Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Oberflächenphysik Dienstag<br />
der the static conditions of a UHV experiment.<br />
O 26.5 Di 16:45 H45<br />
Photodesorption of small molecules adsorbed on ultrathin Ag<br />
— •Olaf Weisse, Claudia Wesenberg, and Eckart Hasselbrink<br />
— FB Chemie, Universitaet Duisburg-Essen, Universitaetstr. 5, 45117<br />
Essen, Germany<br />
Since the early 1990, Ag is known to grow on the Si(100) surface in a<br />
layer-by-layer fashion. The resulting surface forms an epitaxial Ag(111)<br />
layer. These ultrathin Ag films(20-100ML) are ideally suited to study the<br />
elektron dynamics in such films and the influence of the film thickness<br />
on charge transfer to the adsorbate and subsequent photodesorption. In<br />
our experiments, NO2 is chosen as the probe molecule. Its adsorbtion is<br />
performed at 95 K on the Ag-covered Si(100) surface. Photodesorption<br />
is induced using a Nd:YAG laser (2.3eV/3.5eV/4.6eV) and the desorbed<br />
molecules are detected by QMS. The film thickness is varied in order<br />
to obtain information about the charge transfer dynamics between the<br />
ultrathin Ag film and the NO2 adsorbate. The photodesorption crosssection<br />
of NO2 is expected to decrease with increasing film thickness.<br />
We belive that the photodesorption cross-section will increase due to hot<br />
electrons generated in the semiconductor.<br />
O 26.6 Di 17:00 H45<br />
Surface plasmons of metal islands and their influence on the infrared<br />
absorption of adsorbates — •A. Priebe, G. Fahsold, and<br />
A. Pucci — Kirchhoff-Institut für Physik, Universität Heidelberg,<br />
The surface enhanced infrared absorption (SEIRA) of adsorbates on<br />
nano-structured metal films are widely used in chemistry and biology. For<br />
the first monolayer the typical asymmetric SEIRA line shape can be explained<br />
by an interaction of the adsorbate with electron-hole pairs of the<br />
metal film. But asymmetric SEIRA lines are observed also for vibrations<br />
in multilayers. From experimental results it is known that the asymmetry<br />
and the enhancement of SEIRA lines show a strong dependency on<br />
the filling factor of the metal in the island film. In this work we show<br />
how both, the asymmetry and the enhancement could be explained with<br />
respect to their change with filling factor. Experimental SEIRA spectra<br />
from adsorbates on nanoparticle arrays with ordered facets can be<br />
described by a theory that only considers the interaction of adsorbate<br />
vibrations with surface plasmons of the metal film.<br />
A. Priebe, M. Sinther, G. Fahsold, and A. Pucci J. Chem. Phys. 119<br />
(2003), 4887<br />
O 26.7 Di 17:15 H45<br />
Adsorption of CO on the (10¯10) surface of Rhenium — •C.<br />
Pauls, D. Przyrembel, and K. Christmann — Inst. f. Chemie, FU<br />
Berlin, Takustr. 3, 14195 Berlin<br />
We have performed LEED, thermal desorption (TD), and work function<br />
change (∆Φ) measurements of CO interacting with the ’open’<br />
Re(10¯10) surface. Upon exposure at 200 K, negatively polarised (∆Φ ≈<br />
780 meV) molecular α states are populated. TD spectra reveal these<br />
states between 250 and 400 K (Edes= 95...118 kJ/Mol) and, in addition,<br />
pronounced β states due to dissociated CO between 600 and 800 K. Direct<br />
CO exposure at 500 K exclusively yields dissociated CO as evidenced by<br />
i) 2 nd order desorption kinetics at low coverages (Edes= 207 kJ/Mol) and<br />
O 27 Gaedepreisvortrag Sander<br />
ii) the formation of a p(1x2) LEED phase at a CO coverage of Θ= 0.25.<br />
carbon]. Between 0.125 and 0.16 ML an additional c(2x4) phase appears.<br />
During desorption, both phases undergo an order-disorder transition. In<br />
the coverage range of the p(1x2) phase the respective TD spectra show a<br />
common leading edge (zero-order kinetics) until the critical temperatur<br />
of ∼ 660 K is reached.<br />
O 26.8 Di 17:30 H45<br />
Electronic properties and hydrogen absorption of Pd and Ni:O<br />
nano-clusters — •Andreas Borgschulte, Ruud J. Westerwal,<br />
Sven de Man, Bernard Dam, Jan H. Rector, and Ronald<br />
Griessen — Vrije Universiteit, FEW - Vaste-stoffysica, De Boelelaan<br />
1081, 1081 HV Amsterdam<br />
We studied by scanning tunneling microscopy the electronic and geometric<br />
