APS March Meeting 2010
Volume 55, Number 2
Monday–Friday, March 15–19, 2010;
Portland, Oregon
Session T32: Focus Session: Self Assembly on Novel Templates
2:30 PM–5:18 PM,
Wednesday, March 17, 2010
Room: E142
Sponsoring
Unit:
DCMP
Chair: Karsten Pohl, University of New Hampshire
Abstract ID: BAPS.2010.MAR.T32.5
Abstract: T32.00005 : Regular metal cluster arrays on graphene/Ir(111)
3:42 PM–4:18 PM
Preview Abstract
Abstract
Author:
Alpha T. N'Diaye
(Uni K\"oln / Lawrence Berkerley National Lab)
Clusters represent a distinct state of matter. Due to their size,
they exhibit a broad range of new properties, such as magnetism
for normally non magnetic materials, a highly increased catalytic
activity, or size effects in the electronic spectrum.
These properties are of relevance for information technology or
energy efficiency.
The controlled growth of clusters on a surface is still a challenge.
We have grown regular arrays of various metal clusters (Ir, Pt,
W, Re, Au, IrFe, IrAu) on a self organized graphene/Ir(111)
moir\'{e} template by physical vapor deposition in ultra high
vacuum and studied them with scanning tunneling microscopy.
The template epitaxial graphene grown by the thermal
decomposition of ethene (C$_2$H$_4$) on Ir(111).
This yields a moir\'{e} superstructure with a periodicity of 25.3\AA.
Upon physical vapor deposition of metals, clusters nucleate in
the cells of moir\'{e} superstructure.
The clusters are perfectly ordered in a hexagonal array with an
nearest neighbour distance given by the 25.3{\AA} periodicity of
the moir\'e.
Clusters bind to the graphene layer via a local rehybridization
of the carbon from sp$^2$ to sp$^3$ underneath the cluster.
The average number of atoms in a cluster can be tuned by the
amount of deposited metal, which is for Ir from 4.5 -- 130 atoms.
Despite their small size, the clusters possess a high temperature
stability.
While small Au clusters are only stable at temperatures around
100\,K Ir, clusters are stable above 500\,K.
The decay of the areal density of clusters can be described by an
Boltzmann law with a very low effective attempt frequency below
1000\,Hz and energy barriers between 0.4 -- 0.8\,eV.
The coalescence occurs through two different types of atomic
process: complete coalescence for two small clusters results in
one cluster occupying a single moir\'{e} cell, while for large
clusters a sintering takes place. The resulting cluster spans
multiple moir\'{e} cells.
For some materials, which do not form ordered cluster arrays at
room temperature, the formation of regular cluster superlattices
can be enhanced by a lower substrate temperature. This method is
demonstrated for Au and Re. The obtained Re clusters remain
stable at room temperature.
A second method, to form clusters containing materials, which do
not form clusters at room temperature which is demonstrated for
Fe and Au at room temperature.
We seeded the superlattice with small Ir clusters and in a second
step used these well ordered array of Ir clusters to anchor
additional Fe or Au.
The graphene/Ir(111) moir\'{e} is a versatile template for the
growth of regular metal cluster arrays.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2010.MAR.T32.5