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Journal of Magnetism and Magnetic Materials
Volume 240, Issues 1-3 , February 2002, Pages 251-253

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doi:10.1016/S0304-8853(01)00815-0    How to cite or link using doi (opens new window) Cite or link using doi  
Copyright © 2002 Elsevier Science B.V. All rights reserved.

Asymmetric magnetization reversal on exchange biased CoO/Co bilayers

F. RaduCorresponding Author Contact Information, E-mail The Corresponding Author, a, b, M. Etzkorna, T. Schmittea, R. Siebrechta, c, A. Schreyera, K. Westerholta and H. Zabela

a Institut für Experimentalphysik, Festkörperphysik, Ruhr-Universität Bochum, D 44780 Bochum, Germany
b Departamentul de Fizica Experimentala, Institutul National de Fizica si Inginerie Nucleara, P.O. BOX MG-6, 76900, Magurele-Bucuresti, Romania
c Institute Laue-Langevin, 38042, Grenoble cedex 9, France

Available online 17 October 2001.


Abstract

We study magnetic hysteresis loops after field cooling of a CoO/Co bilayer by MOKE and polarized neutron reflectivity. The neutron scattering reveals that the first magnetization reversal after field cooling is dominated by domain wall movement, whereas all subsequent reversals proceed essentially by rotation of the magnetization. In addition, off-specular diffuse scattering indicates that the first magnetization reversal induces an irreversible change of the domain state in the antiferromagnet.

Author Keywords: Exchange bias; Magnetization reversal; Neutron reflectivity


Article Outline

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(21K)
Fig. 1. (a) MOKE hysteresis loop of a CoO/Co bilayer after field cooling to 50 K in an external field of 2000 Oe. The black dots denote the first hysteresis loop, the open circles the second loop. Any further loops are not significantly different from the second. (b) and (c) Neutron hysteresis loops from the same sample but at 10 K. I++, I--, I+- and I-+ are non-spin flip and spin-flip intensities as a function of external magnetic field. They are measured at special scattering vector values of the reflectivity curves (see text); (d) Off-specular diffuse spin-flip scattering taken at Hc1=-750 Oe (full dots) and in saturation at -1400 Oe (open dots). (e) Specular spin-flip at Hc1 enlarged from panel (b) for better recognition.

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Corresponding Author Contact Information Corresponding author. Fax: +49-234-3214-173; email: radu@spin.ep4.ruhr-uni-bochum.de



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Journal of Magnetism and Magnetic Materials
Volume 240, Issues 1-3 , February 2002 , Pages 251-253


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