Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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-