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Plenarvorträge - DPG-Tagungen

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Magnetismus Montag<br />

MA 8.7 Mo 17:15 H22<br />

Magnetic and elastic properties of YCo5 under pressure —<br />

•Daniela Koudela 1 , Ingo Opahle 1 , Manuel Richter 1 , Klaus<br />

Koepernik 1 , Ulrike Nitzsche 1 , Helge Rosner 2 , Michael<br />

Kuzmin 3 , and Helmut Eschrig 1 — 1 IFW Dresden, PF 270116, 01171<br />

Dresden — 2 MPI-cPfS Dresden, Nöthnitzer Straße 40, 01187 Dresden<br />

— 3 Instituto de Ciencia de Materiales de Aragon, Zaragoza; Spain<br />

We computed the total energy and the magnetic moment of YCo5<br />

in dependence of the lattice parameters. Our calculations are based on<br />

density functional theory in the local spin density approximation. In accordance<br />

with earlier calculations of Yamada et al. [J. Phys.: Condens.<br />

Matter 11 (1999) 483] we find a transition from high spin to low spin under<br />

applied pressure. On the other hand our calculations show a strong<br />

dependence of the magnetic moment on volume in the low spin state close<br />

to the transition volume not observed by the previous authors. This is<br />

connected with a change in the bulk modulus from about 200 GPa to 60<br />

GPa at the transition, which takes place at a pressure of about 9 GPa.<br />

The calculations were done with the full-potential local-orbital method<br />

(FPLO).<br />

MA 8.8 Mo 17:30 H22<br />

Magnetismus und elektronische Struktur von Gadolinium<br />

— •C. Santos 1 , V. Eyert 2 und W. Nolting 1 — 1 Lehrstuhl<br />

Festkörpertheorie, Institut für Physik, Humboldt-Universität zu Berlin<br />

— 2 Institut für Physik, Theoretische Physik II, Universität Augsburg<br />

Durch Kombination einer vielteilchentheoretischen Auswertung des<br />

Kondo-Gitter-Modells mit einer ,,ab initio“ Bandstrukturrechnung bestimmen<br />

wir sowohl die temperaturabhängige elektronische Struktur als<br />

MA 9 Hauptvortrag Demokritov<br />

auch die magnetischen Eigenschaften von HCP-Gadolinium. Das Vielteilchenproblem<br />

wird mit der in Phys. Rev. B 65 144419 vorgestellten Green-<br />

Funktion-Theorie behandelt. Diese haben wir auf das Mehrband-Kondo-<br />

Gitter Modell erweitert und anschließend mit einer ASW-Bandstruktur<br />

kombiniert, wobei Doppelzählung von relevanten Wechselwirkungen vermieden<br />

werden konnte. In diesem Beitrag werden Ergebnisse der selbstkonsistent<br />

berechneten Curie-Temperatur TC, der Magnetisierung 〈S z 〉<br />

und der temperaturabhängigen Quasiteilchen-Bandstruktur vorgestellt.<br />

Es ergibt sich eine fast quantitative Übereinstimmung mit experimentellen<br />

Daten.<br />

MA 8.9 Mo 17:45 H22<br />

Structure and Magnetism of Light Actinides and Their Compounds:<br />

Theorie — •Manuel Richter, Ingo Opahle, Ulrike<br />

Nitzsche, Klaus Koepernik, and Helmut Eschrig — IFW Dresden,<br />

PF 270116, D-01171 Dresden<br />

Structural and magnetic properties of actinides and actinide compounds<br />

are much influenced by spin-orbit interaction and other relativistic<br />

effects. By means of the recently developed fully relativistic fullpotential<br />

local-orbital (R-FPLO, [1]) scheme, we have evaluated equilibrium<br />

volume, bulk modulus, and structural energies of light actinide<br />

metals in the framwork of the local density approximation. In particular,<br />

we find evidence for the existence of a hexagonal Uranium phase<br />

in thin films on W(110) and for the possible existence of cubic Protactinium.<br />

Using the local spin density approximation with orbital polarization<br />

corrections, the magnetic properties of cubic Uranium Sulfide are<br />

investigated.<br />

[1] http://www.ifw-dresden.de/FPLO/<br />

Zeit: Dienstag 09:30–10:00 Raum: H10<br />

Hauptvortrag MA 9.1 Di 09:30 H10<br />

Experimental observation of symmetry breaking soliton modes<br />

in an active ring — •Sergej O. Demokritov 1 , Alexander<br />

A. Serga 1 , Vladislav E. Demidov 1 , Burkard Hillebrands 1 ,<br />

Michail P. Kostylev 2 und Boris A. Kalinikos 2 — 1 Fachbereich<br />

Physik, Technische Universitaett Kaiserslautern, Erwin-Schroedinger-<br />

Strasse 56, 67663 Kaiserslautern, Germany — 2 St. Petersburg Electrotechnical<br />

