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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Deutsche <strong>Physik</strong>alische Gesellschaft e. V. (<strong>DPG</strong>)<br />

WWW-Server für Frühjahrstagungen und E-Verhandlungen<br />

Programm und Abstracts <strong>de</strong>r <strong>Sitzung</strong> O <strong>28</strong><br />

Postersitzung (Elektronische Struktur, Grenzfläche fest-flüssig,<br />

Halbleiteroberflächen und -grenzflächen, Magnetismus und Symposium<br />

SYXM, Methodisches, <strong>Nano</strong>strukturen, Oberflächenreaktionen, Teilchen<br />

und Cluster, Zeitaufgelöste Spektroskopie)<br />

Mi 16:00-19:00<br />

Bereich C<br />

O <strong>28</strong>.1 Poster Mi 16:00 Bereich C<br />

Bulk and surface sensitive photoemission on 1T-TiS 2<br />

•M. Garbrecht, O. Seifarth, M. Skibowski und L. Kipp<br />

Institut für Experimentelle und Angewandte <strong>Physik</strong>, Universität Kiel, D-24098 Kiel, Germany<br />

The bulk and surface sensitive electronic structure of the layered transition metal dichalcogeni<strong>de</strong> 1T-TiS 2 is<br />

investigated by means of angle resolved photoemission spectroscopy with VUV and XUV photons. At photon<br />

energies around 50 eV where ARPES is extremely surface sensitive we observe a semiconducting band<br />

structure. This is contrasted by more bulk sensitive photoemission data obtained at 150 eV where a semimetallic<br />

behavior is found. The results are discussed in the context of recent band structure calculations performed<br />

within the <strong>de</strong>nsity functional theory. The experiments have been performed with the ASPHERE spectrometer at<br />

the HASYLAB beamlines W3.2 and BW3. Work supported by the BMBF project no. 05 KS1 FKB and DFG<br />

Forschergruppe FOR 353<br />

O <strong>28</strong>.2 Poster Mi 16:00 Bereich C<br />

Excited state UPS of C 60<br />

•Arne Rosenfeldt, Klaus Finsterbusch und Helmut Zacharias<br />

AG Zacharias, <strong>Physik</strong>alisches Institut, Westfälische Wilhelms-Universität<br />

A 200 layer C 60 film is prepard by growth on an annealed C 60 monolayer on Cu(111). This system is pumped<br />

with tunable 351 to 415 nm radiation of 100 ps pulse duration and probed with <strong>de</strong>layed 263, 211 and 150 nm<br />

photons. Using the time-of-flight technique photo-electrons are observed from LUMO+1, LUMO, and singlet<br />

exciton states. The excitation probability of these states as a function of photon energy is measured. A<br />

maximum is found for<br />

h ν = 3.16 eV ( λ ∼ 392 nm). Further, the electron dynamic is analyzed and will be discussed.<br />

O <strong>28</strong>.3 Poster Mi 16:00 Bereich C<br />

Geometric and electronic structure of epitaxial PbS on HfS 2<br />

•J. Iwicki, A. Kamenz, O. Seifarth, S. Habouti, M. Kalläne und L. Kipp<br />

Institut für Experimentelle und Angewandte <strong>Physik</strong>, Universität Kiel, D-24098 Kiel, Germany<br />

1 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Misfit layer compounds like (PbS)NbS 2 form a special class of layered heterostructures. Due to 4-fold<br />

symmetries of the PbS layers which contrast the 6-fold symmetry of the NbS 2 layers a misfit is constituted. Up<br />

to now, bulk crystals of misfit compounds could only be grown with metallic hexagonal layers like e.g. NbS 2 or<br />

TiS 2 . Here we show first steps of epitaxial growth of PbS on semiconducting HfS 2 with corresponding STM<br />

images and angle resolved photoemission spectra for different coverages of PbS on HfS 2 . The photoemission<br />

results are compared with data of clean HfS 2 and PbS bulk crystals. The experiments have been performed with<br />

the ASPHERE spectrometer at HASYLAB.<br />

Work supported by the BMBF proj. 05 KS1 FKB and DFG Forschergruppe FOR 353<br />

O <strong>28</strong>.4 Poster Mi 16:00 Bereich C<br />

High energy conduction band states in layered materials<br />

•M. Marczynski, K. Rossnagel, M. Kalläne, E. E. Krasovskii, M. Skibowski, W. Schattke und L. Kipp<br />

Institut für Experimentelle und Angewandte <strong>Physik</strong>, Universität Kiel, D-24098 Kiel, Germany<br />

Employing angle resolved photoemission in the constant initial state mo<strong>de</strong> we investigate the conduction band<br />

states of layered materials up to about 100 eV above the Fermi level. The layered materials HfS 2 and TiTe 2<br />

serve as mo<strong>de</strong>l systems showing distinct features even for higher conduction bands. The experimentally<br />

observed structures are discussed in the context of theoretical results obtained by ab initio calculations. In<br />

particular, photoemission final states are treated within ELAPW based scattering theory.<br />

The experiments have been performed at HASYLAB (BW3 beamline) and the Advanced Light Source (beamline<br />

7).<br />

Work supported by the BMBF project no. 05 KS1 FKB and DFG Forschergruppe FOR 353.<br />

O <strong>28</strong>.5 Poster Mi 16:00 Bereich C<br />

Angle resolved measurement of the (1p) -1 photoemission cross section of CO adsorbed on Pt(111)<br />

•Sebastian Wegner, Grigorios Tsilimis, Jörg Kutzner und Helmut Zacharias<br />

<strong>Physik</strong>alisches Institut, Westfälische Wilhelms Universität Münster, Wilhelm-Klemm-Straße 10, D-48149<br />

Münster<br />

High or<strong>de</strong>r harmonic radiation is generated by focussing femtosecond Ti:sapphire pulses into a noble gas. The<br />

pulsed radiation is tunable in the range of 20-110 eV in steps of 3.1 eV. At an energy of 32.4 eV we measured<br />

the CO(1π) -1 photoemission of the c(4×2)-2CO/Pt(111) surface. In contrast to experiments on oriented<br />

molecules in the gas phase we observe emission parallel as well as perpendicular to the axes of the adsorbed<br />

CO. We fitted the angular distribution by Legendre polynomials P l (cosθ). It is best fitted by l = 3 and l = 4<br />

polynomials indicating a large contribution of d and f partial waves.<br />

O <strong>28</strong>.6 Poster Mi 16:00 Bereich C<br />

Fermi-Surface-Mapping an Übergangsmetallen<br />

•M. Krause, S. Dreiner, M. Schürmann, U. Berges und C. Westphal<br />

Universität Dortmund, Experimentelle <strong>Physik</strong> I, 44221 Dortmund<br />

Die Kenntnis <strong>de</strong>r elektronischen Struktur von Metallen ist grundlegend für das Verständnis vieler physikalischer<br />

Phänomene. Die elektronischen Zustän<strong>de</strong> an <strong>de</strong>r Fermikante bedingen z.B. die elektrische Leitfähigkeit, die<br />

Temperaturabhängigkeit <strong>de</strong>s Ferromagnetismus, die Supraleitung und die Hochtemperatursupraleitung. Durch<br />

Aufnahme winkelaufgelöster Photoemissionsspektren über <strong>de</strong>m Halbraum <strong>de</strong>r Probe mit HeI Strahlung wur<strong>de</strong>n<br />

Schnitte durch die Fermiflächen gemessen. Zur Interpretation wur<strong>de</strong>n Vergleichsrechnungen <strong>de</strong>r<br />

Dichtefunktionaltheorie (LKKR) durchgeführt.<br />

Die Meßergebnisse für Cu, Ni, Pd und Rh wer<strong>de</strong>n gezeigt und mit <strong>de</strong>n jeweiligen Rechnungen verglichen. Diese<br />

2 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Ergebnisse bil<strong>de</strong>n die Grundlage für zukünftige Experimente.<br />

O <strong>28</strong>.7 Poster Mi 16:00 Bereich C<br />

Surface state as local sensor for single magnetic impurities<br />

•Daniel Wegner, Andreas Bauer und Günter Kaindl<br />

Freie Universität Berlin, Institut für Experimentalphysik, Arnimallee 14, 14195 Berlin-Dahlem<br />

The (0001)-surface of Lu metal exhibits a highly localized surface state directly at the Fermi energy, E F [1]. It<br />

appears as a sharp peak in the tunnelling spectra measured by low-temperature scanning tunnelling<br />

spectroscopy (STS) at 10 K. We have used this surface-state peak as a sensor for single magnetic impurities of<br />

Gd and Ho atoms embed<strong>de</strong>d in the film surface. Within a radius of about 15 Å around such an impurity, the<br />

surface-state appears as a double-peaked structure in the tunnelling spectra with a narrow dip in between; this<br />

dip is only a few meV wi<strong>de</strong> and is located within less than 1 meV at E F . The results are discussed on the basis<br />

of the Kondo effect.<br />

This work was supported by the DFG, Sfb-290.<br />

[1] A. Bauer, A. Mühlig, D. Wegner, and G. Kaindl, Phys. Rev. B 65, 75421 (2002).<br />

O <strong>28</strong>.8 Poster Mi 16:00 Bereich C<br />

Correlation of electronic transport and structural properties of Cs layers on Si(001)<br />

•Hong Liu, A.A. Shklyaev, V. Zielasek und H. Pfnür<br />

Universität Hannover, Institut für Festkörperphysik, Appelstr. 2, 30167 Hannover<br />

Combining LEED, EELS, and conductivity measurements we have studied the correlation of electronic transport<br />

with structural properties of Cs layers on Si(001). Depending on the substrate temperature T during Cs<br />

<strong>de</strong>position we find three different growth regimes. Only for T < 160 K we observe the growth of a continuous<br />

metallic Cs film consisting of three-dimensional islands on top of the first 2 monolayers. Between 170 K and<br />

room temperature a pseudomorphic wetting layer forms with a saturation coverage of 1-1.5 ML.<br />

For Cs <strong>de</strong>position at around 160 K we observe discontinuities of the surface conductivity at 0.5, 1, and 1.5<br />

monolayer coverage, respectively. Those at 0.5 and 1 ML can be associated with transitions of the surface<br />

reconstruction from 3 × 4 to 3 × 2 and 3 × 2 to 2 × 1, respectively. Based on EELS data, electrical phase<br />

transitions (metal - semiconductor - metal) in the submonolayer coverage range have been reported by others<br />

[1]. While according to EELS the wetting layer should be metallic, conductivity measurements show that the<br />

electrical transport in the layer is activated. Refined mo<strong>de</strong>ls of the surface structure will be presented.<br />

[1] Ki-Dong Lee and Jinwook Chung, Phys. Rev. B 55 (1997) 12906.<br />

O <strong>28</strong>.9 Poster Mi 16:00 Bereich C<br />

STM-Simulation <strong>de</strong>r Selbstassemblierung von A<strong>de</strong>nin auf Graphit in Abhängigkeit <strong>de</strong>r Scanrichtung<br />

•Thomas Markert 1 , Thomas Markert 1 , Ferdinand Jamitzky 2 , Frank Trixler 3 , Axel Groß 1 , Wolfgang Heckl 3 ,<br />

Ferdinand Jam itzky 2 , Frank Trixler 3 und Axel Groß 1<br />

1 <strong>Physik</strong>-Department, TU München, D-85747 Garching<br />

2 MPI für extraterrestrische <strong>Physik</strong>, D-85740 Garching<br />

3 Department für Geo- und Umweltwissenschaften, LMU München, D-80333 München<br />

STM-Bil<strong>de</strong>r von Molekülnetzwerken, die über Wasserstoff-Brückenbindungen stabilisiert sind, zeigen i.a. eine<br />

<strong>de</strong>utliche Abhängigkeit von <strong>de</strong>r Scanrichtung, da kleine Verschiebungen <strong>de</strong>r Moleküle, die während <strong>de</strong>s<br />

Scanvorgangs durch die Spitze verursacht wer<strong>de</strong>n, abhängig von <strong>de</strong>r Orientierung <strong>de</strong>r<br />

3 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Wasserstoff-Brückenbindungen sind. Bei gleicher Auslenkung sind die Rückstellkräfte parallel zur<br />

Wasserstoff-Brückenbindung größer als senkrecht zu ihr. Mit Hilfe von LDOS-Bil<strong>de</strong>rn, die aus<br />

DFT-Rechnungen erstellt wur<strong>de</strong>n, wird am Beispiel <strong>de</strong>r Selbstassemblierung von A<strong>de</strong>nin auf Graphit versucht<br />

die experimentell gewonnenen Bil<strong>de</strong>r einer Drehserie zu simulieren.<br />

O <strong>28</strong>.10 Poster Mi 16:00 Bereich C<br />

Elctronic structure of MgSO 4 crystals<br />

•V.V. Maslyuk 1,2 , C. Tegenkamp 1 , T. Bredow 3 und H. Pfnür 1<br />

1 Institut für Festkörperphysik, Appelstr.2 D-30167 Hannover, Germany<br />

2 Uzhhorod National University, Pidgirna St.2 88000 Uzhhorod, Ukraine<br />

3 Institut für Theoretische Chemie, Am Kleinen Fel<strong>de</strong> 30 D-30167 Hannover, Germany<br />

Typically, the crystallographic structures of minerals are quite well investigated, but there is not much<br />

knowledge about their electronic structures. As one candidate of an insulator consisting chemically of more than<br />

two different elements, we investigated the crystallographic and electronic structure of MgSO 4 and kieserite<br />

(MgSO 4 ·H 2 O), respectively. Starting with kieserite with 36 atoms per unit cell, we <strong>de</strong>termined the electronic<br />

structure by ab-initio calculations. Using CRYSTAL03 the lattice parameters were calculated within an accuracy<br />

better than 0.01 Å by choosing basis sets for magnesium and oxygen taken from MgO and for sulfur taken<br />

from CaSO 4 including also d-orbitals. In or<strong>de</strong>r to calculate the band gap of kieserite, the method of hybrid<br />

mixing of Hartree-Fock and DFT hamiltonians was used. The band gap at the Γ-point was <strong>de</strong>temined to be 7.4<br />

eV. To support the theoretical calculations, first photoelectron- and electron energy loss spectroscopy<br />

experiments have been performed. Thereby, bulk kieserite crystals have been used. Obviously, the effect of<br />

surface relaxation effects and <strong>de</strong>fects are small, because the measured band gap agrees quite well with the<br />

theoretical findings. Nevertheless, our calculations will be further refined.<br />

O <strong>28</strong>.11 Poster Mi 16:00 Bereich C<br />

Valence band photoemission spectroscopy of chemically disor<strong>de</strong>red ultrathin Ni x Pd 1-x films on<br />

Cu 3 Au(100)<br />

•Frank Matthes 1 , Liu-Niu Tong 1 , Alexej Rzhevskii 2 und C.M. Schnei<strong>de</strong>r 2<br />

1 Leibniz Institut für Festkörper- und Werkstoffforschung Dres<strong>de</strong>n, PF 27 01 16, D-01171 Dres<strong>de</strong>n<br />

2 Institut für Elektronische Eigenschaften, Forschungszentrum Jülich, 52425 Jülich<br />

We have studied the valence band structure of ultrathin Ni x Pd 1-x alloys on a single crystalline Cu3Au(100)<br />

substrate. Ni and Pd are isoelectronic, but while Ni is ferromagnetic with an average exchange splitting of 0.3<br />

eV along the ∆ direction, Pd exhibits a higher spin orbit coupling (band splitting 0.3 eV). Via the alloy<br />

concentration one can conveniently vary the relative weight of these two spin-<strong>de</strong>pen<strong>de</strong>nt interactions with<br />

profound effects for the electronic structure. We will present first results of our high-resolution photoemission<br />

measurements for 15 monolayer thick Ni x Pd 1-x films with different compositions. The measurements were<br />

performed along the ∆ direction for excitation energies from 16 eV to 40 eV. As a main spectral feature, we<br />

observed contributions from bands originating from 3d Ni and 4d Pd electrons near the Fermi energy. This<br />

feature only disperses weakly with the excitation energy. Starting with pure Ni films, we observed a broa<strong>de</strong>ning<br />

of the spectra while increasing the Pd concentration up to 30%. This may be caused by the chemically induced<br />

disor<strong>de</strong>r. To distinguish the spin <strong>de</strong>pen<strong>de</strong>nt contributions and thus arrive a more <strong>de</strong>tailed interpretation of the<br />

photoemission data, we performed for three different Ni rich alloy compositions also spin-resolved<br />

photoemission experiments.<br />

O <strong>28</strong>.12 Poster Mi 16:00 Bereich C<br />

Site-specific Valence-electronic Structure of SrTiO 3 by X-ray Standing Waves and XPS<br />

4 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

•Sebastian Thiess 1 , Tien-Lin Lee 1 , Bruce C. C. Cowie 1 , Joe C. Woicik 2 und Jörg Zegenhagen 1<br />

1 ESRF, Grenoble, France<br />

2 NIST, Gaithersburg, USA<br />

We used the x-ray standing waves (XSW) technique and x-ray photoelectron spectroscopy (XPS) to <strong>de</strong>termine<br />

the contribution of the constituent elements Sr, Ti and O of a SrTiO 3 (STO) crystal to the STO valence band,<br />

thus <strong>de</strong>riving their partial <strong>de</strong>nsity of states.<br />

Lattice site-specific electronic information - which is not available from standard XPS - is obtained by utilising<br />

the spatial intensity modulation of an x-ray standing wave (XSW) interference field, generated by the coherent<br />

superposition of an inci<strong>de</strong>nt and a Bragg-reflected x-ray beam. By proper positioning the antino<strong>de</strong>s of the XSW<br />

within the STO unit cell, photoemission from specific lattice sites can be preferentially excited and their valence<br />

electronic contribution i<strong>de</strong>ntified.<br />

XSW fields were generated by the STO(111) and STO(112) reflections at photon energies of 2.7 and 3.9 keV.<br />

XSW modulated, high-resolution core and valence-electron emission spectra were recor<strong>de</strong>d from an in-situ<br />

