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Plenarvorträge - DPG-Tagungen

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Magnetismus Dienstag<br />

in der Schichtebene führt. Bei den Fe-Schichten tritt die Austauschanisotropie<br />

überraschenderweise nicht auf. Die Effekte werden an Hand von<br />

detaillierten Magnetisierungsmessungen diskutiert<br />

[1] B. Sass et al., submitted to J. Phys. C<br />

MA 13.55 Di 15:00 Bereich A<br />

Magneto-Transport Properties of Multilayer Antidot Arrays<br />

— •Kornelius Nielsch, Fernando J. Castaño, and Caroline<br />

A. Ross — Department of Materials Science and Engineering, Massachusetts<br />

Institute of Technology, Cambridge, MA, USA<br />

The magneto-transport properties of Pseudo-spin-valve (PSV) thin<br />

film structures grown onto sub-200 nm porous alumina templates have<br />

been investigated. Hexagonal and quadratic pore arrangements were<br />

achieved by defining a grid in silicon substrates using a combination<br />

of interference lithography and reactive ion etching. An aluminum layer<br />

was then evaporated and anodized, resulting in large area porous structures<br />

with interpore distance of 180 nm (quadratic lattice) and 208 nm<br />

(hexagonal lattice) and a pore diameter ranging from 80 to 150 nm. The<br />

PSV antidot arrays were fabricated by depositing NiFe/Cu/CoFe thin<br />

film structures onto the alumina templates. The room temperature hysteresis<br />

loops of the antidot structures show the distinct switching of both<br />

soft and hard magnetic layers, as well as a significant shearing of the<br />

loop, as compared with that of the PSV thin film structure on a Si substrate.<br />

Magnetic anisotropies induced by the different arrangements will<br />

be discussed. Surprisingly the giant magnetoresistance ratio of the PSV<br />

antidot arrays is only slightly smaller than that of the PSV thin film<br />

structure.<br />

MA 13.56 Di 15:00 Bereich A<br />

Interlayer exchange coupling of magnetic rare-earth thin films<br />

— •J.E. Prieto, K. Döbrich, O. Krupin, F. Heigl, G. Kaindl,<br />

and K. Starke — Institut für Experimentalphysik, Freie Universität<br />

Berlin, Arnimallee 14, 14195 Berlin<br />

Exchange coupling between magnetic layers determines the properties<br />

of magnetic heterostructures. Magnetic moments in rare-earth metals<br />

are strongly localized and couple only indirectly through the conduction<br />

electrons. In the case of magnetic films separated by nonmagnetic spacer<br />

layers, the thickness and electronic structure of the latter determine the<br />

sign and magnitude of the coupling. We have studied epitaxial Gd/Y/Tb<br />

trilayers on W(110) element-specifically by means of x-ray magnetooptical<br />

Kerr effect (XMOKE) performed at the M4,5 absorption thresholds<br />

of Gd and Tb. The two magnetic rare-earth films have different coercivities.<br />

For applied magnetic fields smaller than the Tb coercivity, shifted<br />

Gd hysteresis curves are observed. A strong dependence of this exchange<br />

bias on the thickness of the Y spacer layer as well as on the temperature<br />

is found.<br />

MA 13.57 Di 15:00 Bereich A<br />

Transition rates via Bethe ansatz for the XXZ and the XX<br />

chain — •Daniel Biegel 1 , Michael Karbach 1,2 , Gerhard<br />

Müller 2 , and Klaus Wiele 1 — 1 Bergische Universität Wuppertal,<br />

Fachbereich Mathematik und Naturwissenschaften, Physik, 42097<br />

Wuppertal — 2 Department of Physics, University of Rhode Island,<br />

Kingston, RI 02881-0817, USA<br />

As part of a study that investigates the dynamics of the s = 1<br />

2 XXZ<br />

model in the planar regime |∆| < 1, we discuss the singular nature of<br />

the Bethe ansatz equations for the case ∆ = 0, i.e. the XX model. We<br />

identify the general structure of the Bethe ansatz solutions for the entire<br />

XX spectrum, which include states with real and complex magnon momentas.<br />

We present determinantal expressions for transition rates of spin<br />

fluctuation operators between Bethe wave functions. As an application,<br />

we calculate lineshapes for dynamic structure factors relevant for experiments.<br />

The predominant excitations are identified within the framework<br />

of quasiparticles excited from a corresponding vacuum.<br />

MA 13.58 Di 15:00 Bereich A<br />

Generation of ultrashort current pulses with photoconductive<br />

switches — •S. Bretschneider 1 , A. Parge 1 , J. Seeger 2 , T.<br />

Salditt 2 , A. Förster 3 , and M. Münzenberg 1 — 1 IV. Phys. Inst.<br />

Universität Göttingen — 2 Inst. für Röntgenphysik Universität Göttingen<br />

— 3 Inst. für Schichten und Grenzflächen (ISG1) Forschungszentrum<br />

Jülich<br />

Ultra short current pulses can be generated by excitation of a photoconductive<br />

switch with fs-laser pulses from a TiSa-laser system. As material<br />

for the switches we use low temperature grown GaAs (LT-GaAs).<br />

Due to the short carrier life time in LT-GaAs current pulses of the optical<br />

