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Physica B: Condensed Matter
Volume 335, Issues 1-4 , July 2003, Pages 59-62

Proceedings of the Fourth International Workshop on Polarised Neutrons for Condensed Matter Investigations

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doi:10.1016/S0921-4526(03)00191-1    How to Cite or Link Using DOI (Opens New Window)  
Copyright © 2003 Elsevier Science B.V. All rights reserved.

Layer magnetization evolution in an Fe/Cr multilayer with uniaxial anisotropy

H. J. LauterCorresponding Author Contact Information, E-mail The Corresponding Author, a, V. Lauter-Pasyuka, b, c, B. P. Topervergd, e, U. Rückerd, M. Milyaevf, L. Romashevf, T. Krinitsynaf and V. Ustinovf

a Institut Laue Langevin, BP 156, Grenoble Cedex 9, F-38042, France
b Physik Department, TU München, Garching D-85747, Germany
c Joint Institute for Nuclear Research, 141980 Dubna, Moscow Region, Russia
d Forschungszentrum Jülich, IFF, Jülich D-52425, Germany
e Petersburg Nuclear Physics Institute, 188350 Gatchina, St. Petersburg, Russia
f Institute of Metal Physics, Ekaterinburg 62019, Russia

Available online 13 May 2003.


Abstract

The direction of the magnetization of each Fe layer in an Fe/Cr multilayer with uniaxial anisotropy was determined with polarized neutron reflectometry. The vectors of the layer magnetization of the multilayer transit from an antiferromagnetic alignment into a nearly ferromagnetic one with increasing magnetic field. In the transition region the system consists of an antiferromagnetically aligned part and a ferromagnetically aligned part. The magnetization curve is characterized by the subsequent switching of the antiferromagnetically aligned bilayers into the nearly ferromagnetically aligned state. Via this mechanism the antiferromagnetic part of the multilayer reduces in favor of the ferromagnetically aligned part with increasing magnetic field.

Author Keywords: Polarized neutron reflectometry; Antiferromagnetic coupling; Layer magnetization


Article Outline

• References



Enlarge Image
(11K)
Fig. 1. Schematic presentation of the Fe/Cr multilayer sample with scattering geometry. Here, only four Fe layers are shown from the [Fe/Cr]x12 structure. The sample has uniaxial in-plane anisotropy.

Enlarge Image
(10K)
Fig. 2. Magnetization curve of the Fe/Cr multilayer determined with VSM. The crosses indicate the magnetic field at which neutron reflectometry experiments were performed and what values of the net magnetization were obtained from the reflectivity data. The inset shows the uniaxial behavior of the sample measured at ~100 G.

Enlarge Image
(21K)
Fig. 3. Reflectivity curves (not corrected for polarization efficiency) taken from the Fe/Cr multilayer at various fields. The squares mark the measured (++) and (−−) spin configuration, respectively. (+) and (–) denote that neutron spin and magnetic field are parallel or antiparallel, respectively. The spin–flip scattering from the sample (±) and (±) are represented for (±) in the lower curve of each figure. The fit to the data (solid lines) includes the polarization efficiency of the polarizer and the analyzer. The reflectivity curves were measured at the magnetic fields: (a) H=20 G, (b) H=14 G, (c) H=450 G and (d) H=680 G.

Enlarge Image
(8K)
Fig. 4. Configuration of the layer magnetizations at five magnetic fields: (a) H=20 G, (b) H=14 G, (c) H=90 G, (d) H=450 G and (e) H=680 G. The presentation of the layer magnetizations with full and broken arrows helps to identify couples of anitiferromagnetically coupled layers and their transition to the ferromagnetic-like alignment.

References

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Corresponding Author Contact InformationCorresponding author. Tel.: +33-476-207-239; fax: +33-476-207-120



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Physica B: Condensed Matter
Volume 335, Issues 1-4 , July 2003, Pages 59-62
Proceedings of the Fourth International Workshop on Polarised Neutrons for Condensed Matter Investigations


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