UHV annealed STO single crystal at beamline ID32 at the ESRF.<br />

O <strong>28</strong>.13 Poster Mi 16:00 Bereich C<br />

Mechanisms and capability of Steam Laser Cleaning<br />

•F. Lang 1 , M. Mosbacher 1 , S. Georgiou 2 und P. Lei<strong>de</strong>rer 1<br />

1 University of Konstanz, Fach M676, 78457 Konstanz, Germany<br />

2 FORTH - IESL, P.O. Box 1527, 71110 Heraklion, Greece<br />

Steam Laser Cleaning is a powerful approach to remove submicron particles from surfaces. In the first step a<br />

liquid is applied onto the contaminated surface. Afterwards a laser pulse heats part of the fluid to a superheated<br />

state resulting in bubble nucleation and growth. Thereby strong forces are exerted on the contaminants, which<br />

are able to overcome the adhesion of the particles to the surface.<br />

Our measurements covering a broad range of particle sizes <strong>de</strong>monstrated the existence of a universal cleaning<br />

threshold for the laser fluence. In addition the influence of different liquid layer thicknesses was explored.<br />

Investigations of the surfaces after cleaning verified for the first time that damage free removal can be achieved,<br />

if the experimental parameters are chosen properly. Moreover fundamental studies of the bubble nucleation and<br />

growth in the superheated liquid were conducted to gain a more <strong>de</strong>tailed un<strong>de</strong>rstanding of the phase transition<br />

dynamics.<br />

O <strong>28</strong>.14 Poster Mi 16:00 Bereich C<br />

In-situ Vi<strong>de</strong>o-STM Untersuchung <strong>de</strong>r Dynamik von Sulfidadsorbaten auf Cu(100)-Elektro<strong>de</strong>n<br />

•Tunay Tansel und Olaf Magnussen<br />

Institut für Experimentelle und Angewandte <strong>Physik</strong> Christian-Albrechts-Universität Kiel<br />

Die Diffusion und Wechselwirkung von Adsorbaten an Elektro<strong>de</strong>noberflächen ist von großer Be<strong>de</strong>utung für das<br />

Verständnis <strong>de</strong>r elektrochemischen Phasengrenze. Solche dynamischen Prozesse wur<strong>de</strong>n hier am Beispiel von<br />

Sulfidadsorbaten (Be<strong>de</strong>ckungen 0,01 bis 0,03ML) auf Cu(100) in 0,01M HCl mittels elektrochemischer<br />

Hochgeschwindigkeits- Rastertunnelmikroskopie (Vi<strong>de</strong>o-STM) direkt auf <strong>de</strong>r atomaren Skala untersucht. Eine<br />

statistische Analyse <strong>de</strong>r Diffusion isolierter S ad ergab Sprungfrequenzen im Bereich von ? 2·10 -1 Hz. An <strong>de</strong>n<br />

Domänengrenzen c(2x2)-Phase ist die S ad Mobilität jedoch stark erhöht. Dies zeigt, dass die Gegenwart <strong>de</strong>s<br />

c(2x2)-Cl Koadsorbatgitters die effektive Diffusionsbarriere von S ad <strong>de</strong>utlich vergrößert. Weiterhin weisen die<br />

Beobachtungen auf attraktive S ad -S ad Wechselwirkungen und eine erhöhte Mobilität von Clustern an mehreren,<br />

benachbarten S ad hin.<br />

5 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

O <strong>28</strong>.15 Poster Mi 16:00 Bereich C<br />

In-situ-Vi<strong>de</strong>o-STM-Untersuchungen <strong>de</strong>s (1x1) ? ''hex'' - Phasenüberganges an<br />

Au(100)-Elektro<strong>de</strong>noberflächen<br />

•Klaus Krug 1 , Miguel Labayen 1 , Claudia Ramirez 2 , Wolfgang Schattke 2 und Olaf Magnussen 1<br />

1 Institut für Experimentelle und Angewandte <strong>Physik</strong> Christian-Albrechts-Universität zu Kiel<br />

2 Institut für Theoretische <strong>Physik</strong> und Astrophysik Christian-Albrechts-Universität zu Kiel<br />

Die Dynamik <strong>de</strong>s elektrochemisch induzierten (1x1) ? ''hex'' Übergangs an Au(100)-Elektro<strong>de</strong>n wur<strong>de</strong> in 0.01 M<br />

Na2SO4 + 1 mM HCl mittels in-situ Vi<strong>de</strong>o-STM untersucht. Der Phasenübergang erfolgt über Nukleation und<br />

Wachstum elementarer Einheiten <strong>de</strong>r Oberflächenrekonstruktion, 5 Atomreihen breiten, hexagonal geordneten<br />

Streifen in <strong>de</strong>r obersten Atomlage. Wachstum, kollektive Bewegung und Wechselwirkung <strong>de</strong>r Streifen konnten<br />

mit hoher Zeitauflösung als Funktion von Potential und Temperatur beobachtet wer<strong>de</strong>n. Diese Beobachtungen<br />

weisen unter an<strong>de</strong>rem auf einen schnellen eindimensionalen Massentransport von Goldatomen entlang <strong>de</strong>r<br />

Streifen hin, <strong>de</strong>r sowohl über Verzerrungen im Streifen selbst als auch über Adatome auf <strong>de</strong>m Streifen erfolgen<br />

kann. Diese Interpretation wird durch Dichtefunktionalrechnungen gestützt.<br />

O <strong>28</strong>.16 Poster Mi 16:00 Bereich C<br />

In-situ Vi<strong>de</strong>o-STM-Untersuchungen <strong>de</strong>r lateralen Bewegung von ''hex''-Streifen auf<br />

Au(100)-Elektro<strong>de</strong>noberflächen<br />

•Christian Haak, Miguel Labayen und Olaf Magnussen<br />

Institut für experimentelle und Angewandte <strong>Physik</strong>, Christian-Albrechts-Universität, Leibnizstraß e 19, 24118<br />

Kiel<br />

Die Dynamik von fünf Atomreihen breiten, hexagonal geordneten Streifen auf Au(100)-Oberflächen wur<strong>de</strong><br />

mittels Vi<strong>de</strong>o-STM in 0.01 M Na 2 SO 4 + 1 mM HCl untersucht. Diese Streifen existieren transient während <strong>de</strong>s<br />

potentialinduzierten Übergangs von <strong>de</strong>r Au(100) (1×1) zur ''hex'' rekonstruierten Oberfläche und weisen eine<br />

überraschend hohe Mobilität senkrecht zur Streifenrichtung auf (Sprungraten von ca. 40 s -1 ). Die Bewegung<br />

dieser nanoskaligen Streifen wur<strong>de</strong> mit automatischen Bil<strong>de</strong>rkennungsverfahren analysiert und statistisch<br />

ausgewertet. Dabei erhaltene Sprungverteilungsfunktionen weisen auf die Existenz zweier elementarer Prozesse<br />

hin (Sprünge um einen bzw. zwei Atomabstän<strong>de</strong>), welche simultan ablaufen. Diese Sprünge können über die<br />

Bewegung versetzungsähnlicher Verzerrungen in <strong>de</strong>n Streifen erklärt wer<strong>de</strong>n.<br />

O <strong>28</strong>.17 Poster Mi 16:00 Bereich C<br />

Copper sulfidation at the solid/liquid interface<br />

•A. Spänig, T. Mangen, P. Broekmann und K. Wan<strong>de</strong>lt<br />

Institut für <strong>Physik</strong>alische Chemie; Wegelerstr. 12; 53115 Bonn<br />

The initial stage of the sulfidation process of a Cu(100) electro<strong>de</strong> surface has been studied un<strong>de</strong>r<br />

electrochemical conditions by means of in-situ Scanning Tunneling Microscopy (STM). At negative electro<strong>de</strong><br />

potential sulfi<strong>de</strong> anions form a regular c(2 × 6) adsorbate layer which transforms irreversibly into<br />

two-dimensional copper sulfi<strong>de</strong> phases at more positive potentials. Depending on the applied electro<strong>de</strong> potential<br />

different sulfi<strong>de</strong> induced reconstruction phases could be generated which can be seen as precursor phases for<br />

the formation of bulk copper sulfi<strong>de</strong>. The reconstruction process is accompanied by a massive mass transport<br />

out of the topmost copper layer pointing to a sulfi<strong>de</strong> induced expansion of the topmost substrate layer.<br />

O <strong>28</strong>.18 Poster Mi 16:00 Bereich C<br />

Katalytische und elektrochemische Oxidation von Ameisensäure auf einer Pd(111)-Elektro<strong>de</strong><br />

•Katrin Brandt, Marco Steinhausen, Thomas Schmidt und Klaus Wan<strong>de</strong>lt<br />

6 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Institut für <strong>Physik</strong>alische und Theoretische Chemie, Universität Bonn, 53115 Bonn<br />

Mit <strong>de</strong>m Ziel kleine, organische Moleküle als "Son<strong>de</strong>n" auf die Oberflächenreaktivität elektrokatalytisch aktiver,<br />

binärer Elektro<strong>de</strong>n einzusetzen, wer<strong>de</strong>n potentielle organische Säuren zunächst auf <strong>de</strong>n Oberflächen <strong>de</strong>r<br />

einzelnen Metallkomponenten untersucht.<br />

Dazu wur<strong>de</strong> das Reaktionsverhalten von Ameisensäure (HCOOH) bei Kontakt mit einer Pd(111)-Elektro<strong>de</strong> im<br />

UHV mittels TDS, UPS und IRRAS sowie in Lösung mit IRRAS untersucht.<br />

Die spektroskopische Charakterisierung <strong>de</strong>r chemisorbierten HCOOH im UHV zeigt die Desorption <strong>de</strong>s intakten<br />

Moleküls aus <strong>de</strong>r Multilage bei 160 K und in geringen Mengen aus <strong>de</strong>r Monolage bei 186 K. In <strong>de</strong>r Monolage<br />

überwiegt <strong>de</strong>r Zerfall zu CO 2 und H 2 . Zahlreiche Intermediate <strong>de</strong>s katalytischen Zerfalls können anhand ihrer<br />

IR-Absorptionsfrequenzen zwischen 1800 cm -1 und 1900 cm -1 nachgewiesen wer<strong>de</strong>n.<br />

In situ IR-Untersuchungen in reiner HCOOH zeigen sowohl die katalytische Freisetzung von CO 2 als auch die<br />

beschleunigte elektrochemische Oxidation ( > 0.4 V vs. NHE) <strong>de</strong>r Säure.<br />

O <strong>28</strong>.19 Poster Mi 16:00 Bereich C<br />

Ab-Initio-Investigation of Static and Magnetic Properties of Fe|GaAs(001)<br />

•Harald Dobler und Dieter Strauch<br />

Institut für Theoretische <strong>Physik</strong>, Universität Regensburg, 93040 Regensburg<br />

We <strong>de</strong>termine the structure and magnetic properties of the (001)-surface of GaAs covered by iron. Encouraged<br />

by our former investigations of the system Fe|ZnSe, where we have obtained dramatic <strong>de</strong>viations from the i<strong>de</strong>al<br />

structure as well as sensitivity of the magnetic properties to structural changes, we consi<strong>de</strong>r another example<br />

for the compound semiconductor. Again, the lattice constant of GaAs and the doubled value of α-Fe agree very<br />

well. Nevertheless, we find significant variations of the i<strong>de</strong>al behavior. We present our results for one, two,<br />

three, and four monolayers of iron. Similar to the case of Fe|ZnSe the effects are most interesting for a single<br />

monolayer. Therefore, we show the structures and the profiles of the <strong>de</strong>nsity of valence electrons and the<br />

magnetization in the direction perpendicular to the interface.<br />

The computations are carried out in the framework of spin polarized <strong>de</strong>nsity functional theory implemented in<br />

the program package VASP [1,2]. Further, we use expansion in plane waves, ultrasoft pseudopotentials, and<br />

generalized gradient corrections (GGA). The relaxations of the structures are realized using a conjugate-gradient<br />

method.<br />

[1] G. Kresse and J. Hafner, Phys. Rev. B 47, 558 (1993)<br />

[2] G. Kresse and J. Furthmüller, Phys. Rev. B 54, 11169 (1996)<br />

O <strong>28</strong>.20 Poster Mi 16:00 Bereich C<br />

Si(001) surface optical properties modified by organic functionalization and oxidation<br />

•Andreas Hermann, Frank Groth, Wolf G. Schmidt, Kaori Seino, Martin Preuss, Patrick H. Hahn und Friedhelm<br />

Bechstedt<br />

Institut für Festkörpertheorie und Theoretische Optik, Friedrich-Schiller-Universität, Max-Wien-Platz 1, 07743<br />

Jena, Germany<br />

Tremendous efforts have been <strong>de</strong>voted to investigate the optical properties of clean Si(001) surfaces. Their<br />

reflectance anisotropy spectra (RAS) are now well un<strong>de</strong>rstood in terms of <strong>de</strong>fects and transitions between<br />

surface states as well as surface-modified bulk wave functions [1]. Far less is known about the modifications<br />

of the surface optical response by chemical reactions. Inspired by recent experiments [2] we study numerically<br />

the influence of organic functionalization with phenanthrenequinone and layer-by-layer oxidation on the RAS<br />

spectrum of Si(001). The calculations are performed using the gradient-corrected <strong>de</strong>nsity functional theory<br />

(DFT-GGA) in conjunction with non-normconserving ultrasoft pseudopotentials and a plane-wave basis. The<br />

7 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

optical spectra are <strong>de</strong>termined in the in<strong>de</strong>pen<strong>de</strong>nt-particle approximation from all-electron wave functions<br />

obtained by the projector-augmented wave (PAW) method.<br />

[1] T. Yasuda et al., Phys. Rev. Lett. 74, 1995, 3431; R. Shioda, J. van <strong>de</strong>r Wei<strong>de</strong>, Phys. Rev. B 57, 1998,<br />

R6823; W.G. Schmidt, F. Bechstedt, J. Bernholc, Phys. Rev. B 2001, 63, 5322.<br />

[2] C.A. Hacker, R.J. Hamers, J. Phys. Chem. B 107, 2003, 7689; T. Yasuda et al., Phys. Rev. Lett. 87, 2001,<br />

037403.<br />

O <strong>28</strong>.21 Poster Mi 16:00 Bereich C<br />

Rauheit und Schädigung einer GaAs-Oberfläche nach <strong>de</strong>m chemisch unterstützten Ionenstrahlätzen<br />

mit Cl 2 /Ar +<br />

•Jens Dienelt, Klaus Zimmer, Justus von Sonntag und Bernd Rauschenbach<br />

Leibniz-Institut für Oberflächenmodifizierung (IOM), Permoserstr. 15, 04318 Leipzig<br />

Die chemische und die physikalische Abtragskomponente während <strong>de</strong>s chemisch unterstützten<br />

Ionenstrahlätzens (CAIBE) von GaAs mit Cl 2 /Ar + bewirkt sehr unterschiedliche Einflüsse auf die Rauheit und<br />

die Schädigung <strong>de</strong>s oberflächennahen Bereiches. Die Charakteristik <strong>de</strong>r Einzelprozesse spiegelt sich direkt in <strong>de</strong>r<br />

Oberflächenrauheit wie<strong>de</strong>r. Der starke chemische Ätzangriff von Chlorgas auf die GaAs-Oberfläche zeigt eine<br />

ausgeprägte Anisotropie <strong>de</strong>r Ätzprofilentwicklung, wobei die {111}-Ebenen durch <strong>de</strong>ren geringe Ätzrate <strong>de</strong>n<br />

Abtragsprozess maß geblich beeinflussen. Neben <strong>de</strong>r Temperatur o<strong>de</strong>r <strong>de</strong>m Chlordruck hat <strong>de</strong>mnach auch die<br />

Kristallorientierung einen großen Einfluss auf die Oberflächenrauheit. Beim reinen Zerstäubungsprozess ergeben<br />

sich aufgrund <strong>de</strong>r Impuls- und Energieübertragung <strong>de</strong>s gerichteten Ionenbeschusses die glattesten Oberflächen.<br />

Im Gegensatz zur geringen Oberflächenrauheit wird bei <strong>de</strong>r Zerstäubung <strong>de</strong>r oberflächennahe Bereich jedoch am<br />

stärksten geschädigt. Hierzu wer<strong>de</strong>n ortsaufgelöste Photolumineszenz-Untersuchungen an<br />

Mehrfach-Quantentrog-Strukturen aus Al 0,35 Ga 0,65 As/GaAs gezeigt, die unter Anwendung <strong>de</strong>r<br />

Schrägschlifftechnik präpariert wur<strong>de</strong>n.<br />

O <strong>28</strong>.22 Poster Mi 16:00 Bereich C<br />

Structural, electronic and spin properties of In nanowires on Si(111) surface<br />

•Xóchitl López 1,2 , Anna Krivosheeva 1 , Friedhelm Bechstedt 1 , Jürgen Furtmüller 1 und Andrey Stekolnikov 1<br />

1 Institut für Festkörpertheorie und Theoretische Optik, FSU Jena, Max-Wien-Platz 1, 07743 Jena<br />

2 Instituto <strong>de</strong> Física, Universidad Autónoma <strong>de</strong> Puebla, Apartado Postal J-48, Puebla 72570, México<br />

In the last years the electronic and structural properties of the indium-induced (4×1), (4×2) and (8×2) surface<br />

reconstructions on Si(111) have been intensively studied due to the potential applications on novel<br />

optoelectronics <strong>de</strong>vices. In this work the electronic structure calculations are performed using <strong>de</strong>nsity<br />

functional theory in the generalized-gradient approximation and ultrasoft pseudopotentials. The atomic positions<br />

were taken from a previous calculations [1], which are consistent with experimental data. The electronic band<br />

structures with and without spin polarization are calculated and discussed with respect to the metallic/insulating<br />

character of the chains. Because the spin <strong>de</strong>nsity distribution on these systems might be important for their<br />

electronic properties, we study the influence of the spin polarization on the atomic structure and electronic<br />

states of the In nanowires on Si(111). Several initial spin configurations are taken into account for all the<br />

surface reconstructions in or<strong>de</strong>r to observe a magnetic or<strong>de</strong>ring. We acknowledge the partial financial support<br />

from CONACyT grants No.36651-E and 36764-E. [1] F. Bechstedt et al., Phys Rev B 68, 1934XX (2003).<br />

