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Magnetismus Vortrag: Fr., 09:40–10:00 F-V52<br />

Exchange bias instability in a bi-layer with an ion beam imprinted stripe<br />

pattern of FM/AFM interfaces<br />

K. Theis-Bröhl 1 , B.P. Toperverg 1 , M. Wolff 1 , H. Zabel 1 , U. Rücker 2<br />

1 Department of Physics, Ruhr-University Bochum, D-44780 Bochum – 2 Institut für<br />

Festkörperforschung, <strong>Forschung</strong>szentrum Jülich GmbH, D-52425 Jülich<br />

We have investigated the magnetization arrangement in an in-plane stripe pattern with<br />

alternating exchange bias domains. The stripe pattern was produced by ion bombardment<br />

induced magnetic patterning, which changed locally the exchange bias direction<br />

at the ferromagnet/ antiferromagnet interface, but not the ferro- or antiferromagnetic<br />

properties of the Co70Fe30 and Mn83Ir17 layers, respectively. For the analysis of the<br />

magnetic domain structure evolution along the hysteresis loop we used a combination<br />

of experimental techniques: magneto-optical Kerr effect (MOKE), Kerr microscopy,<br />

polarized neutron reflectometry (PNR), and off-specular scattering of polarized neutrons<br />

with polarization analysis. Instead of a perfect antiparallel alignment we found<br />

that the magnetization in neighboring stripes is periodically canted with respect to<br />

the stripe axis so that the net magnetization of the ferromagnetic film turns almost<br />

perpendicular to the stripes. At the same time the projection of the magnetization<br />

vector onto the stripe axis has a periodically alternating sign. In Fig.1 the longitudinal<br />

MOKE hysteresis loop and in Fig. 2 specular PNR curves are displayed. In<br />

this measurements the non-spin-flip-reflectivities are almost degenerate and the spin<br />

asymmetry is SA≈0. The experimental observations are explained and quantitatively<br />

described within the frame of a phenomenological model. The model defines conditions<br />

which can be used for tailoring nano- and micro-patterned EB systems with different<br />

types of magnetic order. We gratefully acknowledge financial support by the DFG via<br />

SFB 491 and BMBF 03ZA6BC1.<br />

Fig. 1: MOKE hysteresis loop (line)<br />

and results of fits to the PNR data (symbols).<br />

Fig. 2: PNR measurements taken in the<br />

antiparallel state of the sample.

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