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Phys. Rev. B 72, 012408 (2005) [4 pages]

Loop bifurcation and magnetization rotation in exchange-biased Ni∕FeF2

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Justin Olamit1, Elke Arenholz2, Zhi-Pan Li3, Oleg Petracic3,4, Igor V. Roshchin3, R. Morales3,5, Xavier Batlle3,6, Ivan K. Schuller3, and Kai Liu1,*
1Physics Department, University of California, Davis, California 95616, USA
2Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
3Physics Department, University of California–San Diego, La Jolla, California 92093, USA
4Angewandte Physik, University Duisburg-Essen, 47048 Duisburg, Germany
5Departamento de Fisica, Universidad de Oviedo, Oviedo 33007, Spain
6Departament de Física Fonamental, Universitat de Barcelona, 08028 Barcelona, Catalonia, Spain

Received 11 October 2004; revised 10 January 2005; published 13 July 2005

Exchange-biased Ni∕FeF2 films have been investigated using vector coil vibrating-sample magnetometry as a function of the cooling field strength HFC. In films with epitaxial FeF2, a loop bifurcation develops with increasing HFC as it divides into two sub-loops shifted oppositely from zero field by the same amount. The positively biased sub-loop grows in size with HFC until only a single positively shifted loop is found. Throughout this process, the negative and positive (sub)loop shifts maintain the same discrete value. This is in sharp contrast to films with twinned FeF2 where the exchange field gradually changes with increasing HFC. The transverse magnetization shows clear correlations with the longitudinal subloops. Interestingly, over 85% of the Ni reverses its magnetization by rotation, either in one step or through two successive rotations. These results are due to the single-crystal nature of the antiferromagnetic FeF2, which breaks down into two opposite regions of large domains.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.72.012408
DOI:
10.1103/PhysRevB.72.012408
PACS:
75.70.Cn, 75.60.−d, 75.50.Ee

*Electronic address: kailiu@ucdavis.edu