Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Oberflächenphysik Freitag<br />
going from Co to Ir reflecting the spatial extension of the 3d, 4d and 5d<br />
orbitals. The observed trends are in good agreement with calculated d−f<br />
hybridization matrix elements and, consequently, d − f hybridization is<br />
governed by the spatial overlap of the respective orbitals.<br />
O 44.6 Fr 12:30 H38<br />
Characterisation of the chemical composition and electronic<br />
structure of LiCoO2 thin films using photoelectron<br />
spectroscopy — •Andreas Thissen, David Ensling, Javier<br />
Fernandez-Madrigal, and Wolfram Jaegermann — FB<br />
Materialwissenschaften-Oberflaechenforschung, TU Darmstadt,<br />
Petersenstr. 23, D-64287 Darmstadt<br />
LiCoO2 is used as cathode materials for Li intercalation batteries.<br />
Polycrystalline thin films have been prepared by magnetron sputtering<br />
in an UHV chamber connected to an analysis system. Chemical analysis<br />
using (S)XPS shows that a variation of the sputtering parameters<br />
strongly influences the stoichiometry of the films, leading to different Co<br />
oxidation states (2+, 3+, 4+). Depending on the chemical composition<br />
changes in the electronic structure have been studied by UPS, ResPES<br />
and XAS. The results are in good agreement with DFT band structure<br />
calculations reported in literature. From ResPES measurements the separation<br />
of the O2p- and Co3d-like valence band contributions was possible,<br />
giving the occupation numbers as well. It has been shown by AFM,<br />
REM, XRD, Raman spectroscopy and EXAFS, that also the morphology<br />
and crystal structure of the samples depends on preparation conditions.<br />
(Dis)charging experiments have been carried out in an in-situ battery<br />
device in order to perform XPS and UPS measurements of the cathode<br />
during battery operation. Changes in the electronic structure of the Li1xCoO2<br />
host can clearly be correlated to the charging state of the battery.<br />
O 44.7 Fr 12:45 H38<br />
Second Harmonic Generation on NiO — •Georgios Lefkidis,<br />
Khompat Satitkovitchai, and Wolfgang Hübner — TU Kaiserslautern,<br />
PO Box 3409, D-67653, Germany<br />
The second order susceptibility tensors, which are important for Optical<br />
Second Harmonic Generation (SHG) are studied for NiO starting<br />
from ab-initio calculations. To represent the (001) surface of the rock-<br />
salt NiO lattice we embed a NiO −8<br />
5 cluster in a charge point field which<br />
accounts for the Madelung potential due to the neighboring ions. Sim-<br />
O 45 Zeitaufgelöste Spektroskopie II<br />
ilarly, an embedded NiO −10<br />
6 cluster is used to represent the bulk. The<br />
quantum chemical calculation is performed at various levels, where the<br />
effect of the basis set is studied, and the energy correction due to electron<br />
correlations. A Complete Active Space Configuration Interaction is<br />
performed, while the excited states are studied with Single Excitation<br />
Configuration Interaction (CIS) with energy contribution from double<br />
and triple excitations. The electric and magnetic dipole transitions are<br />
used to calculate the χ (2ω)<br />
eee and χ (2ω)<br />
mee tensors.<br />
While inversion symmetry of the bcc lattice leads to zero tensor elements<br />
for the bulk, the breaking of the symmetry on the surface gives<br />
non-zero elements within the electric-dipole approximation. On the other<br />
hand some χ (2ω)<br />
mee elements exist for both bulk and surface. The effect of<br />
spin-orbit coupling on both tensors is discussed.<br />
O 44.8 Fr 13:00 H38<br />
An X-ray absorption (NEXAFS) and resonant inelastic X-ray<br />
scattering (RIXS) study of liquid water and aqueous solutions<br />
— •O. Fuchs 1 , L. Weinhardt 1 , F. Maier 1 , C. Heske 1 , E. Umbach<br />
1 , Y. Zubavichus 2 , M. Grunze 2 , M. Odelius 3 , L.G.M. Pettersson<br />
3 , A. Nilsson 4 , J.D. Denlinger 5 , Z. Hussain 5 , and R. Follath<br />
6 — 1 Exp. Physik II, Uni Würzburg — 2 Angew. Physikal. Chemie,<br />
Uni Heidelberg — 3 Fysikum, Stockholm University — 4 Stanford Synchrotron<br />
Radiation Lab — 5 ALS, Berkeley — 6 BESSY, Berlin<br />
The electronic and geometric structure of liquids and, in particular, of<br />