University, 197376 St. Petersburg, Russia<br />

Solitons are large-amplitude, spatially confined wave packets in nonlinear<br />

media. A unique feature is their propagation without a change in<br />

shape owing to the stabilizing effect of the nonlinearity. We report on the<br />

first experimental study of solitons in an active ring and their novel pro-<br />

MA 10 Exchange Bias<br />

perties due to phase quantization [1]. As a model system, we constructed<br />

an active nonlinear ring based on spin-wave propagation in a magnetic<br />

film. To address individually each eigen-mode of the ring a newly developed<br />

mode selecting mechanism based on phase sensitive amplification<br />

has been used. Several novel symmetry-breaking soliton-like modes are<br />

found, such as Möbius solitons, which break the fundamental symmetry<br />

of 2p-periodicity in the phase change acquired per loop: a Möbius soliton<br />

needs to travel twice around the ring to meet the initial phase condition.<br />

A phase sensitive interaction between soliton-like modes has been discovered.<br />

This interaction provides the phase correlation between two travelling<br />

solitons if their distance is decreasing. [1] S.O. Demokritov et al.<br />

Nature 426, 159 (2003).<br />

Zeit: Dienstag 10:15–13:00 Raum: H10<br />

MA 10.1 Di 10:15 H10<br />

Exchange coupling in thin Fe-films on NiO(001) — •U. Mick,<br />

W. G. Park, V. Bocatius, H. Meinert, and E. Kisker — Institut<br />

für Angewandte Physik, Universität Düsseldorf<br />

The domain formation and exchange coupling of thin Fe-Films on<br />

NiO(001) have been investigated by x-ray magnetic linear dichroism<br />

(XMLD) and x-ray magnetic circular dichroism (XMCD) in photoemission<br />

electron microscopy (PEEM).<br />

In-situ cleaved NiO crystals provide atomically defined clean NiO(001)surfaces<br />

as is shown in complementary STM-measurements. Thin Fe-films<br />

grown by MBE at room temperature on these NiO(001)-surfaces exhibit<br />

a collinear coupling of their magnetic moments to the spin structure of<br />

by the NiO(001)-substrate as is revealed in angular dependent PEEMmeasurements.<br />

Fe-films grown on freshly cleaved NiO(001) can induce<br />

changes in the NiOs AF-domains, which are presumably thermodynamically<br />

unstable. Thermally relaxed NiO(001) surfaces, that have been annealed<br />

above Neel-temperature, show a rearrangement in their domain<br />

structure that is not altered by subsequent deposition of Fe anymore while<br />

the Fe-films still show collinear coupling after the onset of FM-coupling,<br />

as has been investigated for different film thicknesses of Fe from 1 ML to<br />

15 ML.<br />

Neither x-ray absorption spectroscopy (XAS) nor PEEM-investigations<br />

on Ni-MCD gave any evidence for significant interface reactions between<br />

the Fe-films grown at room temperature and the NiO substrate.<br />

This work has been performed at BESSY-UE52 and was supported by<br />

the BMBF under grant No. 05KS1PFB/1<br />

MA 10.2 Di 10:30 H10<br />

Soft X-ray Resonant Magnetic Scattering studies on CoO/Fe<br />

exchange bias bilayers — •Florin Radu, Gregor Nowak, Johannes<br />

Grabis, Alexei Nefedov, and Hartmut Zabel — Experimentalphysik/Festkoerperphysik,<br />

Ruhr-Universitaet Bochum, 44780<br />

Bochum, Germany<br />

We have used the ALICE diffractometer and soft X-ray Resonant Magnetic<br />

Scattering (XRMS) techniques to search for the presence of an effective<br />

ferromagnetic moment in an antiferromagnetic (AF) layer which<br />

is in close contact with a ferromagnetic (F) layer. Using rf-sputtering we<br />

have prepared two samples in a single run: one is a CoO(25 ˚A)/Fe(150<br />

˚A) exchange bias system and the other is a single CoO(25 ˚A) AF layer<br />

deposited on a sapphire substrate. The samples were cooled in a field of<br />

+2000 Oe from above the TN=291 K of the CoO AF layer to T=30 K.<br />

Taking advantage of the element specificity of the XRMS technique, we<br />

have measured hysteresis loops of both Fe and CoO layers. The result is<br />

that a single layer of CoO deposited on a substrate shows no ferromagnetic<br />

signal while for the CoO layer deposited on the Fe ferromagnetic<br />

layer we observe hysteresis loops. From these measurements we conclude

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