2013
DOI: 10.1063/1.4812761
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Tailoring exchange bias through chemical order in epitaxial FePt3 films

Abstract: Intentional introduction of chemical disorder into mono-stoichiometric epitaxial FePt3 films allows to create a ferro-/antiferromagnetic two-phase system, which shows a pronounced and controllable exchange bias effect. In contrast to conventional exchange bias systems, granular magnetic interfaces are created within the same crystallographic structure by local variation of chemical order. The amount of the exchange bias can be controlled by the relative amount and size of ferromagnetic and antiferromagnetic vo… Show more

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Cited by 12 publications
(7 citation statements)
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“…FexPt1-x alloys are well known for their unusually robust magnetic anisotropy properties arising from the strong conduction electron spin-orbit interaction with the Fe orbital moment [17,18], and also for the dependence of the magnetic state on the chemical order. For example, well-ordered Fe0.25Pt0.75 exhibits antiferromagnetism, while chemically disordered Fe0.25Pt0.75 is ferromagnetic [19,20]. Ferromagnetic FexPt1-x films also exhibit quite large anomalous Hall effects (AHE) [21][22][23], which suggests that FexPt1-x can be a promising material for the generation of spin currents by the extrinsic SHE.…”
mentioning
confidence: 99%
“…FexPt1-x alloys are well known for their unusually robust magnetic anisotropy properties arising from the strong conduction electron spin-orbit interaction with the Fe orbital moment [17,18], and also for the dependence of the magnetic state on the chemical order. For example, well-ordered Fe0.25Pt0.75 exhibits antiferromagnetism, while chemically disordered Fe0.25Pt0.75 is ferromagnetic [19,20]. Ferromagnetic FexPt1-x films also exhibit quite large anomalous Hall effects (AHE) [21][22][23], which suggests that FexPt1-x can be a promising material for the generation of spin currents by the extrinsic SHE.…”
mentioning
confidence: 99%
“…Polarised neutron reflectometry (PNR) measurements performed on the artificial FM/AF bilayer confirm the interface between the two magnetic orders of FePt 3 is very sharp (<5 nm) and free of any chemical modulation [23]. Despite an almost perfect interface, the unique EB characteristics of the ion-beam derived FM/AF bilayer are an order of magnitude less than previous reports on FePt 3 FM/AF films fabricated by modulating the substrate temperature during film growth [20,24]. In response, the main objective of this article is to enhance the magnetic coupling across the FM/AF interface of the ion-beam-designed FePt 3 bilayer via thermal annealing.…”
Section: Introductionmentioning
confidence: 61%
“…By analysing the integrated intensity ratio between the film's fundamental and superstructure x-ray diffraction Bragg peaks [29], it is calculated that 82% of the film's Fe + Pt basis atoms (on average) assume the chemically ordered L1 2 atomic arrangement. From previous investigations, such films are known to order antiferromagnetically below a Néel temperature of ≈160 K [24]. The prepared film was subsequently irradiated at 298 K on the LEII-Surface Engineering beamline of the SIRIUS Tandem Accelerator located at the Australian Nuclear Science and Technology Organisation (ANSTO).…”
Section: Sample Preparation and Characterisationmentioning
confidence: 99%
“…26 The value of S is comparable to those previously obtained by our group following the same optimized sample preparation conditions. 27,28 The out-of-plane lattice parameter (a) of the film was determined to be a = 3.89 ± 0.01 Å, which is consistent with the reported bulk (a = 3.87 Å) 14 and previous thin film values (a = 3.88 Å). 13,29 From XRD analysis, the average out-of-plane FePt 3 crystallite size was 620 Å (lower-bound approximation only), with a mosaic spread of 0.81°along the film epitaxial growth direction.…”
Section: ■ Conclusionmentioning
confidence: 99%