction produced mutually contradictory results: two different structures were proposed – one in which (1212) graphene hexagons lie on (1111) Ru unit cells (denoted henceforth as 12-on-11) [1], and another suggesting an 11-on-10 structure [2]. None of these studies, however, had the necessary spatial sensitivity to unambiguously resolve
Figure 1: (a) The vertical displacement field (in Å) of the corrugated supercell of graphene on Ru, which consists of four, not quite identical, subunits; (b) The ruthenium substrate is also slightly corrugated, in antiphase to the graphene.