2002
DOI: 10.1063/1.1447531
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Thermally activated self-alignment of exchange coupling in NiO/NiFe bilayers

Abstract: Long-term and temperature stability of the exchange coupling are important conditions for the practical application of spin-valve devices. Here we present magnetic measurements on the properties of sputtered NiO/NiFe bilayers. After deposition a temperature dependent magnetic self-alignment process was observed where the exchange bias field H eb increased according to a ln(t) law. The temperature dependence of this aftereffect indicates that a thermally activated process takes place which can be explained by a… Show more

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Cited by 24 publications
(30 citation statements)
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“…Since for defect creation within the AF volume the exchange coupling constant and the magnetically effective contact area is not changed the energy barrier ∆ i between the two minima in the free energy function is lowered and therefore some AF domains may thermally change their anisotropy axes even at room temperature. This leads to a slow increase of H eb with time after the IB, similar to the thermal after effect of the EB [2].…”
Section: Ion Bombardment Induced Modifications Of H Ebmentioning
confidence: 61%
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“…Since for defect creation within the AF volume the exchange coupling constant and the magnetically effective contact area is not changed the energy barrier ∆ i between the two minima in the free energy function is lowered and therefore some AF domains may thermally change their anisotropy axes even at room temperature. This leads to a slow increase of H eb with time after the IB, similar to the thermal after effect of the EB [2].…”
Section: Ion Bombardment Induced Modifications Of H Ebmentioning
confidence: 61%
“…Some AF/FM bilayers showed a thermal after effect [2] of H eb , i.e. after the H eb has been initially set H eb slowly increases with time to a certain saturation value H eb,0 .…”
Section: Introductionmentioning
confidence: 99%
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“…To establish the initial unidirectional anisotropy (defined here as the ''x-direction'') throughout the whole sample, a magnetic field H gro ¼ 40 Oe was applied in x-direction parallel to the substrate surface plane during film growth. After deposition the exchange coupling was stabilized by annealing the samples at 540 K for 20 min and subsequent cooling to room temperature in a magnetic field of 1 kOe parallel to the easy axis of magnetization [15]. A hysteresis loop of sample no.…”
Section: Sample Preparation and Ibmpmentioning
confidence: 99%
“…The bilayer was deposited in a Leybold Z400 rf diode sputtering system on a 0:2 nm thin glass substrate. NiFe oxidation was prevented by a Ta capping layer of 2 nm: The deposition process of this sample has been described previously [9,15], so only the most important parameters should be briefly mentioned here. The antiferromagnetic NiO layers were deposited in a reactive sputtering process from a pure Ni target in an Ar=O 2 gas mixture of 100 sccm Ar and 0:6 sccm O 2 : The deposition rates were determined by calibration films and amounted to 4:3 nm=min; 7:8 nm=min; and 5:7 nm=min for NiO, NiFe, and Ta, respectively.…”
Section: Sample Preparation and Ibmpmentioning
confidence: 99%