O <strong>28</strong>.23 Poster Mi 16:00 Bereich C<br />

Ultrathin layers of Ag <strong>de</strong>posited on 4H-SiC(0001)<br />

•Serguei Soubatch und Ulrich Starke<br />

8 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Max-Planck-Institut für Festkörperforschung, Heisenbergstraße 1, 70569 Stuttgart<br />

Despite the significance of SiC for high-temperature and high-power electronic <strong>de</strong>vices based on<br />

metal/semiconductor interfaces, the initial stages of metal layer formation on SiC surfaces still remain<br />

insufficiently explored in comparison to well known metal/silicon heterointerfaces, such as Ag on Si. We<br />

investigated the <strong>de</strong>position of Ag on 4H-SiC(0001) using quantitative low-energy electron diffraction (LEED).<br />

Ag layers of 0.2, 0.5 and 1 ML coverage were <strong>de</strong>posited on the clean (3×3) and (?3×?3)R30 ? SiC(0001) surface<br />

phases. The structural <strong>de</strong>velopment after room temperature <strong>de</strong>position as well as after annealing was studied.<br />

The (3×3) phase is only marginally influenced by Ag <strong>de</strong>position at room temperature. Annealing leads to Ag<br />

diffusion and subsequent <strong>de</strong>sorption without a significant phase transformation. In case of the (?3×?3)R30 ?<br />

phase consi<strong>de</strong>rable changes can be monitored in the LEED intensities spectra immediately after <strong>de</strong>position. Here,<br />

structural changes are found during annealing also, possibly caused by Ag diffusion. In both cases the original<br />

surface phases reappear after Ag <strong>de</strong>sorption.<br />

O <strong>28</strong>.24 Poster Mi 16:00 Bereich C<br />

High temperature stable silici<strong>de</strong> contacts on the nanometer scale<br />

•G. Gardinowski, C. Tegenkamp, T. Block, S. Vagt, V. Zielasek und H. Pfnür<br />

Institut für Festkörperphysik, Universität Hannover, Appelstrasse 2, 30167 Hannover<br />

In or<strong>de</strong>r to characterize nanostructure electrically contacts are essential to build a bridge between the macrospic<br />

and the mesoscopic world. High temperature experiments with nanostructures on silicon substrates are<br />

particularly interesting, but require contacts which can withstand temperatures up to 1100 ? C without changes in<br />

their chemical composition and without interdiffusion at the contact area of the silici<strong>de</strong> and the silicon. Using<br />

electron beam lithography different silici<strong>de</strong> contacts on both Si(111) and Si(100) surfaces have been fabricated<br />

and tested. With regard to the specific formation temperatures for silici<strong>de</strong>s, mainly Mo, Ta and Ti have been<br />

tested. All three silici<strong>de</strong>s are stable up to at least 800 ? C. The metallic character of the silici<strong>de</strong>s was tested by<br />

masurements of the conductivity. However, for higher temperatures the <strong>de</strong>composition of MoSi 2 and TaSi 2 sets<br />

in leaving behind rough contact areas. Only the TiSi 2 silici<strong>de</strong> remains intact, as checked by µ-Auger<br />

spectroscopy. Furthermore, after optimization of the lithography parameters, TiSi 2 contact pads with separation<br />

lengths of 200 nm were fabricated successfully, i.e. after removing the native oxi<strong>de</strong> from the silicon surface<br />

(with pads) by a high temperature annealing step, perfect silicon was found in between the contacts as seen by<br />

STM/SEM. The edges of the contacts are rather sharp and well-<strong>de</strong>fined. The transition area was <strong>de</strong>termined to<br />

be around 1nm.<br />

O <strong>28</strong>.25 Poster Mi 16:00 Bereich C<br />

Direct evi<strong>de</strong>nce from FTIR for hydrogen incorporation into the MOCVD-grown P-rich reconstructed<br />

InP(100) surface<br />

•Tobias Letzig, H.J. Schimper, Thomas Hannappel und Frank Willig<br />

Hahn-Meitner-Institute, Glienicker Str. 100, 14109 Berlin, Germany<br />

Recently, the groups of Schmidt and Bechstedt have discussed several different surface reconstructions for<br />

InP(100). Three of those have been assigned to actually prepared surface reconstructions. In the case of<br />

MOCVD growth the P-rich (2x1/2x2) surface is postulated to contain hydrogen bonds that stabilize buckled P-P<br />

dimers. A P-rich surface with a different reconstruction is formed via MBE growth in the absence of hydrogen.<br />

The In-rich (2x4) reconstruction also does not contain any hydrogen atoms. We present here experimental<br />

support for the postulated hydrogen bonds on the surface of MOCVD grown P-rich (2x1/2x2) reconstructed<br />

InP(100) in the form of FTIR spectra that were measured in UHV. We ma<strong>de</strong> use of a patented contamination<br />

free transfer of the sample from the MOCVD reactor into a mobile UHV chamber. FTIR spectra will be<br />

presented for the as-grown surface and for the surface after further exposure to hydrogen and <strong>de</strong>uterium.<br />

O <strong>28</strong>.26 Poster Mi 16:00 Bereich C<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

RMS-roughness of Si from nm to mesoscopic scale<br />

•Stefan Schrö<strong>de</strong>r, Herbert Pfnür und Martin Henzler<br />

Institut für Festkörperphysik, Appelstr.2 D-30167 Hannover,Germany<br />

The International Technology Roadmap for Semiconductors (ITRS) <strong>de</strong>fines a <strong>de</strong>crease in surface roughness<br />

and an increase of the site planarity on a nm scale as two of the requirements for starting materials for industrial<br />

fabrication of next generations of silicon based micro- and nano<strong>de</strong>vices. The rms-roughness on different length<br />

scales is the principal property examined to verify the accomplishment of the goals set. We calculate Power<br />

Spectral Densities to examine the <strong>de</strong>cay of rms-roughness on the length scales open to STM-measurements (nm<br />

to µ m) and light scattering methods (µ m to mm) on standard wafers after annealing in a hydrogen<br />

environment. The light scattering method allows the <strong>de</strong>tection and counting of numbers of particles per area, as<br />

<strong>de</strong>man<strong>de</strong>d by the ITRS, to make sure that improved flatness is not accompanied by an increase in<br />

<strong>de</strong>fect-<strong>de</strong>nsity. In further experiments profiles of etched steps are monitored to <strong>de</strong>termine diffusion behaviour.<br />

We gratefully acknowledge financial support by Wacker Siltronic GmbH.<br />

O <strong>28</strong>.27 Poster Mi 16:00 Bereich C<br />

Photoelektronenbeugung an <strong>de</strong>r oxidierten 4H-SiC(0001) Oberfläche<br />

•M. Schürmann, S. Dreiner, U. Berges, M. Krause und C. Westphal<br />

Universität Dortmund, Experimentelle <strong>Physik</strong> I, 44221 Dortmund<br />

SiC ist ein Halbleitermaterial mit großer Bandlücke. Aufgrund seiner Eigenschaften ist es hervorragend geeignet<br />

zur Herstellung von Halbleiterbauelementen, die bei hohen Temperaturen, mit hohen Strömen und hohen<br />

Frequenzen betrieben wer<strong>de</strong>n können. In diesem Zusammenhang gewinnt auch die Kenntnis über die Struktur<br />

an <strong>de</strong>r SiO 2 /SiC-Grenzfläche an Be<strong>de</strong>utung. In einer Photoelektronenbeugungsuntersuchung wur<strong>de</strong>n<br />

Beugungsmuster an einer oxidierten 4H-SiC(0001) Oberfläche aufgenommen. Am U41-PGM Meßplatz bei<br />

BESSY II stand Synchrotonstrahlung mit hohem Photonenfluß und guter Energieauflösung zur Verfügung.<br />

Dadurch war es möglich die einzelnen, chemisch verschobenen Komponenten in <strong>de</strong>n XPS-Spektren aufzulösen<br />

und unterschiedliche Beugungsmuster aufgrund <strong>de</strong>r unterschiedlichen lokalen Umgebung <strong>de</strong>r Emitter zu<br />

erhalten. Ein Vergleich mit Simulationsrechnungen gibt Aufschluß über ihren Ursprung und die atomare Struktur<br />

in <strong>de</strong>r SiO 2 /SiC-Grenzfläche.<br />

O <strong>28</strong>.<strong>28</strong> Poster Mi 16:00 Bereich C<br />

Si2p-Photoemissionsspektroskopie an <strong>de</strong>r SiO 2 /Si(100)-Grenzfläche<br />

•S. Dreiner, M. Schürmann, M. Krause, U. Berges und C. Westphal<br />

Universität Dortmund, Experimentelle <strong>Physik</strong> I, 44221 Dortmund<br />

Die SiO 2 /Si Grenzfläche spielt eine wichtige Rolle in <strong>de</strong>r mo<strong>de</strong>rnen Halbleiterindustrie. Ein genaues Verständnis<br />

<strong>de</strong>r Grenzschichtstruktur kann zur Verbesserung <strong>de</strong>r Qualität von Halbleiterbauelementen beitragen.<br />

Die untersuchten SiO 2 /Si(100) Schichten mit einer Dicke von wenigen Ångström wur<strong>de</strong>n durch thermische<br />

Oxidation erzeugt. Mit Synchrotronstrahlung (BESSY II, U41 PGM) wur<strong>de</strong>n hochaufgelöste<br />

Si2p-Photoemissionsspektren über <strong>de</strong>m gesamten Halbraum bei einer Photonenenergie von hν = 180 eV<br />

aufgenommen. Diese Spektren ermöglichen durch Anpassungsroutinen die Trennung <strong>de</strong>r Si-Oxidationszustän<strong>de</strong><br />

(Si 1+ , Si 2+ , Si 3+ , Si 4+ ) vom Volumensignal (Si B ). Dabei zeigt sich, dass zwei weitere Komponenten (Si α , Si β )<br />

für eine verbesserte Anpassung nötig sind. Um <strong>de</strong>n Ursprung dieser Komponenten zu ermitteln wird die<br />

Winkelabhängigkeit dieser Signale analysiert. Dazu wer<strong>de</strong>n die gemessenen Photoelektronenbeugungsmuster mit<br />

Vielfachstreusimulationen verglichen.<br />

O <strong>28</strong>.29 Poster Mi 16:00 Bereich C<br />

Indium- und Indiumselenid-terminierte Si(111)-Oberflächen als neuartige Pufferschichten in <strong>de</strong>r<br />

Heteroepitaxie<br />

10 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

•Stefan Andres, Wolfram Calvet, Tilo Plake und Christian Pettenkofer<br />

Hahn-Meitner-Institut Berlin, Glienicker Strasse 100, 14109 Berlin<br />

Zur Passivierung von Silizium-Substraten für die Heteroepitaxie sind III-VI terminierte Oberflächen von grossem<br />

Interesse. Wir präsentieren erste Ergebnisse dünner In- bzw. InSe-Schichten auf Si(111). Die Präparation <strong>de</strong>r<br />

Proben erfolgte mittels Molekularstrahlepitaxie (MBE) auf H-Si(111)1x1-, Si(111)7x7- und <strong>de</strong>finiert<br />

nasschemisch oxidierten Si(111)-Substraten. Die Schichten wur<strong>de</strong>n in situ mittels Photoelektronenspektroskopie<br />

(PES), nie<strong>de</strong>renergetischer Elektronenbeugung (LEED) und Rastertunnelmikroskopie (STM) bezüglich ihrer<br />

Morphologie und elektronischen Struktur analysiert. Es wur<strong>de</strong> zunächst <strong>de</strong>r Einfluss von elementarem Indium<br />

auf Si(111) untersucht. Im weiteren Prozess erfolgte durch sukzessives Koverdampfen von In und Se die<br />

Herstellung einer InSe-terminierten 1x1-Oberfläche. Es zeigt sich, dass InSe in einer sogenannten Halblage<br />

aufwächst, wobei die In-Atome direkt an die Si-Oberfläche gebun<strong>de</strong>n sind. Eine Selenisierung <strong>de</strong>r Si-Oberfläche<br />

fin<strong>de</strong>t nicht statt. Die Energetik <strong>de</strong>r Grenzfläche wird bezüglich Bandversatz und Grenzflächendipolen bestimmt.<br />

O <strong>28</strong>.30 Poster Mi 16:00 Bereich C<br />

Electrospray Deposition of Sensitive Analytes<br />

•Frank Stadler 1 , Sergei Koltsov 2 , Eugenio Lune<strong>de</strong>i 1 , Giovanni Costantini 1 und Klaus Kern 1<br />

1 Max-Planck-Institut für Festörperforschung, D-70569 Stuttgart<br />

2 Institute for Analytical Instrumentation, Russian Aca<strong>de</strong>my of Sciences, 19813 Saint Petersburg<br />

Electrospray ionization is well-known as a means to solve the volatilization and ionization problem of sensitive<br />

analytes such as large biomolecules [1]. Recently Ouyang et al. [2] reported that electrosprayed protein ions<br />

remain intact, after ionization, in vacuo transfer, mass-selection and soft landing. We present a novel<br />

electrospray <strong>de</strong>position source, whose objective is the non-<strong>de</strong>structive <strong>de</strong>position of large sensitive (e.g. organic<br />

and biological) analytes un<strong>de</strong>r UHV conditions. Aim of this project is to overcome the limitations of size and<br />

mass of the <strong>de</strong>posited sample material that are intrinsic to the organic molecular beam epitaxy techniques based<br />

on sublimation. Besi<strong>de</strong>s the explanation of the un<strong>de</strong>rlying working principle of this novel experimental setup, the<br />

relevant technological aspects will be discussed. In addition, AFM images of electrosprayed metal colloid- and<br />

protein-containing analyte solutions (<strong>de</strong>posited on highly oriented pyrolytic graphite) will be presented.<br />

[1] J. B. Fenn et al., Science, 246 (1989), 64-71<br />

[2] Z. Ouyang et al., Science, 301 (2003), 1351-1354<br />

O <strong>28</strong>.31 Poster Mi 16:00 Bereich C<br />

VUV photon <strong>de</strong>tector with improved resolution for inverse photoemission<br />

•R. Stiepel, R. Ostendorf, C. Benesch, H. Merz und H. Zacharias<br />

<strong>Physik</strong>alisches Institut, Universität Münster, D-48149 Münster, Germany<br />

We have significantly improved the energy resolution of a VUV isochromat spectrometer for inverse<br />

photoemission. The <strong>de</strong>tector used is a Geiger-Müller counter with acetone as filling gas and a CaF 2 entrance<br />

window. With this <strong>de</strong>tector we achieve an optical energy resolution of 330 meV (FWHM) at a mean energy of<br />

9.9 eV for the optical bandpass. With an additional gas absorption filter arranged between two CaF 2 windows at<br />

the entrance of the counting tube we enhance the resolution to 90 meV (FWHM) at a slightly <strong>de</strong>creased mean<br />

energy of 9.8 eV. The higher resolution <strong>de</strong>creases the counting rate to approximately 20%, but by filling or<br />

evacuating the gas chamber we can switch between the two mo<strong>de</strong>s high resolution and high counting rate<br />

within seconds.<br />

O <strong>28</strong>.32 Poster Mi 16:00 Bereich C<br />

Konventionelle und positroneninduzierte Auger-Elektronenspektroskopie am System Kupfer-Gold<br />

11 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

•Benno Straßer, Christoph Hugenschmidt und Klaus Schreckenbach<br />

Technische Universität München, Lichtenbergstraße 1, D-85748 Garching<br />

Bei positroneninduzierter Auger-Elektronenspektroskopie (PAES) erfolgt die Anregung <strong>de</strong>r untersuchten Probe<br />

durch Annihilation von nie<strong>de</strong>renergetischen Positronen mit Rumpfelektronen <strong>de</strong>s Probenmaterials. Die Energie<br />

<strong>de</strong>r eingestrahlten Positronen kann dabei so klein gewählt wer<strong>de</strong>n, dass sie keinen<br />

Sekundärelektronen-Untergrund im Energiebereich <strong>de</strong>r Auger-Peaks erzeugen. PAES besitzt <strong>de</strong>shalb ein<br />

wesentlich besseres Signal-zu-Untergrund-Verhältnis als konventionelle AES und verfügt außer<strong>de</strong>m über eine<br />

höhere Oberflächensensitivität.<br />

Die an <strong>de</strong>r Technischen Universität München bestehen<strong>de</strong> PAES-Apparatur wur<strong>de</strong> mit einer Effusionszelle und<br />

einem Elektronenstrahlverdampfer zur Probenbeschichtung im Sub-Monolayer-Bereich erweitert. Daneben<br />

wur<strong>de</strong>n eine Argonkanone zur in situ Probenreinigung, eine Probenheizung sowie einen Probenschleuse<br />

installiert. Die Beschichtungsanlage wur<strong>de</strong> an mit Gold bedampften, polykristallinen Kupferproben getestet und<br />

Vergleichsmessungen zur Oberflächensensitivität von elektronen- und positroneninduzierter AES durchgeführt.<br />

O <strong>28</strong>.33 Poster Mi 16:00 Bereich C<br />

Focussing XUV photons with high contrast<br />

•J. Buck 1 , M. Kalläne 1 , S. Harm 1 , M. Skibowski 1 , R. L. Johnson 2 und L. Kipp 1<br />

1 Institut für Experimentelle und Angewandte <strong>Physik</strong>, Universität Kiel, D-24098 Kiel, Germany<br />

2 Institut für Experimentalphysik, Universität Hamburg, D-22761 Hamburg, Germany<br />

Photon sieves consisting of a large number of pinholes appropriately distributed over the Fresnel zones focus<br />

electromagnetic radiation [1]. As part of the program to <strong>de</strong>velop photon sieves for VUV FEL radiation [2] we<br />

present first experimental results on the focussing properties of reflective photon sieves, which allow to<br />

enhance the image contrast efficiently. The experiments have been performed with visible light (hν = 1.96 eV)<br />

and XUV radiation (hν = 100 eV) supplied from the BW3 beamline at HASYLAB.<br />

[1] L. Kipp, M. Skibowski, R.L. Johnson, R. Berndt, R. A<strong>de</strong>lung, S. Harm and R. Seemann, Nature 414, 184<br />

