Physical review. B, Condensed matter · 2003 · 90 citations · 19 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsFinite Element AnalysisMagnetic MaterialsAntiferromagnetismExchange Bias MaterialsExchange InteractionsFerromagnetic MaterialsMagnetic AnisotropyMagnetism In SolidsDomain Wall EnergyExchange BiasExchange Bias FieldFerromagnet InterfacesHysteresisInterfacial Exchange CouplingMagnetic Exchange BiasUnidirectional Anisotropy
Energy associated with unidirectional anisotropy is stored in lateral domain walls between antiferromagnetic grains, unlike previous partial‑wall models. The study proposes a mechanism for exchange bias and training in antiferromagnet/ferromagnet bilayers with fully compensated interfaces. The bias shift and coercivity arise from domain‑wall formation between exchange‑coupled grains, and finite‑element micromagnetic calculations show that weak exchange between randomly oriented grains and spin‑flop coupling at a perfectly compensated interface produce shifted hysteresis loops. The mechanism naturally yields a training effect during magnetization loop cycling, as demonstrated by the calculated shifted hysteresis loops.
A mechanism for exchange bias and training for antiferromagnet/ferromagnet bilayers with fully compensated interfaces is proposed. In this model, the bias shift and coercivity are controlled by domain-wall formation between exchange-coupled grains in the antiferromagnet. A finite element micromagnetic calculation is used to show that a weak exchange interaction between randomly oriented antiferromagnetic grains and spin-flop coupling at a perfectly compensated interface are sufficient to create shifted hysteresis loops characteristic of exchange bias. Unlike previous partial wall models, the energy associated with the unidirectional anisotropy is stored in lateral domain walls located between antiferromagnetic grains. We also show that the mechanism leads naturally to a training effect during magnetization loop cycling.
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