Chemistry Reference
In-Depth Information
For stability issues special model catalysts have to be designed with dis-
tinct morphologies in order to be able to visualize and follow structural
degradation of the model catalyst after reaction with scanning electron
microscopy (SEM). In stability studies we applied RuO
2
-based and CeO
2
-
based nanofibers as model catalysts (cf. Figure 8.1d). These model systems
bear the additional advantage of having large active surface areas of about
20-30 m
2
g
1
to conduct kinetic studies in a typical flow reactor set-up.
d
n
9
r
4
n
g
|
8
8.3 Synthesis of Single Crystalline RuO
2
Films for
Gaining Molecular Information on Stability and
Activity
In order to produce single crystalline RuO
2
films with specific
surface orientations one can start from metallic Ru single crystals which
are cut along particular directions. A well-ordered crystalline RuO
2
film is
grown by exposing the single crystalline Ru surfaces to large amounts of
molecular oxygen (say 10
6
L, at 10
5
mbar; 1 L (where L means Langmuir)
corresponds to an exposure of 1.33
10
6
mbars) at temperatures in the
range from 600 to 750 K. This procedure leads to the growth of a 1-2 nm
thick RuO
2
film. On the Ru(0001) surface a single crystalline RuO
2
film in
(110) orientation is preferentially formed (cf. Figure 8.1a),
35,36
while on the
Ru
ð
1010
Þ
a high quality RuO
2
film in (100) orientation can be grown.
37,38
Occasionally other orientations are observed on the Ru(0001) and Ru
ð
1010
Þ
single crystal surfaces, such as (101).
39,40
Unfortunately RuO
2
films thicker
than 3-5 nm can only be formed at higher surface temperatures, where
the oxide surface roughens considerably,
.
forming facets with various
orientations.
40
Thicker (and flat) single crystalline RuO
2
(110) films with variable thick-
ness of several 10 nm can be prepared on TiO
2
(110) single crystals serving as
templates.
41-43
Ru-carbonyls are frequently used as Ru-containing pre-
cursors and the actual oxidation process is assisted by an oxygen plasma.
The adsorption and decomposition of (Ru)
3
(CO)
12
over TiO
2
(110) has been
studied in great detail by XPS and RAIRS.
44,45
However, carbon contamin-
ation is unavoidable. At growth temperatures above 700 K Ti and Ru inter-
diffuse to form mixed Ru
x
Ti
2
x
O
2
epitaxial films. This mixed oxide buffer-
film can be utilized to minimize the lattice mismatch between RuO
2
(110)
and TiO
2
(110), thereby producing flat single crystalline unstrained
RuO
2
(110) films of more than 20 nm thickness.
43
Very recently, RuO
2
islands
and closed films epitaxially grown on TiO
2
(110) could be prepared
(cf. Figure 8.1b) using an electron beam induced Ru evaporation as a carbon-
free Ru source.
46
Thin films of RuO
2
can be produced either by deposition of Ru and
subsequent oxidation of Ru films, or directly by deposition of RuO
2
. For
instance, ultra-thin highly textured Ru films in (0001) orientation can be
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