Publication | Open Access
The exchange bias effect in phase separated Nd<sub>1−<i>x</i></sub>Sr<sub><i>x</i></sub>CoO<sub>3</sub>at the spontaneous ferromagnetic/ferrimagnetic interface
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Citations
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References
2009
Year
Magnetic PropertiesEngineeringSpin SystemsMagnetic ResonanceExchange Bias EffectSpintronic MaterialSpin DynamicMagnetic MaterialsMagnetoresistanceMagnetismQuantum MaterialsTraining EffectSpin-orbit EffectsPhysicsLow-dimensional SystemsMagnetoelasticitySpontaneous Ferromagnetic/ferrimagnetic InterfaceMicro-magnetic ModelingQuantum MagnetismSpintronicsFerromagnetismNatural SciencesApplied PhysicsCondensed Matter PhysicsMagnetic PropertyExchange Bias
We report new results for the exchange bias effect in Nd(1-x)Sr(x)CoO(3) for x = 0.20 and 0.40, where the exchange bias phenomenon is involved with the ferrimagnetic (FI) state in a spontaneously phase separated system. The zero-field-cooled magnetization exhibits FI (T(FI)) and ferromagnetic (FM; T(C)) transitions at ∼23 and ∼70 K, respectively, for x = 0.20. Negative horizontal and positive vertical shifts of the magnetic hysteresis loops are observed when the system is cooled through T(FI) in a positive static magnetic field. A training effect is observed for x = 0.20, which could be interpreted satisfactorily by the spin configurational relaxation model. The unidirectional shifts of the hysteresis loops as a function of temperature exhibit an absence of exchange bias above T(FI) for x = 0.20. Analysis of the cooling field dependence of the exchange bias field and magnetization indicates that the FM clusters consist of a single magnetic domain with an average size of around ∼20 and ∼40 Å for x = 0.20 and 0.40, respectively. The sizes of the FM clusters are close to the percolation threshold for x = 0.20; these grow and coalesce to form the bigger size for x = 0.40 resulting in a weak exchange bias effect.
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