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Magnetoelectric Properties of CoFe{sub}2O{sub}4-BaTiO{sub}3 Core-Shell Structure Composites

机译:Cofe {sub} 2o {sub} 4-batio {sub} 3芯壳结构复合材料的磁电性能

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Magnetoelectric (ME) materials become magnetized when placed in an electric field and electrically polarized when placed in a magnetic field. Thus an effective conversion between electric and magnetic energy becomes possible, and ME materials present themselves as one kind of smart materials. They can be classified into two classes: single phase and composite. For single phase materials, due to the primary requirement to observe the ME effect is the coexistence of magnetic and electric dipoles in an asymmetric structure, the number of compounds that exhibit ME effect is limited, the ME coefficient, α{sub}E=({partial deriv}E/{partial deriv}H){sub}T, is small, working temperature is low and involved expensive materials and processing techniques. These limitations can be overcome when shifted to composites, which usually consist of magnetostrictive and piezoelectric phases, resulting in a ME effect as product property of this combination [1].
机译:当放置在电场中时,磁电(ME)材料变得磁化,并且当放置在磁场中时电极化。因此,电力和磁能之间的有效转换变得可能,并且我材料本身将自己作为一种智能材料。它们可以分为两类:单相和复合。对于单相材料,由于观察ME效果的主要要求是不对称结构中磁性和电偶极子的共存,表现出我效应的化合物的数量是有限的,ME系数,α{Sub} E =( {部分德国} e / {部分eriv} h){sub} t,很小,工作温度低,涉及昂贵的材料和处理技术。当转移到复合材料时,可以克服这些限制,这通常由磁致伸缩和压电阶段组成,导致我作为该组合的产品性能的影响[1]。

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