water and aqueous solutions is currently strongly discussed and investigated.<br />
Until recently, most experimental results were obtained with neutron<br />
and hard X-ray scattering experiments. Recently, soft X-ray spectroscopic<br />
methods such as fluorescence-yield NEXAFS (near-edge X-ray<br />
absorption fine structure) and RIXS were applied and compared with<br />
theoretical DFT calculations and Car-Parinello molecular dynamics simulations.<br />
This combination yields complementary information especially<br />
about the dynamic hydrogen bond network and the molecular dynamics.<br />
A third-generation synchrotron, a highly efficient spectrometer for soft<br />
x-rays, and suitably designed wet cells are essential for RIXS experiments<br />
on solutions. This talk presents a new spectrometer design consisting of<br />
a spherical mirror and a plane variable line spacing grating for the sulfur<br />
L2,3, carbon K, nitrogen K, and oxygen K edges, dedicated to the study of<br />
biologically relevant molecules. Furthermore, RIXS and NEXAFS measurements<br />
for water, heavy water, NaOH solutions (pH 15), and various<br />
other aqueous solutions are discussed.<br />
Zeit: Freitag 11:15–13:00 Raum: H39<br />
O 45.1 Fr 11:15 H39<br />
Two-pulse correlation of femtosecond laser-induced diffusion of<br />
oxygen on Pt(111) — •K. Stépán, J. Güdde, and U. Höfer —<br />
Fachbereich Physik, Philipps-Universität Marburg, D-35032 Marburg<br />
We have studied the mechanism of oxygen diffusion on Pt(111) induced<br />
by femtosecond laser pulses. The dissociative adsorption of O2 on a vicinal<br />
surface was used to selectively decorate the step sites with atomic<br />
oxygen [1]. Diffusion from the step edges onto the terraces was induced<br />
at a substrate temperature of T = 80 K by 100-fs, 800-nm pump pulses<br />
with absorbed fluences of 8-16 mJ/cm 2 . It was monitored in situ with<br />
optical second-harmonic generation (SHG) by exploiting the sensitivity<br />
of SHG to surface symmetry. The diffusion mechanism was explored in<br />
the time domain by performing measurements of the diffusion efficiency<br />
as a function of the delay time between two cross-polarized pump pulses.<br />
The two-pulse correlation has a width of about 1 ps. This indicates a<br />
diffusion process induced by multiple excitations from the hot electron<br />
gas of the metal, similar to the meanwhile well-studied phenomenon of<br />
desorption induced by multiple electronic excitations (DIMET) [2].<br />
[1] P. Gambardella et al. Phys. Rev. Lett. 87, 056103 (2001)<br />
[2] J. A. Misewich et al. Phys. Rev. Lett. 68, 3737 (1992)<br />
O 45.2 Fr 11:30 H39<br />
Electron Dynamics of C6F6/Cu(111) studied by time-resolved<br />
photoelectron and resonant Auger-Raman spectroscopy —<br />
•Patrick Kirchmann 1 , Panagiotis Loukakos 1 , Uwe Bovensiepen<br />
1 , Martin Wolf 1 , Vijayalakshmi Sethuraman 2 , Franz<br />
Hennies 2 , Alexander Föhlisch 2 und Wilfried Wurth 2 — 1 Freie<br />
Universität Berlin, Fachbereich Physik, Arnimallee 14, 14195 Berlin<br />
— 2 Universität Hamburg, Institut für Experimentalphysik, Luruper<br />
Chaussee 149, 22761 Hamburg<br />
Ultrafast charge transfer times in molecular resonances at metal substrates<br />
can be obtained in the frequency domain by the ”atomic-clock”<br />
method, i.e. where the ratio between ”Raman” type and ”Auger” type<br />
decay channels of a resonant core hole excitation is evaluated [1]. On<br />
the other hand, the temporal evolution of the population of photoinjected<br />
electrons into an adsorbate resonance by a femtosecond laser pulse<br />
can be probed directly in the time-domain by two-photon-photoemission<br />
(2PPE)[2]. To compare these two approaches quantitatively, we performed<br />
systematic experiments on C6F6/Cu(111) employing resonant X-ray<br />
photoelectron spectroscopy at BESSY II and time-resolved 2PPE using<br />
sub 30 fs laser pulses in the laboratory. Respective procedures of data<br />
analysis and coverage dependent electron lifetimes will presented.<br />
[1] W. Wurth and D. Menzel, Chem. Phys. 251, 141 (2000).<br />
[2] C. Gahl, K. Ishioka, Q. Zhong, A. Hotzel, and M. Wolf; Faraday<br />
Discussion 117, 191 (2000).