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Exchange bias effect in bulk multiferroic BiFe0.5Sc0.5O3

机译:在散装多重BIFE0.5SC0.5O3中交换偏置效果

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摘要

Below the Néel temperature, T N ~ 220 K, at least two nano-scale antiferromagnetic (AFM) phases coexist in the polar polymorph of the BiFe 0.5 Sc 0.5 O 3 perovskite; one of these phases is a weak ferromagnetic. Non-uniform structure distortions induced by high-pressure synthesis lead to competing AFM orders and a nano-scale spontaneous magnetic phase separated state of the compound. Interface exchange coupling between the AFM domains and the weak ferromagnetic domains causes unidirectional anisotropy of magnetization, resulting in the exchange bias (EB) effect. The EB field, H EB , and the coercive field strongly depend on temperature and the strength of the cooling magnetic field. H EB increases with an increase in the cooling magnetic field and reaches a maximum value of about 1 kOe at 5 K. The exchange field vanishes above T N with the disappearance of long-range magnetic ordering. The effect is promising for applications in electronics as it is large enough and as it is tunable by temperature and the magnetic field applied during cooling.
机译:低于Néel温度,T n〜220 k,至少两个纳米级反铁磁性(AFM)阶段在Bife 0.5 sc 0.5℃的极性多晶型物中共存;其中一个阶段是弱铁磁性。高压合成诱导的非均匀结构畸变导致竞争AFM订单和纳米级自发磁相分离状态。 AFM域和弱铁磁结构域之间的界面交换耦合导致磁化的单向各向异性,从而导致交换偏压(EB)效应。 EB字段,HEB和矫顽磁场强烈依赖于冷却磁场的温度和强度。 H EB随着冷却磁场的增加而增加,并且在5 k下达到约1只koe的最大值。交换场随着远程磁化的消失而消失。该效果对电子产品的应用很大,因为它足够大,并且在冷却期间通过温度和磁场进行可调。

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