switches are in the ps-time scale. It is shown how to prepare the<br />

switches with ebeam- and optical lithography and how to characterize<br />

the current pulses with auto correlation and photoconductive sampling<br />

techniques. In the future these current pulses will be used to study the<br />

magnetization dynamics of magnetic micro- and nanostructures which is<br />

for example important for magnetic switching in MRAM-elements.<br />

MA 13.59 Di 15:00 Bereich A<br />

Simulation of ultrafast dynamics in all optical pump probe experiments<br />

on nanoscale Permalloy elements — •G. Eilers and<br />

M. Münzenberg — IV. Phys. Inst., Universität Göttingen<br />

Nano-size ferromagnetic structures are of strong interest for future high<br />

speed magnetic random access memory and ultra high density magnetic<br />

storage. Magnetic precession Eigen modes depending on the length/width<br />

ratio of rectangular nanostructures of Permalloy are studied using the<br />

Landau-Lifshitz-Gilbert equation. Aim is to investigate the limits of precessional<br />

switching speed in the limit of smallest sized elements.<br />

Demagnetization effects observed in all optical pump probe experiments<br />

with ultrafast Ti:Sapphire lasers still lacks the theoretical background:<br />

electrons are excitated by a pump laser pulse and a subsequent<br />

demagnetization of the spin system in the order of 5% is observed. We<br />

used a demagnetization effect of a laser spot in between 5 to 100 %<br />

in lateral ferromagnetic thin films and nanostructured rectangular ferromagnetic<br />

elements in our simulations. Magnetization dynamics in the<br />

ps to ns range is compared to precession modes observed in all optical<br />

pump probe experiments. For the simulation the oommf micromagnetic<br />

simulation tool is used.<br />

MA 13.60 Di 15:00 Bereich A<br />

Multiples Schaltverhalten von Nanoleiterbahnen komplexer<br />

Geometrie — •Mario Brands 1 , Britta Hausmanns 2 und<br />

Günter Dumpich 1 — 1 Experimentalphysik, AG Farle, Institut für<br />

Physik, Fakultät IV, Universität Duisburg-Essen, Standort Duisburg,<br />

Lotharstrasse 1, 47048 Duisburg — 2 AG Magnetismus, Fachbereich<br />

Physik, Technische Universität Kaiserslautern, Erwin-Schrödinger-Str.<br />

56, 67663 Kaiserslautern<br />

Es wurden Widerstandsmessungen an dünnen Kobalt-Leiterbahnen bei<br />

einer Temperatur von T = 4, 2K und in einem äußeren Magnetfeld von<br />

bis zu B = 4, 5T durchgeführt. Die Leiterbahnen wurden mittels eines<br />

Zwei-Schritt-Elektronenstrahllithografie (EBL)-Prozesses auf GaAs Substraten<br />

hergestellt und haben eine konstante Länge von l = 400µm wohingegen<br />

ihre Breite (w = 100nm bis w = 2000nm) und ihre Schichtdicke<br />

(t = 7nm bis t = 32nm) systematisch variiert wurde. Zum Schutz vor<br />

Oxidation wurden die Leiterbahnen in-situ mit einer t = 2nm dicken Platinschicht<br />

abgedeckt. Der Magnetowiderstand (senkrecht, out-of-plane)<br />

ist negativ und kann im wesentlichen auf den Anisotropen Magnetowiderstand<br />

(AMR) zurückgeführt werden. In longitudinaler Geometrie werden<br />

bei geringen Magnetfeldern (Bsw ≈ 100mT) charakteristische Peaks<br />

im Magnetowiderstand beobachtet, die den Ummagnetisierungsprozess<br />

einzelner Leiterbahnabschnitte charakterisieren. Auf der Basis dieser Ergebnisse<br />

wird das Auftreten von Domänenwandwiderstandsbeiträgen diskutiert.<br />

Diese Arbeit wird gefördert von der DFG im Rahmen des SFB 491.<br />

MA 13.61 Di 15:00 Bereich A<br />

Inductive time-domain measurement of magnetization dynamics<br />

in epitaxial Fe1−xCox-films — •Tobias Martin, B. Becker, S.<br />

Ganzer, T. Hagler, W. Kipferl, M. Sperl, and G. Bayreuther<br />

— Institut für Experimentelle und Angewandte Physik, Universität Regensburg,<br />

93040 Regensburg<br />

For the development of faster memory-technologies, it is important to<br />

study the magnetization dynamics in thin magnetic films.<br />

Here, the precessional motion of the magnetization is excited by a<br />

fast magnetic field step or pulse with a risetime of about 70ps, which is<br />

produced by a current guided through a coplanar waveguide. The precession<br />

of the magnetization induces a signal in the same or in a second<br />

waveguide, which is detected by a digital sampling oscilloscope with a<br />

bandwidth of 20 Ghz.<br />

This setup is used to investigate the magnetization precession in epitaxially<br />

grown Fe1−xCox-films. The film and the waveguide are brought into<br />

close proximity thus allowing for simple changing of samples and pulsefield<br />

angle. The magnetization dynamics, i.e. precessional frequency and<br />

damping coefficient, are determined for different values of the uniaxial<br />

and fourfold magnetic anisotropies, which can be controlled by the thick-

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