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Deutsche Tagung f ¨ur Forschung mit ... - SNI-Portal

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Magnetismus Vortrag: Mi., 17:40–18:00 M-V13<br />

Time, layer, and spatially resolved magnetic domain imaging of layered<br />

magnetic structures by x-ray magnetic circular dichroism photoelectron<br />

emission microscopy<br />

Wolfgang Kuch 1 , Keiki Fukumoto 1 , Jan Vogel 2 , Julio Camarero 3 , Fabien<br />

Romanens 2 , Stefania Pizzini 2 , Marlio Bonfim 2 , Jürgen Kirschner 4<br />

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

Berlin – 2 Laboratoire Louis Neel, CNRS, 25 avenue des Martyrs, F-38042 Grenoble,<br />

France – 3 Universidad Autónoma de Madrid, E-28049 Madrid, Spain – 4 Max-Planck-<br />

Institut für Mikrostrukturphysik, Weinberg 2, D-06120 Halle<br />

Magnetic structures consisting of ferromagnetic layers separated by ultra-thin nonmagnetic<br />

spacer layers exhibit many new and interesting effects. The fundamental<br />

investigation of the magnetization dynamics of such layered magnetic structures calls<br />

for a method capable of delivering microscopic magnetic information about each of<br />

the magnetic layers separately. X-ray magnetic circular dichroism photoelectron emission<br />

microscopy (XMCD-PEEM) is such a technique. It combines the layer-resolved<br />

visualization of magnetic domain patterns at surfaces and in buried layers with a timeresolved<br />

stroboscopic measurement of the magnetization reversal dynamics, taking advantage<br />

of the time structure of the synchrotron radiation. Using this time-resolved,<br />

layer-selective microscopic technique we observed evidence for the importance of a local<br />

magnetic interlayer coupling mediated by magnetostatic stray fields emanating from<br />

domain walls. During the fast magnetization reversal, stray fields from domain walls<br />

in the hard magnetic layer can lead to a locally enhanced domain nucleation and thus<br />

to a faster switching of the soft magnetic layer. The images show furthermore that<br />

the speed of domain wall motion is influenced by the domain wall energy, leading to<br />

a lower velocity when domains are small. This becomes apparent as a delay in the<br />

nucleation of reversed domains.

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