Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Oberflächenphysik Dienstag<br />
ments and spectroscopic images (dI/dV maps) taken at T = 3.9 K on<br />
this superlattice showing site-dependent characteristic features very different<br />
from the clean Ag(111) surface. Calculations within a nearly free<br />
electron model and tight binding simulations show good agreement with<br />
our data. Furthermore, spectra obtained on compressed and slightly disordered<br />
lattices were successfully simulated and show the dependence of<br />
the LDOS on the local environment. Specifically, we identify the observed<br />
spectroscopic structures with singularities at the high-symmetry points<br />
of the mini-Brillouin zone created by the hexagonal Ce adatom superlattice.<br />
The stability of this superlattice results from the energy gain of<br />
the system manifesting itself by the opening of gaps at the mini-Brillouin<br />
zone boundery.<br />
[1] F. Silly, M. Pivetta, M. Ternes, F. Patthey, J. Pelz, and W.-D.<br />
Schneider, Phys. Rev. Lett., in press.<br />
O 17.8 Di 13:00 H36<br />
Probing of bulk band edges with STM: An ab initio analysis<br />
— •A. Dick 1,2 , M. Hansmann 2 , J.I. Pascual 2,3 , G. Geballos 2,4 ,<br />
H.-P. Rust 2 , K. Horn 2 , and J. Neugebauer 1 — 1 Universität Paderborn,<br />
Dekanat Physik, Warburger Straße 100, D-33098 Paderborn —<br />
2 Fritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, D-<br />
14195 Berlin — 3 Institut de Ciència de Materials de Barcelona - CSIC,<br />
08193 Bellaterra, Spain — 4 Laboratorio Nazionale TASC-INFM, 34012<br />
Trieste, Italy<br />
O 18 Adsorption an Oberflächen I<br />
The analysis of standing electronic waves at noble metal surfaces by<br />
scanning tunneling microscopy/spectroscopy (STM/STS) has given valuable<br />
insight into different surface properties such as, e.g., surface state<br />
lifetimes on free surfaces as well as artificial atomic structures. These<br />
studies, however, were mainly limited to surface states. We have therefore<br />
studied the electronic structure of the Ag(110) surface employing<br />
low temperature STS and density-functional theory. In the calculations<br />
atomic relaxation has been fully taken into account and the convergence<br />
of the slab thickness has been carefully checked. Based on these results<br />
a generalized Tersoff-Hamann theory [1] has been used to simulate STS<br />
spectra. A comparison of the experimental and theoretical spectra showed<br />
excellent agreement and clearly demonstrate that bulk states can be<br />
probed in STS.<br />
[1] A.Selloni et al., Phys. Rev. B 31, 2602 (1985)<br />
Zeit: Dienstag 11:15–13:15 Raum: H38<br />
O 18.1 Di 11:15 H38<br />
Composition of the surface oxide on Pd(100) in an O2 and CO<br />
environment — •Jutta Rogal, Karsten Reuter, and Matthias<br />
Scheffler — Fritz-Haber-Institut der MPG, Berlin,Germany<br />
The oxidation of the Pd(100) surface leads to a ( √ 5 × √ 5)R27 ◦ surface<br />
oxide structure, which was recently identified to be essentially a<br />
PdO(101) overlayer on Pd(100)[1]. In thermodynamic equilibrium with<br />
an O2 gas phase this surface oxide represents the most stable phase over<br />
a wide range of environmental conditions, suggesting that the surface oxide<br />
may play some role in the catalytic oxidation of CO on the Pd(100)<br />
surface.<br />
To get a first insight into this catalytic reaction we investigate the<br />
structure and composition of the surface oxide in equilibrium with an<br />
arbitrary O2 and CO gas environment using density-functional theory<br />
and ”constrained” atomistic thermodynamics[2]. Studying the simultaneous<br />
adsorption of CO and O we arrive at a (T, p)-phase diagram of the<br />
stable structures, and discuss possible kinetic effects due to the ongoing<br />
reaction.<br />
[1] M. Todorova et al., Surf. Sci. 541, 101-112 (2003)<br />
[2] K. Reuter and M. Scheffler, Phys. Rev. B 68, 045407 (2003)<br />
O 18.2 Di 11:30 H38<br />
In-situ XPS studies of CO adsorption on Pd(111) in the pressure<br />
range from 10 −8 to 1 mbar — •J. Pantförder, S. Pöllmann,<br />