(2001)<br />

[2] A free-elecron laser (FEL) <strong>de</strong>livering transversal coherent radiation in the vacuum ultraviolet regime with<br />

photon energies up to several 100 eV is currently un<strong>de</strong>r construction at the Hamburg Synchrotron Radiation<br />

Laboratory HASYLAB/DESY. Work supported by the BMBF proj. 05 KS1 FK1<br />

O <strong>28</strong>.34 Poster Mi 16:00 Bereich C<br />

TOF-PEEM für zeitaufgelöste Mikrospektroskopie von Oberflächen basierend auf einer fs-Laser<br />

EUV-Lichtquelle<br />

•G. H. Fecher 1,2 , A. Oelsner 1 , G. Schönhense 1 , J. Kutzner 2 , G. Tsimilis 2 und H. Zacharias 2<br />

1 Johannes Gutenberg - Universität, 55099 Mainz<br />

2 Westfälische Wilhelms - Universität, 48149 Münster<br />

Die Kombination eines Photoemissions Elektronen Mikroskops (PEEM) mit einer Femtosekun<strong>de</strong>n Laser<br />

gepumpten EUV Lichtquelle wird präsentiert. Das PEEM ist für simultane Bildaufnahme und Flugzeitanalyse<br />

(TOF) mit einem 3D (x,y,t) Detektor ausgestattet. Dies erlaubt neuartige Anwendungen in <strong>de</strong>r<br />

Mikrospektroskopie von Oberflächen.<br />

Die Lichtpulse im extremen ultraviolett Bereich wer<strong>de</strong>n in E<strong>de</strong>lgasen durch ein 30fs Ti:Saphir Lasersystem<br />

generiert. Intensive IR Pulse erzeugen im Konversionsgas hohe Harmonische bis 120eV. Ein Toroidgitter wird<br />

zur Auswahl <strong>de</strong>r Harmonischen eingesetzt. Al-Filter und Au-Spiegel beschränkten <strong>de</strong>n Energiebereich auf<br />

15-72eV. Die herkömmliche Bil<strong>de</strong>inheit <strong>de</strong> PEEM wur<strong>de</strong> durch einen 3D-Delayline Detektor ersetzt. Dieser<br />

registriert die Elektronen in 2 räumlichen und einer zeitlichen Koordinate. Die rückwärtige Mikroskopsäule wird<br />

als Flugzeitstrecke betrieben. Die Zeitauflösung <strong>de</strong>s Detektors beträgt 125ps. Erste Ergebisse zeigen, daß <strong>de</strong>r<br />

12 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Bildkontrast empfindlich von <strong>de</strong>r ausgewählten Energie <strong>de</strong>r Elektronen abhängt. Die <strong>de</strong>rzeitige Begrenzung <strong>de</strong>r<br />

räumlichen (160nm) und zeitlichen Auflösung <strong>de</strong>r Metho<strong>de</strong> ist durch die Repetitionsrate (1kHz) <strong>de</strong>s anregen<strong>de</strong>n<br />

Lasers bedingt.<br />

O <strong>28</strong>.35 Poster Mi 16:00 Bereich C<br />

Growth of Platin <strong>Nano</strong>wire Networks on Nafion<br />

•M. Elbahri, J. Franc, O.C. Aktas, R. A<strong>de</strong>lung und F. Faupel<br />

Lehrstuhl für Materialverbun<strong>de</strong>, Technische Fakultät <strong>de</strong>r CAU Kiel<br />

The Nafion polymer, produced by the Dupont company, is still the most prominent membrane material for the<br />

commercial polymer electrolyte fuel cell (PMFC). Usually, the Nafion membrane is sandwiched by two catalytic<br />

layers, consisting of a metal-Nafion-carbon mixture in or<strong>de</strong>r to provi<strong>de</strong> catalytic activity as well as electrical and<br />

proton conductivity. It turns out that most of the Platinum doesn't contribute to the catalytic efficiency, which<br />

increases the total cost for the PMFC-fuel cell. An alternative approach might be a catalytic layer formed by a<br />

Pt-nanowire network. We present here a strategy to <strong>de</strong>posit Pt in the form of a nanowire networks. Therefore<br />

we used sputter <strong>de</strong>posited Pt on a vacuum <strong>de</strong>posited amorphous carbon mask layer. We show different<br />

Pt-nanowire networks generated on the Nafion surface and discuss the mechanisms that tune the network<br />

parameters like nanowire dimensions and mesh width.<br />

The authors thank the Technologiestiftung Schleswig-Holstein for supporting the project.<br />

O <strong>28</strong>.36 Poster Mi 16:00 Bereich C<br />

Imaging of optical near fields of nanostructures with fs laser pulses<br />

•Juliane Birk, Johannes Boneberg und Paul Lei<strong>de</strong>rer<br />

Universität Konstanz, FB <strong>Physik</strong>, LS Lei<strong>de</strong>rer, SFB 513, 78457 Konstanz<br />

The optical properties of nanostructures are a topic of interesting investigations. In analogy to the near fields<br />

around a Hertz dipole we expect near fields in the surrounding of all nanostructures. Up to now they were<br />

analysed with the scanning near field optical microscope (SNOM). We want to introduce an alternative method<br />

to image near fields with intensive short laser pulses. The intensity is adjusted to values where the substrate far<br />

from the particle is not affected. Nevertheless, the surface around and below the particle can be ablated, due to<br />

the local intensity enhancement in the optical near field. After the laser pulse the modified surface is imaged with<br />

atomic force microscopy (AFM) and thus the optical near fields of different nanostructures on several<br />

substrates, for example silicon, can be studied. A few examples of the near fields of various nanostructures are<br />

shown.<br />

O <strong>28</strong>.37 Poster Mi 16:00 Bereich C<br />

Infrared-optical properties of Cu nanoparticles on CaF 2 (111)<br />

•Birgit Gehring, Andreas Priebe und Annemarie Pucci<br />

Kirchhoff-Institut für <strong>Physik</strong>, Im Neuenheimer Feld 227, D - 69120 Hei<strong>de</strong>lberg<br />

Using IR spectroscopy the growth of Cu nanoparticles on UHV-cleaved CaF 2 (111) was investigated in situ.<br />

Relative transmission spectra informed about the dynamic conductivity of the nanoparticle film and about the<br />

influence of the substrate temperature on the percolation threshold.<br />

In the range from about 1000 cm -1 up to about 2500 cm -1 a relative transmission > 100 % was observed for Cu<br />

coverage below percolation, which corresponds to an anti-reflection effect. The magnitu<strong>de</strong> of this effect<br />

<strong>de</strong>pends on the growth temperature.<br />

For certain average Cu thicknesses we exposed CO at a sample temperature of about 100 K. The CO adsorption<br />

on different Cu facets was studied by IR transmission spectroscopy. The morphology of the nanoparticle layer<br />

13 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

was verified with atomic force microscopy (AFM) ex situ. From the AFM pictures the particle <strong>de</strong>nsity was<br />

estimated and the filling factor could be evaluated.<br />

O <strong>28</strong>.38 Poster Mi 16:00 Bereich C<br />

Steering host-guest interactions at surfaces using tailor-ma<strong>de</strong> two-dimensional nanoporous<br />

coordination systems<br />

•Sebastian Stepanow 1 , Magalí Lingenfel<strong>de</strong>r 1 , Alexandre Dmitriev 1 , Hannes Spillmann 1 , Erik Delvigne 2 , Nian<br />

Lin 1 , Xiaobin Deng 3 , Chengzhi Cai 3 , Johannes V. Barth 2 und Klaus Kern 1,2<br />

3 Department of Chemistry and Center for Materials Chemistry, University of Houston, Houston, TX<br />

77204-5003, USA<br />

1 Max-Planck-Institut für Festkörperforschung, Heisenbergstraße 1, D-70569 Stuttgart<br />

2 Institut <strong>de</strong> Physique <strong>de</strong>s <strong>Nano</strong>structures, Ecole Polytechnique Fédérale <strong>de</strong> Lausanne, CH-1015 Lausanne,<br />

Switzerland<br />

The so-called rational <strong>de</strong>sign principle, i.e., synthesis of materials with predictable structures and properties<br />

from appropriate organic molecular linkers connecting to metal no<strong>de</strong>s, has recently been explored to control<br />

pore size and functionality of open three-dimensional networks. Here we <strong>de</strong>monstrate the fabrication of<br />

surface-supported metal-organic coordination networks (MOCNs) comprising tailored pore sizes and chemical<br />

functionality by the modular assembly of polytopic organic carboxylate linker molecules and iron atoms on a<br />

Cu(100) surface un<strong>de</strong>r ultra-high vacuum conditions. The nanocavity arrays provi<strong>de</strong>d can be employed to host<br />

C 60 guest molecules. Temperature-controlled studies reveal at the single-molecule level how pore size and<br />

chemical functionality <strong>de</strong>termine the host-guest interactions.<br />

O <strong>28</strong>.39 Poster Mi 16:00 Bereich C<br />

Dynamic Mo<strong>de</strong> Force Microscopy Studies of Individual Single Wall <strong>Nano</strong>tubes on HOPG<br />

•Timo Behnke 1 , Makoto Ashino 1 , Alexan<strong>de</strong>r Schwarz 1 , Roland Wiesendanger 1 , Keith A. Williams 2 und Cees<br />

Dekker 2<br />

1 Institute of Applied Physics, University of Hamburg, Jungiusstrasse 11, D-20355 Hamburg, Germany<br />

2 Department of Applied Physics and DIMES, Delft University of Technology, Lorentzweg 1, 26<strong>28</strong> CJ Delft,<br />

The Netherlands<br />

The growing interest in single wall carbon nanotubes (SWNT) is related to their prospected applications of their<br />

unique possibilities in upcoming nanotechnology (1). To study structural properties of SWNTs down to the<br />

atomic scale dynamic mo<strong>de</strong> force microscopy is well suited.<br />

In a first step, we <strong>de</strong>veloped a technique to prepare SWNTs on HOPG. Tapping Mo<strong>de</strong> Imaging in ambient<br />

conditions showed a homogeneous SWNT distribution on atomically flat and well <strong>de</strong>fined graphite (HOPG) with<br />

only negligible small amounts of contamination. Although most of SWNTs appeared as bundles or ropes, we<br />

found a sufficient <strong>de</strong>nsity of individual SWNTs. In a second step, we took advantage of the increased resolution<br />

of dynamic mo<strong>de</strong> force microscopy and spectroscopy in ultrahigh vacuum and used a home-built low noise and<br />

very stable low-temperature force microscope to resolve the atomic structure of individual tubes.<br />

[1] Baughman, Zakhidov, <strong>de</strong> Heer, Science 296, 787 (2002)<br />

O <strong>28</strong>.40 Poster Mi 16:00 Bereich C<br />

Dynamik von selbstorganisierten <strong>Nano</strong>partikeln auf Oberflächen<br />

•Anton plech 1 , Vassilios Kotaidis 1 , Samuel Gr'esillion 2 und Gero von Plessen 3<br />

1 Fachbereich <strong>Physik</strong> <strong>de</strong>r Universität Konstanz, Universitätsstr. 10, 78457 Konstanz<br />

14 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

2 ESPCI 10, rue Vauquelin, F-75005 Paris<br />

3 RWTH Aachen, I. <strong>Physik</strong>alisches Institut A, D-52074 Aachen<br />

Naßchemisch hergestellte <strong>Nano</strong>partikel können über Selbstaggregationsverfahren auf Oberflächen abgelagert<br />

wer<strong>de</strong>n. Es wer<strong>de</strong>n so <strong>de</strong>finiert Submonolagenbe<strong>de</strong>ckungen erreicht. Diese Systeme erlauben das Studium <strong>de</strong>r<br />

strukturellen Eigenschaften von quasifreien Partikeln, wie thermische Expansion o<strong>de</strong>r strukturelle Dynamik.<br />

Es wer<strong>de</strong>n die strukturellen Relaxationen <strong>de</strong>r Partikel auf die ultraschnelle Laseranregung <strong>de</strong>r<br />

Plasmonenresonanz untersucht. Als Son<strong>de</strong> dient ultraschnelle zeitaufgelöste Röntgenbeugung (Meßplatz ID09,<br />

ESRF, Frankreich). Neben <strong>de</strong>r thermischen Anregung und Kühlung <strong>de</strong>s Kristallgitters wer<strong>de</strong>n auch<br />

Nichtgleichgewichtsprozesse beobachtet und im Rahmen von Partikeleigenschwingungen ge<strong>de</strong>utet.<br />

O <strong>28</strong>.41 Poster Mi 16:00 Bereich C<br />

Gold <strong>Nano</strong>teilchen auf Al 2 O 3 /Nb(110): Eine STM Studie dynamischer Umladungeffekte bei<br />

Raumtemperatur<br />

•Christof Dietrich, Berndt Koslowski und Paul Ziemann<br />

Abt. Festkörperphysik, Universität Ulm<br />

Um ein System zu präparieren, das Coulomb-Blocka<strong>de</strong> bei Raumtemperatur zeigt, wur<strong>de</strong>n epitaktische<br />

Niob(110)-Filme auf Saphir(0001) durch dc-magnetron-Sputtern bei einer Substrattemperatur von 1200K<br />

hergestellt. Diese Metallschichten haben eine extrem glatte Oberfläche (RMS:2nm auf 500nm 2 ) und mit <strong>de</strong>m<br />

STM konnte atomare Auflösung erzielt wer<strong>de</strong>n. Auf diese Schichten wur<strong>de</strong> eine 1nm dicke Aluminiumschicht<br />

aufgedampft und anschließ end in einem Sauerstoffplasma o<strong>de</strong>r in Sauerstoffatmosphäre oxidiert. Bei geeigneter<br />

Prozessführung kann auch ein epitaktisches Oxid hergestellt wer<strong>de</strong>n. Auf diese Tunnelbarriere wur<strong>de</strong>n Gold<br />

<strong>Nano</strong>teilchen mit Größ en von 1nm-15nm mittels einer mizellaren Technik aufgebracht.<br />

I-V-Spektroskopien auf <strong>de</strong>n Teilchen zeigen eine klare Coulomb-Blocka<strong>de</strong>, die sich sehr gut mit Hilfe <strong>de</strong>r "<br />

orthodoxen" Theorie <strong>de</strong>r Coulomb-Blocka<strong>de</strong> anpassen lassen. Durch Präparation verschie<strong>de</strong>ner Teilchengröß en<br />

konnten die Parameter <strong>de</strong>r Coulomb-Blocka<strong>de</strong> größ enabhängig bestimmt wer<strong>de</strong>n. Um die laterale Variation <strong>de</strong>r<br />

Parameter <strong>de</strong>r Coulomb-Blocka<strong>de</strong> auf <strong>de</strong>n Teilchen zu bestimmen, wur<strong>de</strong>n zusätzlich I-V-Karten angefertigt.<br />

Demnach sind die Parameter stark von <strong>de</strong>r Position auf <strong>de</strong>m Teichen abhängig.<br />

O <strong>28</strong>.42 Poster Mi 16:00 Bereich C<br />

Kombination mizellarer und lithographischer Techniken - ein unkonventioneller<br />

Strukturierungsansatz<br />

•Oliver Dubbers 1 , S. Fricker 1 , A. Klimmer 1 , H.-G. Boyen 1 , A. Plettl 1 , P. Ziemann 1 , M. Ott 2 und M. Möller 2<br />

1 Abt. Festkörperphysik, Universität Ulm, D-89069 Ulm<br />

2 Abt. Organische Chemie 3, Universität Ulm, D-89069 Ulm<br />

Inverse P2VP-PS-Mizellen in Lösung können mit verschie<strong>de</strong>nen Metallsalzen bela<strong>de</strong>n wer<strong>de</strong>n.<br />

Selbstorganisationsprozesse führen bei Abscheidung auf glatten Oberflächen zu einer hexagonalen Anordnung.<br />

Nach Entfernung <strong>de</strong>s Polymers in einem H 2 - o<strong>de</strong>r O 2 -Plasma erhält man schließlich <strong>Nano</strong>teilchen, <strong>de</strong>ren Größe<br />

und Abstand durch die Polymerkettenlängen bestimmt wer<strong>de</strong>n. Die Teilchen lassen sich auch noch nachträglich<br />

in einer HAuCl 4 /NH 2 OH-Lösung elektro<strong>de</strong>nfrei weiter vergrößern. Dieser mizellare Ansatz läßt sich mit<br />

lithographischen Metho<strong>de</strong>n kombinieren. In lithographisch <strong>de</strong>finierte Fenster von Lack- o<strong>de</strong>r Metallmasken<br />

lassen sich Mizellen einfüllen und anschließend veraschen. Beim Lift-off <strong>de</strong>r Maske wer<strong>de</strong>n die darauf liegen<strong>de</strong>n<br />

Teilchen mit entfernt, so dass sich nur noch die Teilchen auf <strong>de</strong>r Oberfläche befin<strong>de</strong>n, die direkt auf <strong>de</strong>m<br />

Substrat aufgebracht wur<strong>de</strong>n. Derart <strong>de</strong>ponierte <strong>Nano</strong>teilchen lassen sich beim anisotropen Plasmaätzen als<br />

Maske verwen<strong>de</strong>n, um zum Beispiel <strong>Nano</strong>säulen in Silizium und Titan herzustellen.<br />

O <strong>28</strong>.43 Poster Mi 16:00 Bereich C<br />

15 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

<strong>Nano</strong>structures as a result of the thermal instability of metal thin films on insulators<br />

•Torsten Kolb, Dominik En<strong>de</strong>rs, Annemarie Pucci und Gerhard Fahsold<br />

