Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Oberflächenphysik Montag<br />
O 14.6 Mo 18:00 Bereich C<br />
Physisorption systems with moderate lattice mismatch: The<br />
structure of CO2/KCl(100) — Milica Hadnadev 1 , J.-Peter<br />
Toennies 2 , Franziska Traeger 2 , •Jochen Vogt 1 , and Helmut<br />
Weiss 1 — 1 Chemisches Institut, Universität Magdeburg, Universitätsplatz<br />
2, 39106 Magdeburg, Germany — 2 Max-Planck-Institut für<br />
Strömungsforschung, Bunsenstr. 10, 37073 Göttingen, Germany<br />
Weakly bound adsorbates with a moderate lattice mismatch between<br />
the solid adsorptive and the substrate are examples of self-organizing<br />
systems in which short-range forces may induce complicated long-range<br />
order. The lattice constant of solid CO2 is 12 % smaller than that of<br />
KCl(100). On the latter CO2 initially adsorbs in an unsaturated phase<br />
with (2 √ 2× √ 2)R45 ◦ symmetry which is barely visible at 80 K and wellordered<br />
at 20 K. The saturated 2D phase forms a (6 √ 2× √ 2)R45 ◦ lattice,<br />
verified both with helium atom scattering (HAS) and low-energy electron<br />
diffraction (LEED). Moreover, we use polarization infrared spectroscopy<br />
(PIRS) and show that dense phase IR spectra in the region of the CO2<br />
asymmetric stretch vibration are consistent with dynamic dipole-dipole<br />
coupling of 12 molecules in the corresponding unit cell. The spectra reveal<br />
an aging of the freshly prepared layer within short time. This is attributed<br />
to the heat of adsorption (25±1 kJ/mol) being slightly lower than the<br />
heat of sublimation of solid CO2 (27 kJ/mol). Hence the 2D layer should<br />
be metastable and form 3D clusters. The 2D phase collapses immediately<br />
to the latter upon exposure to acetylene, which has no lattice mismatch<br />
to KCl(100) and a heat of adsorption of 27 kJ/mol.<br />
O 14.7 Mo 18:00 Bereich C<br />
Manipulation of ultrafast surface processes by means of fs-pulse<br />
shaping — •Felix Steeb, Marlies Wessendorf, Jörg Lange,<br />
Alexander Mönnich, Michael Bauer, and Martin Aeschlimann<br />
— FB Physik, TU Kaiserslautern, Erwin-Schrödinger-Str. 46, 67663<br />
Kaiserslautern<br />
In the last years, coherent control of chemical reactions in the gas<br />
phase [1], or in the liquid phase [2] by means of adaptive femtosecond<br />
pulse shaping has been demonstrated.<br />
In this paper, we present application of the pulse shaping technique to<br />
the optimization / manipulation of ultrafast surface processes, such as<br />
surface chemical reactions.<br />
The apparatus used to shape 20 fs pulses consists of an all-reflective<br />
zero-dispersion compressor in combination with a programmable 640stripe<br />
liquid crystal spatial light modulator (SLM). A closed loop setup,<br />
controlled by an evolutionary algorithm [3], iteratively achieves optimization<br />
of an experimental signal which is used as feedback. We find that<br />
the Two-Photon-Photoemission Yield, e.g. measured from an adsorbate<br />
resonance on the system Cs/Cu(111), is a possible detection scheme that<br />
enables us to control specific surface-related properties. The experimental<br />
setup, preliminary results and future prospects will be discussed.<br />
[1] A. Assion et al.: Science 282, 919 (1998)<br />
[2] T. Brixner et al: Nature 414, 57 (2001)<br />
[3] D. Zeidler et al.: Phys. Rev. A 64, 023420 (2001)<br />
O 14.8 Mo 18:00 Bereich C<br />
Growth and thermal stability of Ni adsorption layers on<br />
the (111) Mo crystal surface — •Cezary Tomas 1,2 , Jan<br />
Kolaczkiewicz 1 , and Herbert Pfnür 2 — 1 Institute of Experimental<br />
Physics, University of Wroclaw, Poland — 2 Institut Für<br />
Festkörperphysik, Universität Hannover, Germany<br />
The low-density (111) surfaces of bcc metals have a high surface free<br />
energy and undergo faceting at sufficiently high temperatures, when covered<br />
with a chemisorbed layer. However, not all chemisorbed adsorbates<br />
lead to this process. Madey and coworkers have studied the reconstruction<br />
of the W(111) surface. They found that faceting occurs in the presence of<br />
metals with electronegativity 2 or more on the Pauling scale. Our results<br />
do not support this classification. We suggest that the major cause of<br />
faceting is the adsorbate-substrate and adsorbate-adsorbate interaction<br />
and the magnitude of the atomic radii of the adsorbate and substrate.<br />
The goal of this study was to investigate the growth mechanism and the<br />
thermal stability of Ni layers adsorbed on the (111) Mo surface. AES,<br />
LEED, ∆φ and STM has been used in this work. We find that Ni does<br />
not cause faceting. Only for coverages Θ > 3ML 3D crystallites appear<br />
on the surface and pass into 2D forms with increasing temperature.<br />
O 14.9 Mo 18:00 Bereich C<br />