D. Borgmann, R. Denecke, and H.-P. Steinrück — Physikalische<br />
Chemie II, Universitaet Erlangen-Nuernberg, Egerlandstr. 3, 91058 Erlangen<br />
In an effort to extend the usable pressure range for electron based spectroscopies<br />
from UHV into the so-called pressure gap region, we have built<br />
a new experimental setup for in-situ XPS up to 1 mbar. The principle of<br />
the high pressure cell is based on several stages of differentially pumping<br />
between sample and electron detection, similar to earlier experimental<br />
setups [1]. In our apparatus the measurements can be performed either<br />
by using an ambient pressure in the cell or by application of a directed<br />
gas beam yielding a considerably lower background pressure. The performance<br />
of the high pressure setup will be discussed by the pressure<br />
dependence of CO adsorption on Pd(111), which can be compared to<br />
SFG and XP measurements [2].<br />
Supported by the DFG (Schwerpunktsprogramm 1091, Ste620/3-3).<br />
[1] H.J. Ruppender et al., Surf. Interface Anal. 15 (1990) 245; R.W.<br />
Joyner et al., Surf. Sci. 87 (1979) 501.<br />
[2] V. V. Kaichev et al., J. Phys. Chem. B 107 (2003) 3522.<br />
O 18.3 Di 11:45 H38<br />
Adsorption of water on Pd(111) — •Ari P Seitsonen 1 , Bako<br />
Imre 2 , Gabor Palinkas 2 , and Jürg Hutter 1 — 1 Physikalisch<br />
Chemisches Institut der Universität Zürich — 2 Chemical Research<br />
Centre of the Hungarian Academy<br />
The adsoprtion of water on transition metal surfaces has recently received<br />
wealth of interest. Our studies are motivated by the STM experiments<br />
by Salmeron and co-workers [Mitsui et al, Science 297 (2002)<br />
1850]. They were able to follow the initial adsorption and diffusion of<br />
small water molecules on Pd(111). We have performed density functional<br />
theory (DFT) calculations on water monomer and dimer on the same surface,<br />
using periodic plane wave/pseudo potential method. We find that<br />
the water dimer adsorbs with only one of the molecules adsorbed directly<br />
on the surface, the second one being bound mainly by the hydrogen bond<br />
between the molecules. Our diffusion barrier for the monomer agrees excellently<br />
with the experimental one, however our diffusion barrier for<br />
the dimer is higher than for the monomer, contradicting the conclusions<br />
achieved in the experiments.<br />
O 18.4 Di 12:00 H38<br />
Angular dependence of H2 dissociation at DB steps of Si(001)<br />
— •C. Stanciu and U. Höfer — Fachbereich Physik, Philipps-<br />
Universität Marburg, D-35032 Marburg<br />
The dynamics of dissociative adsorption of molecular hydrogen at the<br />
DB steps of Si(001) was investigated by performing angular dependent<br />
measurements of the initial sticking coefficient for different kinetic energies<br />
of H2 from a supersonic molecular beam. Optical second-harmonic<br />
generation (SHG) was used as a sensitive monitor of hydrogen coverage<br />
at the steps sites. For Ekin = 350 meV, a kinetic energy that considerably<br />
exceeds the mean barrier height of Ea = 80 meV, the polar distribution<br />
is strongly forward-peaked (∼ cos 7.8 θ) whereas for Ekin < Ea,<br />
H2-momentum parallel to the step edges was found to enhance dissociation,<br />
giving rise, e.g., to a broad polar distribution (∼ cos 1.2 θ) for<br />
Ekin = 30 meV. This behaviour contrasts the one previously observed for<br />
H2 adsorption on the terraces [1]. A sharp angular distribution, directed<br />
along the direction of the dangling bonds, was observed in that case for<br />
Ekin < Ea, indicating a strong lateral corrugation of the barrier height<br />
due to the high directionality of the dangling bonds. The behaviour at<br />
the steps, however, suggests the dominant influence of a geometric corrugation.<br />
Possible origins of such a lateral variation of the barrier position<br />
parallel to the step edges, and effects the steering of low energetic<br />
molecules will be discussed.<br />
[1] M. Dürr and U. Höfer, Phys. Rev. Lett. 88, 076107 (2002)