Kirchhoff-Institut für <strong>Physik</strong>, Universität Hei<strong>de</strong>lberg, Im Neuenheimer Feld 227, D-69120 Hei<strong>de</strong>lberg<br />

We investigate the possibility of structuring metal thin films on a nanoscale by exploiting their thermal instability.<br />

Various metal thin films (Cu, Au, Fe) were <strong>de</strong>posited on different substrates (MgO, SiO 2 ) and subsequent<br />

annealing processes were applied for fractioning these films. For in-situ and online analysis of this fractioning<br />

we use infrared spectroscopy, which we perform during annealing in UHV. Measuring IR transmission enables<br />

investigation of both dynamics and energetics (critical temperatures) of the processes caused by the thermal<br />

instability of metal thin films. Their morphological properties were characterized ex-situ by atomic force<br />

microscopy (AFM). The <strong>de</strong>pen<strong>de</strong>nce of the resulting morphology on annealing temperature and crystalline<br />

structure will be <strong>de</strong>monstrated.<br />

O <strong>28</strong>.44 Poster Mi 16:00 Bereich C<br />

Metal-on-insulator nanostructures via surface color centers<br />

•Svend Vagt, Tammo Block, Volkmar Zielasek und Herbert Pfnür<br />

Institut für Festkörperphysik, Universität Hannover, Appelstr. 2, 30167 Hannover<br />

We present first experimental results obtained in a pursuit of a new type of electron beam nanolithography in<br />

UHV that is based on the generation of surface color center patterns on epitaxial insulator films and the selective<br />

nucleation of metal islands. Experiments were performed in a combined system of an SEM (1-25 keV, resol. 4<br />

nm) and a confocal variable temperature STM (80-900 K). Epitaxial NaCl layers on Ge(100) (up to 6 ML thick)<br />

were irradiated by the electron beam of the SEM un<strong>de</strong>r varying doses. EELS and scanning Auger microscopy<br />

showed the generation of color centers and Na clusters and colloids associated with electron-induced <strong>de</strong>sorption<br />

of Cl in the irradiated areas. The NaCl films turned out to be extremely sensitive to a 3 keV electron beam and<br />

due to high surface mobility of Na metal clusters formed easily. After high e-beam exposure STM at 2<br />

monolayer thick NaCl layers revealed the formation of beam-induced line-shaped gaps in the film down to the<br />

substrate. Depending on the electron dose, a width down to 35 nm was observed, probably limited by<br />

secondary electrons. Deposition of Ag on the surface leads to metal aggregation in the center of the gaps,<br />

presently being investigated by STM and SEM. The un<strong>de</strong>rlying physical mechanisms as well as the potential use<br />

of this type of nanostructuring technique and possible refinements will be discussed.<br />

O <strong>28</strong>.45 Poster Mi 16:00 Bereich C<br />

Pb on Si(557) - Steps towards a one-dimensional conductivity<br />

•Ziad Kallassy, Martin Henzler, Heinz-Lorenz Günter und Herbert Pfnür<br />

Institut für Festkörperphysik,Applestrasse 2,30167 Hannover<br />

The conductivity of ultrathin Pb films evaporated onto a highly stepped Si(557) surface was investigated by<br />

modified macroscopic 4-point measurements in UHV. After annealing 4 to 10 ML of Pb, evaporated at a sample<br />

temperature of 80K, to temperatures of 990K we obtained a strongly anisotropic conductivity at temperatures<br />

below 100K, with up to a factor of 20 higher conductance in the direction parallel to the step edges compared<br />

with the direction normal to them. While conductivity in this direction was found to be thermally activated and<br />

close to the conductivity of 1 ML of Pb on Si(111), it strongly <strong>de</strong>creases with increasing temperature in<br />

directions parallel to steps. The measurements will be correlated with LEED and STM results.<br />

O <strong>28</strong>.46 Poster Mi 16:00 Bereich C<br />

Depen<strong>de</strong>ncy of the scattering of light by small planar particles on the direction of inci<strong>de</strong>nce and<br />

polarization<br />

•Manuel Gonçalves und Othmar Marti<br />

Department of Experimental Physics, University of Ulm, D-89069 Ulm, Germany<br />

16 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

The scattering of light by small particles has been intensively researched in the last <strong>de</strong>ca<strong>de</strong>s. The well known<br />

<strong>de</strong>pen<strong>de</strong>ncies of the scattering of light on the size, shape, material and environment of the particles reveals the<br />

complexity of the problem. Several publications have shown numerical simulations and experimental results<br />

<strong>de</strong>monstrating resonances and local field-enhancements on sub-wavelength particles.<br />

Particles of size comparable to the wavelength and of sub-wavelength size, of planar geometry i.e. where the<br />

thickness is much smaller than their linear dimensions, are of great interest in photonics.<br />

We have investigated planar particles of different shapes by confocal and SNOM microscopy. These particles<br />

show interesting <strong>de</strong>pen<strong>de</strong>ncies on the direction of the inci<strong>de</strong>nce of light, on polarization and on the dielectric<br />

constant of the material.<br />

We have observed important differences in the scattering patterns for each material, and each relative orientation<br />

of the particles with the direction of inci<strong>de</strong>nce of the light.<br />

O <strong>28</strong>.47 Poster Mi 16:00 Bereich C<br />

Self-imaging observed on colloid crystals and Fischer projection patterns<br />

•Manuel Gonçalves und Othmar Marti<br />

Department of Experimental Physics, University of Ulm, D-89069 Ulm, Germany<br />

The self-imaging phenomenon in optical systems is known since the Talbot effect was discovered in the 19th<br />

century. The Talbot effect is generated by the interference of the incoming light from a diffraction array of<br />

apertures of size a that takes place near the array (Fresnel zone). In general, a >> λ.<br />

Apertures separated by a distance d, when illuminated by a coherent and plane wave of wavelength λ produce<br />

self-images at distances d T = ν 2 d 2 / λ, for ν = 1, 2, ... [1],[2].<br />

We have observed that arrays of colloidal crystals of polystyrene spheres with diameter of few µm produce<br />

self-images, at distances of several tenths of µm. The theoretical Talbot length is compared with the measured<br />

distances for self-images, for different illumination mo<strong>de</strong>s of coherent light.<br />

A discussion of the multiple scattering and diffraction of light by a regular array of colloidal particles is<br />

introduced and analyzed.<br />

[1] K. Patorski, in Prog. Opt. XXVII, Elsevier, 1989.<br />

[2] A. Lohmann and J. A. Thomas, Appl. Opt., 29 29, 4337-4340.<br />

O <strong>28</strong>.48 Poster Mi 16:00 Bereich C<br />

Plasma CVD-grown carbon nanotubes studied by field emission<br />

•Daniell Malsch 1 , Martin Sveningsson 2 , Eleanor Campbell 2 und Juergen A. Schaefer 1<br />

1 Institut für <strong>Physik</strong> und Zentrum für Mikro- und <strong>Nano</strong>technologien, TU Ilmenau, P.O. Box 100565, 98684<br />

Ilmenau, Germany<br />

2 Department of Experimental Physics, Gothenburg University and Chalmers University of Technology, 41296<br />

Gothenburg, Swe<strong>de</strong>n<br />

Films of carbon nanotubes show an excellent field emission behaviour that allows a wi<strong>de</strong> range of application in<br />

field emitting <strong>de</strong>vices. The influence of the different emission parameters has to be investigated in or<strong>de</strong>r to<br />

improve their performance. We study the field emission of vertically aligned PCVD-grown multiwall carbon<br />

nanotubes. A systematic influence of the tube length on the emission current, the light emission, and the surface<br />

temperature of the film is found. We also examine blackbody radiation from resistive heating during field<br />

emission. This leads, in agreement with light emission behaviour and long-time stability measurements, to a<br />

stepwise <strong>de</strong>gradation of the carbon nanotube films.<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

O <strong>28</strong>.49 Poster Mi 16:00 Bereich C<br />

Generation of metal nanodroplets and experiments on their velocity and landing<br />

•Anja Habenicht, Michael Olapinski, Johannes Boneberg und Paul Lei<strong>de</strong>rer<br />

Universität Konstanz, FB <strong>Physik</strong> SFB 513, 78457 Konstanz<br />

An interesting observation can be ma<strong>de</strong> when gold nanostructures placed on a substrate are illuminated with an<br />

intensive short laser pulse: Just above the melting threshold all particles leave the surface. The reason for this<br />

effect is the wetting behaviour: Gold does not wet the glass substrate, thus the liquid nanostructures can reduce<br />

their surface energy by reforming to spheres. If this transformation is sufficiently fast the liquid spheres take<br />

off from the surface. The velocity of the flying nanodroplets can be <strong>de</strong>termined by analyzing the time <strong>de</strong>pen<strong>de</strong>nt<br />

scattering signal which arises when the droplets cross a sheet of light. This signal can be converted into a<br />

velocity <strong>de</strong>pen<strong>de</strong>nt particle <strong>de</strong>nsity. The particles cool down during the flight due to thermal radiation. By<br />

catching the nanodroplets on a further substrate at different distances, the droplets can be lan<strong>de</strong>d either in liquid<br />

or in solid state. First results of velocity measurements and the impact experiments are shown.<br />

O <strong>28</strong>.50 Poster Mi 16:00 Bereich C<br />

<strong>Nano</strong>structuring using colloid crystals and dry and wet etching techniques<br />

•Manuel Gonçalves 1 , Moritz Trautvetter 2 , Oliver Dubbers 2 , Sebastian Fricker 2 , Alfred Plettl 2 , Paul Ziemann 2<br />

und Othmar Marti 1<br />

1 Department of Experimental Physics, University of Ulm, D-89069 Ulm, Germany<br />

2 Department of Solid State Physics, University of Ulm, D-89069 Ulm, Germany<br />

Sub-wavelength structures produced using latex colloidal crystals have been intensively investigated in the last<br />

years, namely to produce photonic crystals. One of most known techniques to produce nanoparticles using<br />

monolayers of latex spheres as lithographic masks, has been <strong>de</strong>veloped by U. Ch. Fischer et al. in 1981 (Fischer<br />

projection patterns or FPP). This method, however, is restricted to few possible particle shapes.<br />

We have <strong>de</strong>veloped two techniques to extend the number the possible shapes and geometrical configurations,<br />

using colloidal crystals and FPPs combined with dry and wet etching techniques.<br />

Inverse projection pattens have been produced using the common FPPs combined with wet chemical etching.<br />

We have also <strong>de</strong>veloped a technique to produce sub-wavelength structures using monolayers of latex spheres<br />

etched by a plasma. The size and the separation of the particles can be controlled by the etching level and by<br />

selecting the size of the latex spheres.<br />

Several nanostructures using these techniques have been produced and characterized by scanning probe<br />

microscopy and scanning electron microscopy. The optical properties of some samples produced using metallic<br />

thin films are also presented.<br />

O <strong>28</strong>.51 Poster Mi 16:00 Bereich C<br />

Application of imaging XPS for chemical analysis and mapping of magnetic domains<br />

•S. Schmidt 1 , M. Escher 2 , F. Forster 1 , D. Funnemann 3 , B. Krömker 3 , M. Merkel 2 , F. Reinert 1 und N. Weber 2<br />

2 Focus GmbH<br />

3 Omicron <strong>Nano</strong>technology GmbH<br />

1 Universität <strong>de</strong>s Saarlan<strong>de</strong>s, FR 7.2 Experimentalphysik, Postfach 151150, 66041 Saarbrücken<br />

We present first scientific applications of a new <strong>Nano</strong>ESCA [1] spectrometer: we have used the good spatial<br />

resolution to investigate the chemical structure of plain and <strong>de</strong>corated grain boundaries in two reference<br />

materials Al 0.98 Sn 0.02 and Cu 0.98 Bi 0.02 [2]. The data measured at the high-intensity small-spot beamlines of<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

BESSY II also exhibit <strong>de</strong>tailed information about the oxidation processes in such materials. In Al 0.98 Sn 0.02 we<br />

have <strong>de</strong>tected small differences in the binding energy of the Al 2p XPS peak of 30-50 meV that could be related<br />

to different grain orientations. We also present data taken on the nanowire prototype system Cu/ZnSe 2 [3]<br />

where the Cu-nanowires are effectively protected against oxidation even during air-exposure. Using cicular<br />

polarization at the undulator we were able to map magnetic domains [4] in a Fe single crystal at the Fe 2p XPS<br />

core-level with high contrast.<br />

[1] D. Funnemann et al., Bessy Annual Report, 2002<br />

[2] S. Schmidt et al., Bessy Annual Report, 2002<br />

[3] R. A<strong>de</strong>lung et. al, Adv. Mater. 14, 15, p.<br />

[1056-1061, 2002 4] C. Schnei<strong>de</strong>r et al., Rep. Prog. Phys, 65, R1785-R1839, 2002<br />

O <strong>28</strong>.52 Poster Mi 16:00 Bereich C<br />

Lead on hydrogen terminated Si(111): A comparison of two different <strong>de</strong>position techniques<br />

•C. Rettig 1,2 , H. Hövel 1 , V. Chamard 1 , S. Warren 2 , T. H. Metzger 2 und J. Zegenhagen 2<br />

1 Universität Dortmund, Experimentelle <strong>Physik</strong> I, D-44221 Dortmund (Germany)<br />

2 European Synchrotron Radiation Facility (ESRF), B.P. 220, F-38043 Grenoble (France)<br />

We studied the epitaxy of electrochemically <strong>de</strong>posited Pb clusters on Si(111):H <strong>de</strong>pen<strong>de</strong>nt on the applied<br />

overpotential. The former measurements [1] and the present investigations are carried out in-situ using Cyclic<br />

Voltammograms and Surface X-ray Diffraction (SXRD). The specular measurements show a predominant<br />

alignment of the Pb(111) plane parallel to the Si(111) plane. In the sample plane the Pb Clusters are aligned<br />

along the high symmetry direction of Si confirmed by Grazing Inci<strong>de</strong>nce Diffraction (GID). New results<br />

indicate a <strong>de</strong>pen<strong>de</strong>ncy of the Pb clusters alignment in the sample plane on the applied overpotential. Presently we<br />

extend our measurements to Ultra High Vacuum (UHV) environment with in-situ <strong>de</strong>position of Pb on Si(111):H.<br />

This system is studied by Scanning Tunneling Microscopy/Spectroscopy (STM/STS), Low Energy Electron<br />

Diffraction (LEED) and Ultraviolet Photoelectron Spectroscopy (UPS).<br />

[1] J. C. Ziegler et al., Surf. Sci. 452, 150 (2000).<br />

O <strong>28</strong>.53 Poster Mi 16:00 Bereich C<br />

Lifetime of particle plasmon excitation in Ag-<strong>Nano</strong>particles<br />

•Daniela Bayer, Alexan<strong>de</strong>r Mönnich, Jörg Lange, Michael Bauer und Martin Aeschlimann<br />

Dep. of Physics, University of Kaiserslautern<br />

The dynamics of photoexcited hot electrons are of special interest for a large variety of mo<strong>de</strong>rn fields such as<br />

fs-photochemistry and (magneto)electronics. These specific applications <strong>de</strong>pend critically on the inelastic<br />

lifetime T 1 of these hot electrons. Hence, the question arises if it would be possible to manipulate T 1 in a<br />

specific way. In this poster, we will <strong>de</strong>monstrate that the specific structuring of the material on a nanometer<br />

scale can govern the effective electron dynamics. Our interest is focused on localized collective oszillations of<br />

the electron gas in metal particles of nanometer size, the so-called particle plasmons. A. Liebsch predicts that<br />

un<strong>de</strong>r certain conditions the plasmon <strong>de</strong>phasing time at off-resonance excitation can be longer than on<br />

resonance due to the wavelength <strong>de</strong>pen<strong>de</strong>nce of radiation damping. Making use of the Time-Resolved<br />

Two-Photon-Photoemission (TR-2PPE), our investigation concentrates on elliptically shaped silver<br />

nano-particles un<strong>de</strong>r resonant and off-resonant conditions. Experimental results confirming Liebschs theory will<br />

be shown.<br />

O <strong>28</strong>.54 Poster Mi 16:00 Bereich C<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

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Surface Plasmon Propagation In Metallic <strong>Nano</strong>structures<br />

•Phillip Olk 1 , Jan Sei<strong>de</strong>l 1 , Stefan Grafström 1 , Eng Lukas 1 , Fadi Baida 2 , Daniel Van Labeke 2 , Marcell Ott 3 und<br />

Lothar Bischoff 4<br />

1 Institut für Angewandte Photophysik, TU Dres<strong>de</strong>n, 01062 Dres<strong>de</strong>n<br />

2 Laboratoire d'Optique P.M. Duffieux, CentreNational <strong>de</strong> La Recherche Scientifique, Unité Mixte <strong>de</strong>Recherche<br />

6603, Université <strong>de</strong> Franche-Comté, F-25030Besançon Ce<strong>de</strong>x, France<br />

3 Organic Chemistry III / Macromolecular Chemistry, Universität Ulm, 89081 Ulm<br />

4 Research Center Rossendorf, Institute of Ion BeamPhysics and Materials Research, 01314 Dres<strong>de</strong>n<br />

Propagation of surface plasmons in metallic nanostructures and their interaction with <strong>de</strong>fined surface features<br />

are presented. We use near-field optical methods in or<strong>de</strong>r to reveal various properties of such travelling surface<br />

waves, like optical transmission across barriers or coupling to free space electromagnetic waves. These<br />

characteristics are directly <strong>de</strong>termined using an attenuated-total-reflection (ATR) excitation scheme together<br />

with dielectric fiber probes for near-field optical <strong>de</strong>tection. We show results on plasmon propagation in<br />

self-assembled cluster films, discussing propagation lengths and resonance conditions. Furthermore, we present<br />

an experimental and theoretical analysis of plasmon mo<strong>de</strong> coupling in continuous metallic films mediated by a<br />

single groove structure produced by focused ion beam (FIB) writing.<br />

O <strong>28</strong>.55 Poster Mi 16:00 Bereich C<br />

Optical anisotropy of Cs nanostructure formation on GaAs(110), InP(110) and InAs(110)<br />

