Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Oberflächenphysik Donnerstag<br />
is identified as the lowest energy configuration over a broad range of oxygen<br />
pressures. The stabilization of the Fe3O4(001)-surface goes together<br />
with significant changes in the electronic and magnetic properties, e.g. a<br />
halfmetal-to-metal transition. [1] K. Reuter and M. Scheffler, Phys. Rev.<br />
O 30 Hauptvortrag Denecke<br />
B 65, 035406, (2002). [2] R. Pentcheva et al., Phys. Rev. Lett. 90, 076101<br />
(2003). (in collab. with M. Scheffler and W. Moritz; DFG support, PE<br />
883)<br />
Zeit: Donnerstag 10:15–11:00 Raum: H36<br />
Hauptvortrag O 30.1 Do 10:15 H36<br />
Surface chemistry studied by in-situ x-ray photoelectron spectroscopy<br />
— •Reinhard Denecke — Physikalische Chemie II, Universität<br />
Erlangen-Nürnberg, Egerlandstr. 3, 91058 Erlangen<br />
Important aspects of surface science are the dynamics of adsorption<br />
and reaction processes. Using high-resolution x-ray photoelectron spectroscopy<br />
together with high flux synchrotron radiation and in combination<br />
with a molecular beam, such time-dependent processes can be<br />
followed on a time scale of seconds. Spectroscopic information about the<br />
O 31 Oberflächenreaktionen II<br />
species involved can be obtained from the binding energy shifts of adsorbate<br />
and substrate core levels. In the case of hydrocarbons, the vibrational<br />
fine structure can additionally be used to identify surface species.<br />
From quantitative information obtained by intensity analysis, kinetic parameters<br />
can be derived. Examples are discussed for bimolecular reactions<br />
(CO oxidation), activated adsorption (dissociative adsorption of methane<br />
and ethane) and thermal dehydrogenation of hydrocarbons.<br />
Supported by the DFG (Ste 620/4-2).<br />
Zeit: Donnerstag 11:15–13:00 Raum: H36<br />
O 31.1 Do 11:15 H36<br />
Rastertunnelmikroskopische Untersuchung elektroneninduzierter<br />
Prozesse an D2O-Molekülen und -Clustern auf fcc(111)-<br />
Metalloberflächen — •Heiko Gawronski, K. Morgenstern, K.-<br />
F. Braun und K.-H. Rieder — Freie Universität Berlin, Institut für<br />
Experimentalphysik, Arnimallee 14, 14195 Berlin<br />
Diffusion von D2O-Molekülen und kleinen Clustern auf Ag(111)<br />
und Au(111) wird bei 5,5K mittels des Elektronenstroms eines<br />
Tieftemperatur-Rastertunnelmikroskops(RTM) induziert. Hierbei wird<br />
die Abhängigkeit der Diffusion von der Anregungsenergie und der Anregungsdauer<br />
untersucht. Dies erlaubt es, Aussagen über die Abhängigkeit<br />
der Oberflächenreaktionen vom Adsorptionsplatz, der Clustergröße sowie<br />
der angeregten molekularen Schwingung zu treffen. Zunächst werden<br />
die Adsorbate über ihre scheinbaren Höhen identifiziert. Anschließend<br />
induziert man eine diffusive Bewegung durch Injektion von Tunnelelektronen<br />
verschiedener Energie und bestimmt so die Anregungsenergien<br />
der D2O-Moleküle auf den beiden Substraten. Für einzelne Moleküle liegen<br />
diese bei (400±10)mV auf Ag(111) bzw. (440±10)mV auf Au(111)<br />
wobei die Diffusion nach durchschnittlich 0,5ms erfolgt. Die Anregung<br />
der Diffusion eines D2O-Clusters mit der RTM-Spitze direkt über einem<br />
Cluster benötigt auf Au(111) eine Anregungsenergie von (250±10)mV,<br />
während eine Anregung mit der Spitze im Abstand einiger nm erst bei<br />
(480±10)mV stattfindet. Diese Ergebnisse werden mit Ergebnissen von<br />
H2O auf Cu(111) und auf Ag(111) verglichen.<br />
O 31.2 Do 11:30 H36<br />
Interaction of He, Ne and Ar metastable atom beams<br />
with multilayer tunnel systems — •Domokos Kovacs 1 , Johannes<br />
Berndt 1 , Jörg Winter 1 , and Detlef Diesing 2 —<br />
1 Experimentalphysik 2, Ruhr-Universität Bochum — 2 Institut für<br />
Schichten und Grenzflächen 3, Forschungszentrum Jülich<br />
The collision of metastable rare gas atoms He, Ne and Ar with a metal<br />
surface is a well investigated process in surface science. The process leads<br />
with an efficient rate to a relaxation of the atoms and a simultaneous electron<br />
emission from the metal surface. The energy spectrum of the emitted<br />