CO adsorption and desorption processes on Pt(355) investigated<br />
by in-situ high resolution XPS — •B. Tränkenschuh, T.<br />
Fuhrmann, C. Papp, J. F. Zhu, R. Denecke, and H.-P. Steinrück<br />
— Physikalische Chemie II, Universität Erlangen-Nürnberg, Egerlandstr.<br />
3, 91058 Erlangen<br />
The adsorption and thermal desorption of CO on a Pt(355) surface<br />
was studied by the combination of a supersonic molecular beam and<br />
in-situ high resolution XPS. This surface contains five atom wide (111)<br />
terraces separated by monatomic steps with (111) orientation. By using<br />
synchrotron radiation we are able to clearly distinguish between adsorption<br />
sites at steps and at terraces in O 1s and C 1s spectra, even at<br />
fast measuring times (about 4 s per spectrum). The terrace adsorption<br />
sites are comparable to those on a Pt(111) surface, namely bridge and<br />
on-top bound species which are well known in literature [1]. Our measurements<br />
show that first the step sites and than the on-top and bridge sites<br />
on the terraces are occupied. The desorption is studied by temperatureprogrammed<br />
XPS and TPD. Supported by the DFG (STE 620/4-2).<br />
[1] M. Kinne et al., J. Chem. Phys. 117, 23 (2002).<br />
O 14.10 Mo 18:00 Bereich C<br />
Influence of Surface Roughness on the Wetting Behaviour of<br />
Liquid Helium on Alkali Metal Surfaces — •Martin Zech, Armin<br />
Fubel, Jürgen Klier, and Paul Leiderer — University of Konstanz,<br />
Department of Physics, 78457 Konstanz, Germany<br />
For many times wetting transitions have been observed for helium and<br />
hydrogen on certain alkali metal surfaces. However, there exist discrepancies<br />
in the measured contact angles and accompanying hysteresis, in<br />
the movement of the helium contact lines, and sometimes even in the<br />
wetting temperature. Surface roughness is expected to have a significant<br />
influence on the wetting properties, but the working mechanism is not<br />
clearly understood yet. For this reason we have developed a special low<br />
temperature setup. This allows simultaneously an in situ evaporation of<br />
the alkali metals, an investigation of the substrate surface using a scanning<br />
tunnelling microscope (STM), and an investigation of the wetting<br />
behaviour of liquid helium on those surfaces. A coherence between different<br />
surface nanostructuring and emerging wetting phenomena is aimed<br />
to be obtained.<br />
O 14.11 Mo 18:00 Bereich C<br />
Adsorption and decompostion of prenal on Pt(111) — •Jan<br />
Haubrich, Alexander Krupski, Conrad Becker, and Klaus<br />
Wandelt — Institut für Physikalische und Theoretische Chemie, Wegelerstrasse<br />
12, D-53115 Bonn, Germany<br />
The adsorption of prenal on Pt(111) is investigated with HREELS,<br />
TPD and LEED. After adsorption of prenal on Pt(111) at 100K the<br />
desorption of fragments between 1 and 100 amu has been studied with<br />
TPD for series of a increasing exposures. Only signals of the masses 2,<br />
28 and 84 (prenal) have been detected. The TPD results indicate that<br />
molecular prenal desorbs from a monolayer, a 2nd adsorption state and<br />
multilayer at 199K, 177K and 160 K, respectively. For the mass 28, a signal<br />
is observed around 420K, saturating below the monolayer exposure<br />
and pointing towards the decarbonylation of an irreversibly adsorbed<br />
submonolayer species. Several signals are detected for molecular hydrogen<br />
desorption between 285K and 480K. HREELS experiments carried<br />
out between 100K and 500K show only small shifts for the reversibly adsorbed<br />
species, while the species remainig above 199K shows some shifts<br />
and sizeable changes in scattering intensities. Above 420K only traces of<br />
hydrocarbon species can be observed by HREELS.<br />
O 14.12 Mo 18:00 Bereich C<br />
HR-XPS study of furan and pyrrole on Ni(111): reactions of<br />
unsaturated hetero ring systems — •C. Papp, R. Denecke, and<br />
H.-P. Steinrück — Physikalische Chemie II, Universität Erlangen-<br />
Nürnberg, Egerlandstr. 3, 91058 Erlangen<br />
The examination of the two hetero-cycles, furan (C4H4O) and pyrrole<br />
(C4H5N) on the Ni(111) surface with temperature programmed XPS<br />
(TP-XPS) and temperature programmed desorption (TPD) was conducted<br />
in a larger effort to understand the adsorption and reaction of<br />
aromatic molecules on single crystal surfaces. The XP spectra of C 1s,<br />
O 1s and N 1s core levels were recorded with the high resolution and<br />
high flux of the third generation synchrotron source MAX II. In both<br />
hetero-cycles the inequivalent C atoms can be clearly resolved. The two<br />
molecules show significant differences in their reaction behavior. Furan<br />
decomposes at 200 K by forming CO, which is desorbing at 430 K, and