•Karsten Fleischer 1,2 , Gianlorenzo Bussetti 2 , Claudio Goletti 2 , Pierro Chiaradia 2 und Wolfgang Richter 1,2<br />

2 Universitá ``Tor Vergata'', Dipartimento di Fisica, Via Ricerca Scientifica 1, 00133 Roma, Italy<br />

1 TU-Berlin, Institut für Festkörperphysik, Har<strong>de</strong>nbergstr. 36, 10623 Berlin, Germany<br />

We present reflectance anisotropy spectra (RAS) of Cs covered GaAs, InP and InAs cleaved (110) surfaces. In<br />

such systems Cs forms one dimensional wirelike structures at low coverages. For the first time we studied the<br />

formation of these wires in situ with optical and therefore non<strong>de</strong>structive techniques. Wire formation is<br />

accompanied with characteristic minima in the RAS spectra between the E 0 + ∆ 0 and E 1 bulk critical point.<br />

With growing coverages (θ > 0.3 ML) and formation of the two dimensional closed Cs layer (θ ? 0.5 ML),<br />

changes in the Cs related minima occur. Different wire types and also the transition into the disor<strong>de</strong>red Cs<br />

double layers at saturation coverage ( θ ? 1 ML) can be monitored optically.<br />

O <strong>28</strong>.56 Poster Mi 16:00 Bereich C<br />

Methanol oxidation on clean and oxygen-covered copper surfaces<br />

•Sung Sakong und Axel Groß<br />

<strong>Physik</strong>-Department T30, Technische Universität München, 85747 Garching, Germany<br />

We have studied methanol oxidation steps over clean and oxygen-covered copper surfaces by <strong>de</strong>nsity functional<br />

theory (DFT) calculations. The reaction pathways are <strong>de</strong>termined by the nudged elastic band (NEB) method [1]<br />

which in particularly also yields the intermediate states and the reaction barriers. We find that on clean copper<br />

surfaces, methanol is only weakly bound. The <strong>de</strong>composition into methoxy and hydrogen is activated. Upon<br />

heating, methanol rather <strong>de</strong>sorbs than dissociates. The further <strong>de</strong>composition of adsorbed methoxy into<br />

formal<strong>de</strong>hy<strong>de</strong> and hydrogen is hin<strong>de</strong>red by large barriers ( ? 1.5eV).<br />

The surface intermediate states in the methanol oxidation are significantly stabilised by co-adsorbed oxygen. The<br />

DFT calculations show that on oxygen-covered Cu(110), methanol dissociates spontaneously because of the<br />

strong attraction between the methanol hydroxyl hydrogen and the surface oxygen. The reaction steps are<br />

analysed in terms of the un<strong>de</strong>rlying electronic structure. Our calculations confirm the importance of co-exposed<br />

oxygen in the methanol oxidation on copper surfaces found in experiments (see, e.g., [2]).<br />

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[1] G. Henkelman and H. Jónsson, J. Chem. Phys. 113, 9978 (2000).<br />

[2] Ch. Ammon et al., Surf. Sci. 507, 845 (2002).<br />

O <strong>28</strong>.57 Poster Mi 16:00 Bereich C<br />

Electron Solvation during the Interaction of Na Atoms with Polar Molecules<br />

•A. Borodin 1 , O. Höfft 1 , U. Kahnert 1 , V. Kempter 1 , Y. Ferro 2 und A. Allouche 2<br />

1 Institut für <strong>Physik</strong> und <strong>Physik</strong>alische Technologien, TU Clausthal, Leibnizstr. 4, D-38678 Clausthal-Zellerfeld<br />

2 Physique <strong>de</strong>s Interactions Ioniques et Moléculaires, CNRS-UMR6633 Campus Universitaire <strong>de</strong> Saint Jérôme,<br />

Marseille France<br />

The interaction of Na atoms with molecular films (H 2 O; CH 3 OH; NH 3 ) was studied with metastable impact<br />

electron spectroscopy (MIES) un<strong>de</strong>r UHV conditions. The films were grown at 90K, and exposed to Na. The<br />

spectral feature from 3sNa ionization occurs at an energetic position different from that found for metals or<br />

semiconductors. The results are compared with DFT calculations. Experiment and theory agree in the energetic<br />

positions of the main spectral features from the molecular and sodium ionization. The calculations suggest that<br />

the 3sNa emission observed experimentally originates from solvated 3s electrons which are located far from the<br />

Na-core and become stabilized by solvent molecules. The simultaneous emergence of emission from OH (or<br />

CH 3 O) and from solvated 3s electrons suggests that the <strong>de</strong>localization and, consequently, the solvation play an<br />

important role in the Na-induced formation of CH 3 O and OH species from methanol and water, respectively.<br />

O <strong>28</strong>.58 Poster Mi 16:00 Bereich C<br />

Spectral evi<strong>de</strong>nce for oxi<strong>de</strong> free incorporation of oxygen into Ru(0001)<br />

•Raoul Blume 1 , Artur Böttcher 2 , Horst Conrad 3 und Horst Niehus 1<br />

1 Institut für <strong>Physik</strong>, HU-Berlin, Newtonstr. 15, 12489 Berlin<br />

2 Institut für <strong>Physik</strong>alische Chemie, Universität Karlsruhe, Kaiserstr. 12, 76131 Karlsruhe<br />

3 Fritz-Haber-Institut <strong>de</strong>r Max-Planck-Gesellschaft, Faradayweg 4-6, 14195 Berlin<br />

The capability of a smooth and <strong>de</strong>fected Ru(0001) surface towards the oxygen accumulation has been studied<br />

by the means of thermal <strong>de</strong>sorption spectroscopy (TDS) and the high resolution scanning XPS (Elettra,<br />

Trieste). By applying a soft Ar + -sputtering procedure individual surface <strong>de</strong>fects confined to the two outermost<br />

Ru layers were created. The oxidation procedure applied here assures an incorporation of oxygen atoms in the<br />

subsurface region up to 4 monolayer equivalents (MLE) without any traces of RuO 2 -domains (high-pressure<br />

and low-temperature surface oxidation). By measuring the temperature and exposure <strong>de</strong>pen<strong>de</strong>nce of the oxygen<br />

incorporation and analyzing the corresponding evolution of the Ru 3d 5/2 band we found characteristic electronic<br />

signatures allowing to distinguish oxygen atoms occupying the Ru(I)-Ru(II) interlayer space and oxygen species<br />

associated with surface <strong>de</strong>fects. This assignment is supported by mesoscopic-scale surface images as well as<br />

the quantitative O 2 -TD analysis.<br />

O <strong>28</strong>.59 Poster Mi 16:00 Bereich C<br />

Investigation of Au electro<strong>de</strong>position processes on metal single crystal surfaces<br />

•Ahmed Ayyad, Jochim Stettner und Olaf Magnussen<br />

Institut für Experimentelle und Angewandte <strong>Physik</strong>, Christian-Albrechts-Universität Kiel, Leibnizstraße 19,<br />

24098 Kiel<br />

Metal electro<strong>de</strong>position processes have been a subject of substantial basic research during the last years,<br />

motivated by current technologies as well as future applications, such as the electrochemical formation of<br />

ultrathin layers and nanostructures. A major, largely unsettled question is how the electro<strong>de</strong> surface structure<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

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and adsorbates, such as anions or organic additives, influence the growth process. We studied the homoepitaxial<br />

electro<strong>de</strong>position of Au on Au(111) electro<strong>de</strong> surfaces (<strong>de</strong>position rates 0.05 to 0.23 ML/min.) by in-situ x-ray<br />

diffraction un<strong>de</strong>r real time conditions using a hanging-meniscus transmission cell (reduced cell resistance,<br />

unrestricted mass transport), where the Au(111) electro<strong>de</strong> surface is completely covered by an electrolyte<br />

droplet. Parallel to the X-ray measurements cyclic voltammograms were recor<strong>de</strong>d, which confirm that the<br />

hanging-meniscus cell allows high quality electrochemical measurements combined with in-situ surface X-ray<br />

diffraction studies. The X-ray diffraction data and complementary in-situ ellipsometric measurements indicate<br />

that the <strong>de</strong>position process is accompanied by substantial surface roughening.<br />

O <strong>28</strong>.60 Poster Mi 16:00 Bereich C<br />

State selective <strong>de</strong>tection of D 2 after femtosecond-laser induced <strong>de</strong>sorption from Ru(001)<br />

•S. Wagner 1 , M. Rutkowski 2 , R. Du<strong>de</strong>k 3 , C. Frischkorn 1 , H. Zacharias 2 und M. Wolf 1<br />

3 Fritz-Haber-Institut <strong>de</strong>r MPG, Berlin<br />

1 Freie Universtät, Berlin<br />

2 Westfälische Wilhems-Universität, Münster<br />

The energy transfer into different <strong>de</strong>grees of freedom in the fs-laser induced recombinative <strong>de</strong>sorption of<br />

<strong>de</strong>uterium from Ru(001) has been investigated with (1+1')-REMPI and time-of-flight measurements. It has been<br />

shown that hot substrate electrons mediate this reaction within a few hundred femtoseconds [1]. The<br />

rovibrational distributions of the <strong>de</strong>sorbing D 2 molecules are <strong>de</strong>tected via various B 1 Σ u + ? X 1 Σ g + Lyman bands<br />

using tunable vacuum ultraviolet (VUV) laser radiation for the resonant excitation step [2]. Populations of the<br />

rotational quantum states in the vibrational ground and the first excited state are measured. The rotational energy<br />

of D 2 in the vibrational ground state (E rot /k B = 800?200 K) is much lower than the rotational energy in the<br />

excited state ( E rot /k B = 1500?300 K). Assuming a Boltzmann-like energy distribution, these results indicate a<br />

vibrational temperature of E vib /k B = 1200?150 K. The amount of energy coupled to the translation is E trans /k B =<br />

1700?300 K. Possible reasons for the incomplete thermalization will be discussed.<br />

[1] D. N. Denzler, C. Frischkorn, C. Hess, M. Wolf, and G.<br />

[Ertl, Phys. Rev. Lett., in press 2] D. Wetzig, M. Rutkowski, H. Zacharias, and A. Groß Phys. Rev. B 63,<br />

205412 (2001)<br />

O <strong>28</strong>.61 Poster Mi 16:00 Bereich C<br />

Characterisation of Pd/Zn/ZnO real catalysts for methanol steam reforming<br />

•S. Pöllmann 1 , J. Pantför<strong>de</strong>r 1 , A. Kölbl 2 , P. Pfeifer 2 , M. Fichtner 3 , D. Borgmann 1 , R. Denecke 1 und H.-P.<br />

Steinrück 1<br />

1 <strong>Physik</strong>alische Chemie II, Universität Erlangen, Egerlandstr. 3, 91058 Erlangen.<br />

2 FZ Karlsruhe GmbH, Institut für Mikroverfahrenstechnik -IMVT-, Postfach 3640, 76021 Karlsruhe.<br />

3 FZ Karlsruhe GmbH, Institut für <strong>Nano</strong>technologie -INT-, Postfach 3640, 76021 Karlsruhe.<br />

We studied the chemical composition and the temperature <strong>de</strong>pen<strong>de</strong>nt behavior of Pd/Zn/ZnO catalysts that are<br />

used for methanol steam reforming. Real catalysts coated on microstructured foils have been used and their<br />

performance has been characterised in a high pressure flow apparatus un<strong>de</strong>r realistic reaction conditions. We<br />

investigated these samples by means of X-ray photoelectron spectroscopy (XPS) with Al Kα radiation. Utilizing<br />

a high pressure XPS system the experiments were performed in-situ and in the presence of methanol and water<br />

vapour in a pressure range up to 1 mbar, at different temperatures. These measurements allow to establish a<br />

correlation between the different activities for the methanol steam reforming and the chemical composition of<br />

the catalysts surface. Supported by the DFG (Schwerpunktsprogramm 1091, Ste 620/3-3, Fi 816/1-1,2)<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

O <strong>28</strong>.62 Poster Mi 16:00 Bereich C<br />

Drei unterschiedliche Ursachen für beim maschinellen Geschirrspülen auftreten<strong>de</strong><br />

Glasoberflächenschä<strong>de</strong>n<br />

•Chun Wang 1 , Klaus-Peter Martinek 2 , Edda Rädlein 3 und Georg Krausch 1<br />

1 <strong>Physik</strong>alische Chemie II, Universität Bayreuth<br />

2 Nachtmann GmbH<br />

3 IMA, Universität Bayreuth<br />

1. Glasstruktur: Nach einigen hun<strong>de</strong>rt Spülgängen ist die glatte "Glashaut" abgetragen und es bil<strong>de</strong>n sich<br />

Kornmuster in <strong>de</strong>r Größe von 30 nm. Bei mehr als tausend Spülgängen sind diese Körner verschwun<strong>de</strong>n und<br />

Waffelmuster mit Löchern in <strong>de</strong>r Größe bis zu einem µm haben sich gebil<strong>de</strong>t. Damit erscheinen die Gläser<br />

getrübt. Dieses Phänomen kann mit <strong>de</strong>r Theorie <strong>de</strong>r Ionen-Kanäle im Glasnetzwerk von Greaves und mit<br />

unserem Vorschlag einer Glashaut gut erklärt wer<strong>de</strong>n.<br />

2. Feuerpolitur: An manchen Gläsern konnten bereits nach wenigen Spülzyklen wolkige Oberflächenschä<strong>de</strong>n<br />

beobachtet wer<strong>de</strong>n. Die Schä<strong>de</strong>n haben ihre Ursache im industriellen Prozess <strong>de</strong>r Feuerpolitur. Die auf die<br />

Glasoberfläche treffen<strong>de</strong> Flamme hat einen großen Temperaturgradienten. So treten je nach Position <strong>de</strong>r Flamme<br />

unterschiedliche Muster <strong>de</strong>r Phasentrennung in Erscheinung.<br />

3. Organische Komplexbildung durch Getränke: An <strong>de</strong>r Innenseite einzelner, über lange Zeit verwen<strong>de</strong>ter Gläser<br />

ist ein goldfarbiger Belag zu beobachten. Die Reaktionsschicht ist nicht dicht und das Glas unterhalb dieser<br />

Schicht zeigt eine weitere Korrosion. Die Schicht ist auf eine Komplexbildung von organischen Komponenten<br />

aus <strong>de</strong>n Getränken mit <strong>de</strong>m Glas zurückzuführen.<br />

O <strong>28</strong>.63 Poster Mi 16:00 Bereich C<br />

Deposition massenselektierter Metallclusterionen unter Verwendung einer Magnetronsputterquelle<br />

•Nils Bertram, Tim Fischer, Rainer Dietsche, Felix v.Gynz-Rekowski, Young Dok Kim und Gerd Ganteför<br />

Fachbereich <strong>Physik</strong>, Universität Konstanz, 78547 Konstanz.<br />

Das weiche Lan<strong>de</strong>n von massenselektierten Clusterionen erlaubt die Präparation von nanostrukturierten<br />

Oberflächen im extrem kleinen Größenbereich unterhalb von 3 nm und mit atomarer Präzision: die Zahl <strong>de</strong>r<br />

Atome in <strong>de</strong>r <strong>Nano</strong>struktur ist exakt bekannt. Das Problem bei dieser Art von Experimenten ist die niedrige<br />

Intensität <strong>de</strong>r üblichen Clusterionenquellen. Wir präsentieren erste Studien mit einer neu aufgebauten<br />

Magnetron-Sputterquelle (Haberland-Typ). Die <strong>de</strong>ponierten Cluster wer<strong>de</strong>n mittels<br />

Elektron-Energieverlust-Spektroskopie untersucht.<br />

O <strong>28</strong>.64 Poster Mi 16:00 Bereich C<br />

Katalytische Reaktionen massenselektierter E<strong>de</strong>lmetallcluster<br />

•T. M. Bernhardt, L. D. Socaciu, J. Hagen, D. Popolan, J. Le Roux, T. Gleitsmann, M. Vaida, B. Stegemann<br />

und L. Wöste<br />

Institut für Experimentalphysik, Freie Universität Berlin<br />

Kleine Gold- und Silbercluster mit bis zu 13 Atomen zeigen eine starke Größenabhängigkeit in ihrer chemischen<br />

Reaktivität. Für bestimmte Clustergrößen kann in <strong>de</strong>r Gasphase die katalytische Konvertierung von<br />

Kohlenmonoxid zu Kohlendioxid nachgewiesen wer<strong>de</strong>n. Studien zur temperaturabhängigen Kinetik geben<br />

Aufschluß über <strong>de</strong>n Reaktionsmechanismus. Strukturinformationen <strong>de</strong>r Zwischenprodukte können aus<br />

theoretischen Berechnungen und laserspektroskopischen Untersuchungen gewonnen wer<strong>de</strong>n. Aus <strong>de</strong>m<br />

Vergleich zu auf <strong>de</strong>finierten Oberflächen massenselektiv <strong>de</strong>ponierten Clustern können Informationen über <strong>de</strong>n<br />

Einfluß <strong>de</strong>s Trägers auf die katalytische Aktivität gewonnen wer<strong>de</strong>n. Beson<strong>de</strong>re Aufmerksamkeit gilt <strong>de</strong>m<br />

Einfluß <strong>de</strong>r elektronischen Struktur <strong>de</strong>r Cluster auf die Reaktivität und <strong>de</strong>r Modifikation <strong>de</strong>r elektronischen<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Struktur durch <strong>de</strong>n Kontakt mit verschie<strong>de</strong>nen Substraten.<br />

O <strong>28</strong>.65 Poster Mi 16:00 Bereich C<br />

Einfluss <strong>de</strong>r Brechzahl <strong>de</strong>s dielektrischen Substrats auf die optischen Eigenschaften einzelner<br />

Goldnanopartikel<br />

•Katharina Schätzler, Benjamin Schmidt, Christian Dahmen und Gero von Plessen<br />