electrons is a wide distribution with a maximal energy of 4 eV. Due to the<br />
significant width of the emitted electron spectrum one can think about<br />
a distribution of excited defect electrons in the electron emitting metal<br />
surface. This kind of electronic excitation is difficult to detect in a bulk<br />
metal. In a 15 nm thick silver film however the defect electrons may reach<br />
the opposite interface of the metal film. In a multilayer tunnel system,<br />
separating the thin silver film from an aluminium film by a 2 nm thick<br />
oxide spacer one can detect an electron current from the base electrode<br />
to the silver electrode which is exposed to the metastable beam. Competing<br />
processes with deexcitation are discussed. By the application of<br />
a grid filter in the transport tube between the discharge and the vacuum<br />
chamber one can seperate between ion neutralization reactions and<br />
metastable deexcitation. By an asymmetric chopping unit which allows<br />
the exposition of the samples to alternating particle-photon and photon<br />
fluxes we discuss the contribution of the photon induced tunnel current<br />
to the total tunnel current.<br />
O 31.3 Do 11:45 H36<br />
Molecular scattering and adsorption at metallic surfaces studied<br />
by ab initio molecular dynamics simulations — •Axel Groß —<br />
Physik-Department T30, Technische Universität München, 85747 Garching<br />
Molecular dynamics simulations based on density functional theory<br />
(DFT) calculations have been performed to study the interaction of simple<br />
molecules with metallic surfaces. In the simulations, the surface atoms<br />
have been treated dynamically thus allowing a realistic description of the<br />
energy transfer from the impinging molecules to the substrate. In particular,<br />
we focus on the systems O2/Pt(111) [1] and H2/Pd(100). The<br />
energy transfer and dissociation process of O2 which can adsorb both<br />
molecularly as well as dissociatively on Pt(111) is analysed in detail. In<br />
the simulation of H2 adsorption on metallic surfaces, the substrate atoms<br />
are usually kept fixed because of the large mass mismatch between H2<br />
and the metal atoms [2]. This approximation will be critically questioned<br />
by examining the influence of the recoil of the metal atoms on the H2<br />
adsorption dynamics.<br />
[1] A. Groß, A. Eichler, J. Hafner, M.J. Mehl, and D.A. Papaconstantopoulos,<br />
Surf. Sci. 539, L542 (2003).<br />
[2] A. Groß, Surf. Sci. Rep. 32, 291 (1998).<br />
O 31.4 Do 12:00 H36<br />
First-principles Investigation of Structural and Chemical<br />
Properties of Nanoporous Carbon — •Suljo Linic, Johan M.<br />
Carlsson, and Matthias Scheffler — Fritz-Haber-Institut der<br />
Max-Planck-Gesellschaft, Faradayweg 4-6, 14195 Berlin<br />
Production of styrene by dehydrogenation of ethylbenzene(ET) is one<br />
of the most important processes in chemical industry. Iron oxide is used<br />
as catalyst, but it has been observed that ET decomposes during an induction<br />
period leaving nanoporous carbon (NPC) on the oxide support.<br />
NPC are curved, defective, graphitic sheets and experiments have shown<br />
that such materials are active catalysts for oxidative dehydrogenation of<br />
ET.[1] Recently, it was therefore suggested that the actual catalyst under<br />
reaction conditions is NPC.[2] This motivates a theoretical study of<br />
NPC. Our results indicate on the one hand that flat and curved basal<br />
planes of graphitic sheets are chemically inert. Vacancies on the other<br />
hand leave dangling bonds and increase the density of state close to the<br />
Fermi level. This gives the vacancies a much higher reactivity, which is<br />
examplified by a large exothermal energy for dissociative adsorption of<br />
O2. We have then studied oxidation of the defects as function of pressure<br />
and temperature. The resulting oxygenated vacancies show interesting<br />
properties as active sites in the dehydrogenation process. [1] M. S. Kane<br />
et al., Ind. Eng. Chem. Res. 35, 3319 (1996). [2] G. Mestl et al., Angew.<br />
Chem. Int. Ed. 40, 2066 (2001).