Surfaces of complex approximant phases.
V. Fournée 1, A.R.
Ross 2,3, T.A. Lograsso 2,3, J.A. Barrow 2,5,
M. Shimoda 4, A.P. Tsai 4
and P.A. Thiel 2,5.
1 LSG2M, CNRS-UMR7584,
Ecole des Mines, Parc de Saurupt, 54042 Nancy, France.
2 Ames Laboratory, Iowa
State University, Ames, Iowa 50011, USA.
3 Department of Materials
Science and Engineering, Ames, Iowa 50011, USA.
4 National Institute for
Material Science, 1-2-1 Sengen, Tsukuba-shi, Ibaraki 305-0047 Japan.
5 Department of Chemistry,
Iowa State University, Ames, Iowa 50011, USA.
In a first part, we will present experimental results
on the surface structure and stability of approximant phases. Surface of
approximant can be produced "accidentally". This sometime occurs on the 5-fold
surface of the Al-Pd-Mn icosahedral quasicrystal (IQC) when the chemical
composition is driven out of the stability range of the icosahedral phase
during the sputtering and annealing. Structural identification of such crystalline
overlayers based on the analysis of STM images will be presented.
In rare cases, it is also possible to grow single
crystals of approximant large enough for surface science studies. This is
the case for the xÕ-AlPdMn approximant. Two
single crystals of this phase were grown : one by the Bridgman method (BG
sample), the other by a self-flux technique (FG sample). The surface structure
perpendicularly to the pseudo ten-fold axis is investigated by STM and LEED
and compared to the bulk structural model. For both samples, the LEED pattern
shows the expected pseudo ten-fold symmetry, but the local probe of the STM
reveals different morphologies. In particular, high-resolution images reveal
motifs with 5-fold or 10-fold symmetry protruding atop the terraces. They
are identified as part of 3D cluster units from which the xÕ phase can be described. These cluster
sites are preferred over the glue sites during the re-growth of the surface
upon sputtering-annealing. This is in contrast with the 5-fold surface of
the Al-Pd-Mn IQC where the surface re-growth encompasses not only the cluster
sites but also the "glue sites," forming together a relatively dense and
flat top layer. This observation raises question about the relative stability
of clusters and their influence on surface stability.
In a second part, we will describe
the growth and properties of a Pd film deposited
on the xÕ approximant surface. This
topic is related to the catalytic properties of quasicrystal. Deposited Pd
atoms form a rough film with nanosized particles rather than a smooth film.
The
density of Pd particles is high. They are rather stable and the rough aspect
of the film persists even after a short annealing to 920 K. Spectroscopy
data are consistent with a reduced density of states at EF on
the clean surface of the xÕ approximant.
With increasing film thickness, the surface electronic structure changes
from that of a poor metal (with a pseudogap at EF) to that of
a good metal like Pd, and this transition already occurs by 3.5 ML. It follows
that the surface area of the active catalyst (Pd) is large, consistent with
the high catalytic activity measured for AlPdMn IQC. It is also possible that
the catalytic activity derives from a perturbation to the electronic structure,
as we observe for the small Pd particles. Such an effect is known to occur
for other catalytically-active particles.