Polarized neutron reflectivity on CoO/Co exchange biased multilayers
- 1. Institut fuer Experimentalphysik Festkorperphysik, Ruhr-Universitaet Bochum, Bochum (Germany)
- 2. Horia Hulubei National Institute for Physics and Nuclear Engineering, PO Box MG-6, RO-76900 Magurele-Bucharest (Romania)
- 3. Institut Max von Laue - Paul Langevin (ILL), 38 - Grenoble (France)
Description
The exchange bias (EB) phenomenon is associated with interfacial coupling between ferromagnetic and antiferromagnetic layers, which results in an unidirectional magnetic anisotropy. The macroscopic effects related to exchange biased systems are the shift of the hysteresis loop towards positive or negative directions and an increase of the coercivity field as upon cooling the system in an applied magnetic field. However, another macroscopic effect, namely, time relaxation of the exchange bias field has gained little attention so far. The system we used for measuring the three macroscopic effects and, especially, the time relaxation one is a CoO/Co multilayer. The sample was prepared by rf-sputter on an a-plane sapphire substrate. The growth parameters were optimised as to obtain a low interface roughness, in expense of the crystallinity. The measurements were carried out at the ADAM reflectometer (ILL) by Polarised Neutron Reflectometry. The samples have been characterised by x-ray reflectivity and MOKE measurements. Neutron hysteresis loops were measured at 310 K (TN of CoO is 291 K) and 240 K by scanning the magnetic field and detecting the 4 reflectivities (R++, R+-, R-+, R--) at the position of the first multilayer peak. From such curves we see that the reversal of magnetization in the sample occurs not by in-plane rotation but rather through domain walls movement. In-plane magnetic moment rotation would have induced an increase of the spin-flip reflectivities (R+- and R-+) at the crossing-point. There was no difference of the behaviour of the magnetization reversal process from room temperature to low temperature and from the positive to the negative part of the hysteresis loop. We noticed, as well, that the exchange bias field was not stable in time. It decreases from about 180 Oe towards 0 Oe. The half-life time obtained by fitting the time dependence of the exchange bias field (TDEBF) curve with a 'exponential decay' type of function was 580 sec. (authors)
Availability note (English)
Available from author(s) or Office of Documentation, Publication and Printing, Horia Hulubei National Institute for Physics and Nuclear Engineering, PO Box MG-6, RO-76900 Bucharest-Magurele (RO)Additional details
Publishing Information
- Imprint Title
- IFIN-HH, Scientific Report 2000
- Imprint Pagination
- 156 p.
- Journal Page Range
- p. 31
- ISSN
- 1454-2714
- Report number
- IFIN-HH-AR--2001
INIS
- Country of Publication
- Romania
- Country of Input or Organization
- Romania
- INIS RN
- 33052345
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY;
- Resource subtype / Literary indicator
- Non-conventional Literature, Progress Report
- Descriptors DEI
- COBALT; COBALT OXIDES; HYSTERESIS; INTERFACES; LAYERS; MAGNETIC FIELDS; NEUTRON REFLECTORS; NEUTRONS; POLARIZED BEAMS; PROGRESS REPORT; REFLECTIVITY; RELAXATION TIME; TEMPERATURE DEPENDENCE; TEMPERATURE RANGE 0273-0400 K
- Descriptors DEC
- BARYONS; BEAMS; CHALCOGENIDES; COBALT COMPOUNDS; DOCUMENT TYPES; ELEMENTARY PARTICLES; ELEMENTS; FERMIONS; HADRONS; METALS; NUCLEONS; OPTICAL PROPERTIES; OXIDES; OXYGEN COMPOUNDS; PHYSICAL PROPERTIES; SURFACE PROPERTIES; TEMPERATURE RANGE; TRANSITION ELEMENT COMPOUNDS; TRANSITION ELEMENTS
Optional Information
- Notes
- 3 refs., 2 figs.