structure of Pd and Ni nano-clusters grown on oxidized yttrium<br />
surfaces. The catalytic activity of Pd and Ni nano-clusters is estimated<br />
from the optically monitored switching kinetics of the underlying yttrium<br />
layer. The electronic structure depends strongly on the cluster<br />
size and changes after hydrogenation. Small Pd clusters are insulating as<br />
evidenced by tunneling spectroscopy. The critical thickness of the metalinsulator<br />
transition coincidences with the minimal thickness for a significant<br />
catalytic Pd activity. Below the critical thickness nano-clusters have<br />
lost the special catalytic properties of (bulk) Pd. In contrast to Pd, Nisurfaces<br />
oxidize in normal environment (air). In that case the interplay<br />
between hydrogen and oxygen chemisorbed on Ni clusters as well on crystalline<br />
surfaces is studied. Surfaces with a partially reduced oxide show<br />
the catalytically highest activity. The results are compared with X-ray<br />
diffraction studies on the interaction of hydrogen with NiO. We discuss<br />
the relevance of the results for a search of novel catalysts for hydrogen<br />
storage and fuel cells, in particular the role of oxides as catalysts.<br />
O 26.9 Di 17:45 H45<br />
Coadsorption of H and CO on Pd(210) — •Christian Mosch,<br />
Markus Lischka, and Axel Groß — Physics-Department, Technical<br />
University of Munich, D-85747 Garching, Germany<br />
The study of the interaction of molecules with stepped surfaces is of<br />
importance in order to close the structure gap between surface science<br />
and heterogeneous catalysis. We have focused on the adsorption of hydrogen<br />
[1,2] and CO on Pd(210) by performing density functional theory<br />
(DFT) calculations within the generalized gradient approximation. The<br />
(210) surface can be regarded as being built up by small (100) terraces.<br />
CO is known to adsorb on Pd(100) in an upright fashion at the bridge<br />
position [3,4]. On Pd(210), there are two inequivalent bridge positions.<br />
And indeed, we find a relatively small corrugation in the CO adsorption<br />
energies with the two bridge sites being energetically almost degenerate.<br />
CO is furthermore known as a strong poison in heterogeneous catalysis.<br />
We have therefore also addressed the coadsorption of CO with atomic<br />
hydrogen. There is a strong inhibition of the hydrogen adsorption due to<br />
the presence of CO which is analyzed in terms of the electronic structure<br />
of the adsorbate system.<br />
[1] P.K. Schmidt et al., Phys. Rev. Lett. 87, 096103 (2001).<br />
[2] M. Lischka and A. Groß, Phys. Rev. B 65, 075420 (2002)<br />
[3] A. M. Bradshaw and F. M. Hoffmann, Surf. Sci. 72, 513 (1978).<br />
[4] A. Eichler and J. Hafner, Phys. Rev. B 57, 10110 (1998).<br />
Zeit: Mittwoch 15:15–16:00 Raum: H1<br />
Hauptvortrag O 27.1 Mi 15:15 H1<br />
Stress on the atomic scale: From surface reconstruction to stress<br />
oscillations and magnetostriction of atomic layers — •Dirk<br />
Sander — Max-Planck-Institut für Mikrostrukturphysik, Weinberg 2,<br />
D-06120 Halle<br />
Mechanical stress is an important factor, which governs a number<br />
of fundamental aspects in surface science, film growth, and magnetic<br />
anisotropy. Examples are e.g. the surface reconstruction of clean and<br />
adsorbate-covered surfaces, oscillatory stress relaxation in nanosize islands,<br />
and the magnetoelastic coupling in ferromagnetic monolayers.<br />
Stress measurements by the cantilever bending technique are presented<br />
for each example. Film stress in the GPa range, in excess of the tensile<br />
strength of high-strength materials, is measured for epitaxially strained<br />
layers. Structural relaxation due to island growth and coalescence, and<br />
surface alloy formation are comparatively subtle effects, which are detected<br />
by the respective stress signature. The in situ combination of<br />
stress measurements during film growth with magnetoelastic stress measurements<br />
upon magnetization reversal identifies a strain-induced change<br />
of the magnetoelastic coupling constants from the respective bulk value.<br />
The impact on the peculiar magnetic anisotropy of ferromagnetic layers<br />
is discussed.