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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)

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