I. <strong>Physik</strong>alisches Institut (IA), RWTH Aachen<br />

In Berechnungen auf <strong>de</strong>m Gebiet <strong>de</strong>r optischen Eigenschaften von Metallnanopartikeln wird die inhomogene<br />

dielektrische Umgebung <strong>de</strong>s Partikels oft durch einfache Mittelwertbildung über die Umgebungsbrechzahlen<br />

berücksichtigt. In unserer Arbeit wird <strong>de</strong>r Einfluss <strong>de</strong>r Brechzahl <strong>de</strong>s dielektrischen Substrats auf die optischen<br />

Eigenschaften sphärischer Goldnanopartikel mit Hilfe <strong>de</strong>r Dunkelfeld-Mikroskopie sowie -Spektroskopie<br />

untersucht. Diese Metho<strong>de</strong> macht es möglich, einzelne <strong>Nano</strong>partikel zu spektroskopieren und so inhomogene<br />

Verbreiterungseffekte zu vermei<strong>de</strong>n.<br />

O <strong>28</strong>.66 Poster Mi 16:00 Bereich C<br />

Optische Eigenschaften kleiner Aggregate aus Goldnanopartikeln<br />

•Benjamin Schmidt, Katharina Schätzler, Christian Dahmen und Gero von Plessen<br />

I.<strong>Physik</strong>alisches Institut A, RWTH Aachen<br />

Liegen E<strong>de</strong>lmetall-<strong>Nano</strong>partikel nah genug beieinan<strong>de</strong>r, um elektromagnetisch miteinan<strong>de</strong>r zu koppeln, bil<strong>de</strong>n<br />

sich ausge<strong>de</strong>hnte Plasmonen-Mo<strong>de</strong>n aus. Hier untersuchen wir mit Dunkelfeldmikroskopie kleine Aggregate aus<br />

gekoppelten, kugelförmigen Goldnanopartikeln, insbeson<strong>de</strong>re Partikelpaare. Um eine Korrelation <strong>de</strong>r<br />

Aggregat-Topographie und <strong>de</strong>r optischen Eigenschaften herzustellen und um inhomogene Verbreiterungseffekte<br />

zu vermei<strong>de</strong>n, wird polarisationsselektive Spektroskopie an einzelnen Aggregaten durchgeführt. Die nötigen<br />

topographischen Informationen wer<strong>de</strong>n aus elektronenmikroskopischen Aufnahmen gewonnen. Die<br />

experimentellen Ergebnisse wer<strong>de</strong>n mit Resultaten aus <strong>de</strong>r Verallgemeinerten Mie-Theorie verglichen, und es<br />

wird <strong>de</strong>r Versuch unternommen, die Beiträge bestimmter Mo<strong>de</strong>n zu <strong>de</strong>n Spektren zu i<strong>de</strong>ntifizieren.<br />

O <strong>28</strong>.67 Poster Mi 16:00 Bereich C<br />

Homogeneous linewidth of gold nanoshells<br />

•S. Brogl, G. Raschke, A. Susha, A. L. Rogach, T. A. Klar und J. Feldmann<br />

Photonics and Optoelectronics Group, Physics Department and CeNS, University of Munich, Amalienstr. 54,<br />

D-80799 Munich, Germany<br />

<strong>Nano</strong>shells composed of a few nanometer thin gold layer coated on Au 2 S nanoparticles show a pronounced<br />

resonance in their scattering spectra for visible light. Similar to solid noble metal nanoparticles the origin of the<br />

resonance is a collective oscillation of the conduction band electrons, which is known as the nanoparticle<br />

plasmon (NPP). The NPP resonance position of a gold nanoshell can be tuned over a large spectral range by<br />

varying the relative size of the nanoparticle core and the thickness of the gold shell.<br />

Experiments carried out on ensembles of nanoshells show a broad absorption linewidth (FWHM) of about<br />

600 meV. This is by far exceeding what is expected by Mie-theory calculations which yield a NPP resonance<br />

line width of less than 100 meV. We investigate this discrepancy by measuring the homogeneous scattering<br />

spectrum of a single gold nanoshell using dark field microscopy. The results show a homogeneous linewidth<br />

narrowed by 50% compared to ensemble measurements. This indicates that inhomogeneities e.g. distribution of<br />

shell thicknesses and/or core diameters are one important parameter for line broa<strong>de</strong>ning.<br />

O <strong>28</strong>.68 Poster Mi 16:00 Bereich C<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

STM/STS on large silver clusters at germanium (001)<br />

•Karl-Ludwig Jonas, Armin Kleibert, Fanny Geisler, Ralf-Peter Methling, Joachim Bansmann, Viola von<br />

Oeynhausen und Karl Heinz Meiwes-Broer<br />

Fachbereich <strong>Physik</strong>, Universität Rostock, Universitätsplatz 3, D-18051 Rostock<br />

Cluster <strong>de</strong>position is used to create metal-nanodots with a high aspect ratio. We present scanning tunneling<br />

spectroscopy (STS) measurements on isolated silver clusters at germanium (001). The clusters are generated<br />

using an arc cluster ion source (ACIS), mass selected and <strong>de</strong>posited un<strong>de</strong>r soft landing conditions (E kin /atom <<br />

0.5eV). Before performing STM experiments the cluster structure has been investigated using TEM, electron<br />

diffraction and EDX. Particle diameters between 5 and 14 nm have been used for the present studies. Scanning<br />

tunnelling microscopy images of large clusters always contain consi<strong>de</strong>rable tip folding at the steep cluster edges.<br />

Besi<strong>de</strong> the accurately measured cluster height the imaging of particles of this height is therefore restricted to<br />

cluster facets at the top. Using STM and STS on <strong>de</strong>posited silver clusters structural and electronic properties<br />

are observed. In contrast to silver islands grown on germanium (001) the orientation of the crystal lattice is not<br />

fixed if cluster melting is neglected. However, some of the clusters show hexagonal facets at the top. STS is<br />

sensitive to occupied and unoccupied states near the Fermi level and reveals the existence of distinct states in<br />

the tunneling conductivity of the substrate as well as on the clusters. Thus, the richly structured <strong>de</strong>nsity of<br />

states of the germanium (001) surface has been discovered and serves as STM/STS condition test.<br />

O <strong>28</strong>.69 Poster Mi 16:00 Bereich C<br />

Application of the variable phase theory to the systems with quasistationary states.<br />

•Oleg Kidun 1 , Jamal Berakdar 1 und Natasha Fominykh 2<br />

1 Max-Planck Institut fuer Mikrostrukturphysik, Halle, Germany<br />

2 Institute of Physics, St. Petersburg State University, St. Petersburg, Russia<br />

We <strong>de</strong>velop a method of investigation of the quasistationary (QS) states of different physical systems based on<br />

the variable phase approach [1-3]. We consi<strong>de</strong>r the modification of the physical properties of the QS states<br />

(energy position and resonance width) un<strong>de</strong>r the spatial transformation of the potential field as well as its<br />

asymptotical behavior. The role of the possible nonlocality of the potential in the observability of the QS states is<br />

also estimated. The realization of our approach in the studies of molecules and nanostructures is discussed.<br />

[1] F. Calogero, Variable Phase Approach in Potential Scattering, AP, NY (1967)<br />

[2] V. Babikov, Method of the Phase Functions in Quantum Mechanics, Nauka, Moscow (1969)<br />

[3] O. Kidun, N. Fominykh, J. Berakdar, J. Phys. A 35, 9413 (2001)<br />

O <strong>28</strong>.70 Poster Mi 16:00 Bereich C<br />

Electron dynamics of buried interface states in Ar/Cu(100) probed by time-resolved two-photon<br />

photoemission<br />

•M. Rohle<strong>de</strong>r, W. Berthold, K. Duncker, J. Güd<strong>de</strong> und U. Höfer<br />

Fachbereich <strong>Physik</strong> und Zentrum für Materialwissenschaften, Philipps-Universtät, D-35032 Marburg<br />

We <strong>de</strong>monstrate for the system Ar/Cu(100) how in favourable cases the dynamics of electronic states located at<br />

the interface between a metal and an insulator can be investigated by means of time-resolved two-photon<br />

photoemission (2PPE). The interface states of Ar/Cu are located above the vacuum level in the band gaps of<br />

both the Cu(100) surface and the Ar films which were as thick as 70 monolayers (ML). With increasing layer<br />

thickness the states evolve from quantum-well-like resonances into well-<strong>de</strong>fined bound states which arise from<br />

the screened image-potential of the metal. Electrons excited into these states <strong>de</strong>cay on timescales between<br />

100 fs and 250 fs by electron-hole pair excitation in the metal and - for thin Ar layers ( < 20-30 ML) - also by<br />

electron transfer through the insulating Ar layers into the vacuum. In comparison to the image-potential states of<br />

the clean surface, the interface states are modified by the potential insi<strong>de</strong> the dielectric layers. Screening reduces<br />

25 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

their binding energies with respect to the Ar conduction band and also results in longer lifetimes. The dispersion<br />

of the states is found to be parabolic near the band minimum with an effective mass of 0.5 m e .<br />

O <strong>28</strong>.71 Poster Mi 16:00 Bereich C<br />

Zeit- und energieaufgelöste Untersuchungen <strong>de</strong>s Transports optisch angeregter Elektronen in<br />

Metall-Isolator-Metall-Kontakten<br />

•Sven Schramm 1 , Johannes Schnei<strong>de</strong>r 1 , Walter Pfeiffer 1 und Detlef Diesing 2<br />

1 <strong>Physik</strong>alisches Institut Universität Würzburg, Experimentelle <strong>Physik</strong> 1, 97074 Würzburg<br />

2 Institut für Schichten und Grenzflächen, Forschungszentrum Jülich, 52425 Jülich<br />

Metall-Isolator-Metallkontakte (MIM) bestehen aus zwei Metallelektro<strong>de</strong>n die durch eine dünne Oxidschicht<br />

getrennt sind (Ta-TaO-Ag, Al-Al 2 O 3 -Ag). Sie bil<strong>de</strong>n ein Mo<strong>de</strong>llsystem zur Untersuchung <strong>de</strong>s lichtinduzierten<br />

Elektronentransports durch die Oxid-Barriere. Aufgrund <strong>de</strong>r starken Zunahme <strong>de</strong>r Transmission <strong>de</strong>r<br />

Tunnelbarriere für optisch angeregte Ladungsträger wer<strong>de</strong>n diese nach Anregung mit ultrakurzen Lichtimpulsen<br />

als kurzer Elektronenpuls in die Gegenelektro<strong>de</strong> injiziert. Aufgrund <strong>de</strong>r inhomogenen Anregung kommt es zu<br />

einem resultieren<strong>de</strong>n Photostrom. Ausgehend von <strong>de</strong>n bislang durchgeführten Photostrommessungen [1] wird<br />

dieser Injektionsvorgang nun auch energieaufgelöst untersucht. Hierzu wer<strong>de</strong>n in <strong>de</strong>r Rückelektro<strong>de</strong> <strong>de</strong>s<br />

Kontaktes Elektronen mit einem ultrakurzen Lichtimpuls angeregt und dann durch zeitkorrelierte Photoemission<br />

in <strong>de</strong>r Deckelektro<strong>de</strong> nachgewiesen. Der Nachweis <strong>de</strong>s Injektionstromes hängt stark von <strong>de</strong>n<br />

Anregungsbedingungen und <strong>de</strong>n Barriereneigenschaften ab.<br />

[1] Thon et al., Appl.Phys. A 78 (2004) 189<br />

O <strong>28</strong>.72 Poster Mi 16:00 Bereich C<br />

Time <strong>de</strong>velopment of electronic excitations of CO on MgO(001)<br />

•N.-P. Wang 1 , M. Rohlfing 2 , P. Krüger 1 und J. Pollmann 1<br />

1 Institut für Festkörpertheorie, Universität Münster, Wilhelm-Klemm-Str. 10, 48149 Münster<br />

2 School of Engineering and Science, International University Bremen, P.O. Box 750761, <strong>28</strong>725 Bremen<br />

Femtosecond laser excitation is a very useful tool for acquiring important knowledge about the short-time<br />

dynamics of surface excitations. In this context the fundamental question arises how fast an initially localized<br />

excitation, which is not an eigenstate of the surface system but rather <strong>de</strong>fines the 'initial value' of the<br />

time-<strong>de</strong>pen<strong>de</strong>nt Schrödinger equation, <strong>de</strong>velops in space and time. Here the <strong>de</strong>pen<strong>de</strong>nce of the time <strong>de</strong>cay on the<br />

initial molecular excitation and the electronic spectrum of the substrate surface is of particular interest. We have<br />

studied therefore the dynamics of electronic excitations in a CO adlayer on MgO(001)-(1×1) from first<br />

principles. One-particle excitations of the ground state, <strong>de</strong>scribed within DFT-LDA, are calculated employing<br />

the GW approximation. Two-particle excitations and their optical spectrum are obtained solving the<br />

Bethe-Salpeter equation including electron-hole interaction. The time evolution of the molecular excitation is then<br />

<strong>de</strong>termined from the time-<strong>de</strong>pen<strong>de</strong>nt Schrödinger equation. An initial CO exciton state is found to <strong>de</strong>cay<br />

exponentially within two femto-seconds after coupling the adlayer to the substrate. This is due to a resonance<br />

with charge-transfer excitations between the substrate and the adlayer. Interestingly, the <strong>de</strong>cay of the molecular<br />

exciton is an or<strong>de</strong>r of magnitu<strong>de</strong> faster than the <strong>de</strong>cay of single-particle states.<br />

O <strong>28</strong>.73 Poster Mi 16:00 Bereich C<br />

Ultrafast energy relaxation and transport effects in photoexcited metals and metallic thin films<br />

•Panagiotis Loukakos, Martin Lisowski, Uwe Bovensiepen, Julia Stähler, Cornelius Gahl und Martin Wolf<br />

Fachbereich <strong>Physik</strong>, Freie Universität Berlin, Arnimallee 14, 14195 Berlin<br />

Time-resolved two-photon-photoemission spectroscopy is used to study the femtosecond dynamics of<br />

26 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

photoexcited electrons in bulk Ru(001), Cu(111) and thin Cu(111) films epitaxially grown on Si(111)-7x7. After<br />

excitation with photon energies of 1.5-2.4 eV the time evolution of the non-equilibrium electron population in the<br />

vicinity of the Fermi level is probed by a time-<strong>de</strong>layed UV pulse. For Cu film thicknesses between 6 nm to 44<br />

nm we find that the electron relaxation rates increase monotonically with film thickness, which is attributed to<br />

electron transport out of the probe <strong>de</strong>pth into the bulk. For the electron dynamics at the Ru(001) surface we<br />

observe an unexpectedly fast energy dissipation resulting in a <strong>de</strong>creased temperature at the surface with respect<br />

to predictions of the two-temperature mo<strong>de</strong>l. We attribute this to the influence of the non-thermal electron<br />

distribution. With the aid of numerical calculations we propose an increased (ballistic) transport of<br />

non-thermalized electrons and a <strong>de</strong>creased electron-phonon coupling at the surface to account for the efficient<br />

energy dissipation into the bulk.<br />

O <strong>28</strong>.74 Poster Mi 16:00 Bereich C<br />

Space Charge Effects during Ultrashort Laser Pulse Photoemission Electron Microscopy<br />

•D. Thien, M. Horn-von Hoegen, O. Heinz, P. Zhou, D. von <strong>de</strong>r Lin<strong>de</strong> und F.-J. Meyer zu Heringdorf<br />

Institut für Laser und Plasmaphysik, Universität Duisburg-Essen (Campus Essen), 45117 Essen<br />

Visualization of the dynamics of electronic states in mesoscopic structures requires the simultaneous application<br />

of 3 different tools: Ultrashort fs-laser pulses offer time resolution, spectroscopy allows separation of different<br />

excited electronic states and Photoemission Electron Microscopy (PEEM) provi<strong>de</strong>s the crucial possibility to<br />

study surface areas on the nanoscale. We are currently combining an amplified Ti:Sapphire laser system (40fs<br />

pulses at 1kHz repetition rate), and a PEEM with imaging energy filter (ELMITEC) into a novel pump-probe<br />

experiment. While our laser oscillator (20fs, 80MHz) typically images excited electronic states via 2 Photon<br />

Photoemission, the amplifier system provi<strong>de</strong>s a greatly improved intensity of more than 10 15 W/cm 2 and opens<br />

the door for frequency conversion and photoemission experiments with photon energies of more than 30eV.<br />

The intense ultrashort pulses confine a great number of photoemitted electrons into a small area resulting in<br />

coulomb interaction. Here we analyze these space-charge effects using frequency doubled laser pulses on<br />

patterned in-situ grown low-workfunction Cs-layers on Si and SiO 2 substrates. At high photon flux we observe<br />

that the edges of our Cs-pads appear blurred. Subsequent reduction of the laser peak power leads to sharper<br />

edges as are also observed when the 80MHz oscillator is used for illumination.<br />

O <strong>28</strong>.75 Poster Mi 16:00 Bereich C<br />

Time-of-Flight Two-Photon Photoemission Spectromicroscopy of Noble metal cluster films with<br />

Femtosecond Laser Radiation.<br />

•M. Cinchetti, A. Gloskovskii, D. A. Valdaitsev, S. A. Nepijko und G. Schönhense<br />

Johannes Gutenberg-Universität, Institut für <strong>Physik</strong>, 55099 Mainz, Deutschland<br />

Time-of-Flight Two-Photon Photoemission Spectromicroscopy [1] was used to investigate the photoemission<br />

properties of some Nobel metal surfaces un<strong>de</strong>r femtosecond laser irradiation (photon energy 3.1 eV, pulse width<br />

< 200 fs, laser fluence 6.4 µJcm -2 ).In particular, we present the results of investigations of Cu surface<br />

inhomogeneities and Ag nanoparticle films <strong>de</strong>posited on a Si(111) substrate. The photoemission yield resulted to<br />

be enhanced in presence of surface inhomogeneities with dimensions in the nanometer range. The energy<br />

distribution curves obtained from regions characterized by a strongly enhanced photoemission yield are shown<br />

to have the same qualitative behaviour. They differ significantly from the energy distribution curves from the<br />

homogeneous and clean metal surfaces. The differences are explained in terms of (i) a reduction of surface<br />

potential barrier connected with the appearance of local fields between the nanoparticles and the substrate; (ii)<br />

the excitation of Localized Surface Plasmons in the nanoparticles and the consequent modification of the near<br />

field [2], that influences the photoemission. [1] M. Cinchetti, A. Oelsner, G. H. Fecher, H. J. Elmers, and<br />

G.Schönhense, Appl. Phys. Lett. 83, 1503 (2003). [2] V.M. Shalaev, C. Douketis, T. Haslett, T. Stuckless, and<br />

M. Moskovitis, Phys. Rev. B 53, 11193 (1996).<br />

O <strong>28</strong>.76 Poster Mi 16:00 Bereich C<br />

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

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Time-Resolved Photoemission Electron Microscopy at nanostructured surfaces<br />

•Carsten Wiemann, Michael Bauer, Michael Munzinger, Daniela Bayer und Martin Aeschlimann<br />

TU Kaiserslautern<br />

TR-2PPE (Time-Resolved 2-Photon-Photoemission) is a well-established technique to investigate electron<br />

dynamics at surfaces on a femtosecond time-scale. A combination of TR-2PPE with a spatially resolving<br />

electron <strong>de</strong>tection scheme such as Photoemission Electron Microscopy (PEEM) allows in addition to analyze the<br />

precise local origin of the emitted electrons. In this way a 'lifetime mapping' of heterogeneous samples is - in<br />

principle - possible. [O. Schmidt et al. Appl. Phys. B 74 (2002) 223-227] Recent time-resolved PEEM results on<br />

nanostructured surfaces <strong>de</strong>monstrating the capabilities and limits of this setup in extending time-resolved<br />

spectroscopy to the nanoscale will be presented.<br />

O <strong>28</strong>.77 Poster Mi 16:00 Bereich C<br />

Surface Recombination Dynamics of SiO2/Si(100) - A Combined Laser and Synchro Radiation Study<br />

•David Bröcker 1 , Tatjana Gießel 1 und Wolf Widdra 2<br />

1 Max-Born-Institut, Max-Born-Strasse 2a, 12489 Berlin<br />

2 Martin-Lutter-Universtität Halle-Wittenberg, Fachbereich <strong>Physik</strong>, Fachgruppe Experimentelle <strong>Physik</strong> III<br />

The charge carrier dynamics at the silicon surface has been studies by probing the surface photovoltage. Upon<br />

excitation of electron hole pairs in the surface-near region by picosecond laser pulses, the dynamics of the<br />

charge carrier recombination has been <strong>de</strong>termined by time-resolved Si 2p core level photoemission. We<br />

compared several sample preparations, the clean Si(100) surface, the hydrogen monohydri<strong>de</strong>, and thin oxi<strong>de</strong><br />

layers. The <strong>de</strong>cay process could be <strong>de</strong>scribed by a mo<strong>de</strong>l based on thermionic emission. The influence of the<br />

laser fluence and the temperature on the <strong>de</strong>cay process has been studied in <strong>de</strong>tail.<br />

O <strong>28</strong>.78 Poster Mi 16:00 Bereich C<br />

X-ray longitudinal Kerr rotation and ellipticity spectra measured at the 2p edges of Fe, Co, and Ni<br />

•Sergio Valencia 1 , Hans-Christoph Mertins 1 , Peter M. Oppeneer 2 , Dirk Abramsohn 1 , Andreas Gaupp 1 und<br />

Wolfgang Gudat 1<br />

1 BESSY, Berlin<br />

2 IFW Dres<strong>de</strong>n<br />

The first measurements of the X-ray longitudinal magneto-optical Kerr effect (L-MOKE) at the 2p absorption<br />

edges of amorphous Fe, Co, and Ni films are reported. The L-MOKE rotation and ellipticity spectra are<br />

recor<strong>de</strong>d by a complete polarization analysis of the X-rays reflected from the ferromagnetic surface. At the<br />

edges large Kerr rotations of up to ?24 ? are <strong>de</strong>tected, which are more than two or<strong>de</strong>rs of magnitu<strong>de</strong> larger than<br />

those in the visible energy range. Using a numerical simulation package based on the magneto-optical refractive<br />

indices, the spectral contributions stemming from magneto-optically active atomic transitions could be seperated<br />

from layer interference effects. Both theoretically and experimentally it is shown that at grazing inci<strong>de</strong>nce the<br />

longitudinal Kerr rotation and Kerr ellipticity are proportional to the transversal MOKE and the XMCD reflection<br />

spectrum, respectively.<br />

O <strong>28</strong>.79 Poster Mi 16:00 Bereich C<br />

Magnetische Röntgenstreuung an lateralen Strukturen<br />

•Arndt Remhof, Johannes Grabis, Alexei Nefedov, Erik Verduijn und Hartmut Zabel<br />

Experimentalphysik/Festkörperphysik, Ruhr-Univeristät Bochum, 44780 Bochum<br />

<strong>Nano</strong>- und Mikrostrukturierung von dünnen magnetischen Systemen ermöglicht das<br />

<strong>28</strong> of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Ummagnetisierungsverhalten, d. h. die Hystereseschleife, gezielt zu verän<strong>de</strong>rn. Wir haben ein quadratisches<br />

Muster aus Co/CoO Inseln mittels Elektronenstrahl-Lithographie hergestellt. Die Inseln haben einen<br />

Durchmesser von 1mm und eine Perio<strong>de</strong> von 2,5 mm. Die magnetische Hysterese wur<strong>de</strong> mit Bragg-MOKE und<br />

mit resonanter magnetischer Röntgenstreuung (XRMS) an <strong>de</strong>r Co L 2,3 bei verschie<strong>de</strong>ner Ordnung <strong>de</strong>r<br />

Interferenz bestimmt. Bragg-MOKE liefert eine Fourieranalyse <strong>de</strong>s Magnetisierungsprofils während <strong>de</strong>s<br />

Ummagnetisierungsprozesses. Analog dazu liefern auch Hysteresen, die mit XRMS an verschie<strong>de</strong>nen Ordnungen<br />

von Bragg-Reflexen gemessen wer<strong>de</strong>n, eine Fourieranalyse <strong>de</strong>r Ummagnetisierung. Im Vergleich zu<br />

Bragg-MOKE zeichnet sich XRMS durch Elementspezifität und durch höhere Eindringtiefen aus. Wir<br />

präsentieren erste Ergebnisse, die mit Bragg-MOKE und XRMS an strukturierten Co/CoO Proben gewonnen<br />

wur<strong>de</strong>n, und vergleichen die Ergebnisse.<br />

Geför<strong>de</strong>rt durch SFB 491.<br />

O <strong>28</strong>.80 Poster Mi 16:00 Bereich C<br />

Faraday rotation spectrum at shallow core levels: 3p edges of Fe, Co, and Ni<br />

•Sergio Valencia 1 , Hans-Christoph Mertins 2 , Peter M. Oppeneer 3 , Dirk Abramsohn 1 , Andreas Gaupp 1 , Claus M.<br />

Schnei<strong>de</strong>r 4 und Wolfgang Gudat 1<br />

2 FH Münster<br />

3 IFW Dres<strong>de</strong>n<br />

4 IFF, FZ Jülich<br />

1 BESSY, Berlin<br />

We report measurements of the Faraday effect at the 3p edges of thin Fe, Co, and Ni films. The Faraday<br />

rotation and ellipticity are <strong>de</strong>termined by a complete polarization analysis of the synchrotron radiation transmitted<br />

across the samples. Surprisingly, the rotation constants k attain large values comparable to those observed at the<br />

2p edges. Maximal rotation constants of 2.2 ·10 5 , 1.5 ·10 5 , and 0.8 ·10 5 <strong>de</strong>g/mm are found for Fe, Co, and Ni,<br />

respectively. While at the 2p edges the spin-orbit splitting of the 2p levels is consi<strong>de</strong>red to be mainly responsible<br />

for the magneto-optical effects, the unexpected similarity un<strong>de</strong>rlines the role of the exchange-splitting of the 3p<br />

core levels in the extreme ultra-violet region (EUV). A full set of optical and magneto-optical constants, which<br />

were <strong>de</strong>termined from the measured rotation and ellipticity, are presented for the three elements in the energy<br />

range of the 3p edges.<br />

O <strong>28</strong>.81 Poster Mi 16:00 Bereich C<br />

Anomalous ferromagnetism of monatomic Co wire at the Pt(111) surface step edge<br />

•Peter M. Oppeneer 1 , Alexan<strong>de</strong>r B. Shick 2 und Frantiek Máca 2<br />

1 IFW Dres<strong>de</strong>n<br />

2 Inst. of Physics, ASCR, Prague<br />

We report a first-principles investigation of the anomalous ferromagnetism of a quasi-one-dimensional Co chain<br />

<strong>de</strong>corating the Pt(111) step edge. Our calculations <strong>de</strong>monstrate that the symmetry breaking at the Pt step leads<br />

to an easy magnetization axis at an anomalous angle of ∼ 20 ? towards the Pt step, in semi-quantitative agreement<br />

with the experimentally observed peculiar easy axis at an angle of ∼ 40 ? [P. Gambar<strong>de</strong>lla et al., Nature 416, 301<br />

(2002)]. The computed hard magnetization axis direction also corresponds well to the experimentally observed<br />

hard axis. A (T = 0) magnetocrystalline anisotropy energy of 3 meV/Co is calculated in good agreement with the<br />

experimental value of ∼ 2 meV/Co at T = 45 K. On account of the symmetry breaking the Co spin and orbital<br />

moments become noncollinear, even in the case of a collinear ferromagnetic spin arrangement. We also<br />

performed LSDA+U calculations, with which a significant enhancement of the Co orbital magnetic moment is<br />

achieved already when mo<strong>de</strong>st electron correlations (small U) are taken into account.<br />

O <strong>28</strong>.82 Poster Mi 16:00 Bereich C<br />

29 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Transverse magneto-optical Kerr effect at the 3p edges of Fe and Co<br />

•Armin Kleibert 1 , Sergio Valencia 2 , Hans-Christoph Mertins 2 und Joachim Bansmann 1<br />

1 Universität Rostock, Fachbereich <strong>Physik</strong>, Universitätsplatz 3, 18051 Rostock<br />

2 BESSY GmbH, Albert-Einstein-Str. 15, 12489 Berlin, Germany<br />

Soft x-ray based experimental techniques are powerful and very sensitive methods to investigate the magnetism<br />

of systems with low dimensions like ultrathin films or clusters, respectively. In particular, the magneto-optical<br />

Kerr-effect (MOKE) at the 2p edges of Fe, Co, and Ni has attracted much attention. In the transverse geometry<br />

(T-MOKE) huge intensity changes in the resonantly enhanced reflectivity upon reversal of the magnetization<br />

direction have been found. While effects near the 2p core levels were extensively studied in the last years, only a<br />

few experiments were reported concerning the vicinity of the 3p threshold.<br />

In this contribution, we present angular <strong>de</strong>pen<strong>de</strong>nt measurements of the T-MOKE in the energy range of the 3p<br />

edges of thin Fe and Co films, respectively, revealing surprisingly large asymmetries up to 40% near the<br />

Brewster angle. From these reflectivity measurements it is possible to obtain information about the energy<br />

<strong>de</strong>pen<strong>de</strong>nt refractive indices and magneto-optical Voigt constants. In or<strong>de</strong>r to simulate the measured reflectivity<br />

including the influence of capping layers we applied a multilayer formalism <strong>de</strong>scribing magneto-optics. A good<br />

agreement of calculation and experiment was achieved using tabulated values of the in<strong>de</strong>x of refraction and<br />

in<strong>de</strong>pen<strong>de</strong>ntly obtained Voigt constants.<br />

O <strong>28</strong>.83 Poster Mi 16:00 Bereich C<br />

Resonant X-Ray scattering from TbBaCo 2 O 5.5<br />

•N.V. Kasper 1 , P. Wochner 1 , G. Carbone 1 , A. Vigliante 2 , D. Mannix 3 und G. Jakob 4<br />

4 Institut für <strong>Physik</strong>, Universität Mainz, Mainz, Germany<br />

1 Max-Planck-Institut für Metallforschung, Stuttgart, Germany<br />

2 Bruker AXS, Karlsruhe, Germany<br />

3 European Synchrotron Radiation Facility, Grenoble, France<br />

Resonant X-ray scattering at the Co K-edge from epitaxial films and single crystals of TbBaCo 2 O 5.5 cobaltite<br />

with perovskite structure has been studied in insulating and metallic states. Polarization, energy and azimuthal<br />

<strong>de</strong>pen<strong>de</strong>nces of the intensity of (016), (116), and (310) Bragg peaks were measured. Strong oscillations of the<br />

resonantly scattered intensity were observed both in σ' and π' channels. The scattered signal changes very<br />

weakly during the metal-insulator phase transition.<br />

The azimuthal oscillations of the scattered signal are attributed to the tensor character of the anomalous<br />

scattering factor of Co. Using this concept we have <strong>de</strong>veloped a mo<strong>de</strong>l, <strong>de</strong>scribing very well the measured<br />

azimuthal oscillations. On the basis of the obtained experimental results and literature data it is argued that this<br />

anisotropy of the anomalous scattering factor of Co is caused mainly by distortions of the local surrounding of<br />

cobalt ions and not by anisotropies due to or<strong>de</strong>ring of electronic orbitals of Co.<br />

O <strong>28</strong>.84 Poster Mi 16:00 Bereich C<br />

X-ray magneto-optical sum rules in small Co clusters<br />

•Kai Fauth 1,2 , Markus Heßler 1,2 und Gisela Schütz 2<br />

1 <strong>Physik</strong>alisches Institut <strong>de</strong>r Universität Würzburg, Am Hubland, 97074 Würzburg<br />

2 MPI für Metallforschung, Heisenbergstraße 3, 70569 Stuttgart<br />

The so-called spin and orbital sum rules [1,2] in x-ray magnetic circular dichroism (XMCD) spectroscopy are<br />

often believed to apply with reasonable accuracy in the case of the late 3d transition metals and their<br />

compounds, if the magnetic dipole term T z can be neglected. Strong <strong>de</strong>viations can occur due to symmetry<br />

breaking such as given at surfaces, causing the magnetic dipole term to contribute significantly to the spin sum<br />

30 of 32 07.06.2009 22:14


<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

rule, while not contributing to the magnetization. Much less is known in the case of small clusters. We have<br />

<strong>de</strong>rived magnetic moments of superparamagnetic Co 55 clusters from XMCD at various applied magnetic fields.<br />

We find that the moments thus obtained from the magnetization curve and those <strong>de</strong>termined separately from the<br />

sum rules agree to within 10%. This result sets an upper limit for the importance of T z in these clusters.<br />

[1] B. T. Thole et al. , Phys. Rev. Lett. 68, 1943 (1992)<br />

[2] P. Carra et al. , Phys. Rev. Lett. 70, 694 (1993)<br />

O <strong>28</strong>.85 Poster Mi 16:00 Bereich C<br />

X-ray resonant magnetic scattering of Fe/Cr superlattices<br />

•Alexei Nefedov, Johannes Grabis, Andre Bergmann, Florin Radu und Hartmut Zabel<br />

Institut für Experimentalphysik/Festkörperphysik, Ruhr-Universität Bochum, D-44780 Bochum, Germany<br />

We have studied the magnetic and structural properties of an antiferromagnetically (AF) coupled Fe/Cr(001)<br />

superlattice by soft X-ray resonant magnetic scattering. Strong magnetic Bragg peaks are observed at the half<br />

or<strong>de</strong>r positions in reciprocal space parallel to the [001] growth direction and in between the structural Bragg<br />

reflections from the superlattice periodicity. The magnetic hysteresis loops measured at the structural Bragg<br />

peak and at the half-or<strong>de</strong>r peak clearly <strong>de</strong>monstrate the AF coupling of the Fe/Cr multilayer. Transverse scans<br />

and off-specular reflectivity measurements confirm an AF domain structure of the superlattice in remanence<br />

with large perpendicular correlation. In addition, the transverse scan of the half-or<strong>de</strong>r Bragg peak exhibits a<br />

Lorentzian line shape at zero field, which diminishes in higher fields, indicative for a remanent multidomain state<br />

which approaches a single domain state towards saturation.<br />

This work was supported by the German Fe<strong>de</strong>ral Ministry of Education and Research (BMBF) un<strong>de</strong>r Contract<br />

No.03ZAE7BO.<br />

O <strong>28</strong>.86 Poster Mi 16:00 Bereich C<br />

Inducing spin crossover in metallo-supramolecular polyelectrolytes through an amphiphilic phase<br />

transition<br />

•Yves Bo<strong>de</strong>nthin 1 , U. Pietsch 1 , D. Kurth 2 und H. Möhwald 2<br />

1 University of Potsdam, Institute of Physics, Am Neuen Palais 10, 14469 Potsdam, Germany<br />

2 MPI-KG Golm, Am Mühlenberg 1, 14476 Potsdam-Golm<br />

In the last years resonant magnetic X-ray reflectivity experiments (XMCD) become important for the<br />

investigation of molecular magnetism in thin films.<br />

In the present work we report a novel approach to affect spin crossover by introducing mechanical strain<br />

through an amphiphilic phase transition in a metallo-supramolecular polyelectrolyte-amphiphile complex (PAC).<br />

The investigated system consists of thin layers <strong>de</strong>posited in Y-conformation on a silicon substrate by means of<br />

Langmuir-Blodgett technique.<br />

It was observed by EXAFS, x-ray reflectivity and in-plane diffraction experiments that the structural phase<br />

transition in the amphiphilic mesophase is responsible for the distortion of the coordination geometry of the<br />

tightly coupled transition metal centres. Consequently, the energetic separation of the subsets of the iron<br />

d-orbitals changes and gives rise to spin crossover. Using temperature resolved SQUID and XMCD<br />

measurements we observe a diamagnetic to paramagnetic phase transition above room temperature which is<br />

connected to a structural phase transition between two liquid crystalline phases.<br />

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