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Combining large magnetostriction and large magnetostrictive susceptibility in TbFeCo/YxFe1-x exchange-spring-type multilayers

机译:TbFeCo / YxFe1-x交换弹簧型多层膜的大磁致伸缩率和大磁致伸缩率的组合

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摘要

An approach to obtain both large magnetostriction and large magnetostrictive susceptibility is developed. It is applied to sputtered {Tb(Fe0.55Co0.45)(1.5)/(YxFe1-x)} (x=0, 0.1 and 0.2) multilayers. In the as-deposited samples, the TbFeCo layers are in the amorphous state, but the microstructure of the YxFe1-x layers is not the same: A crystalline state is observed in pure Fe layers (x=0), whereas body-centered-cubic-Fe nanocrystals coexist within an YFe amorphous matrix in Y0.1Fe0.9 layers. A parallel magnetostrictive susceptibility chi(lambdaparallel to) as large as 29.4x10(-2) T-1, which is almost half of that (79.6x10(-2) T-1) of the Metglas 2605SC was obtained for x=0.1. This is attributed to the exchange coupling between sandwiched TbFeCo layers and nanostructured YFe layers. (C) 2004 American Institute of Physics.
机译:开发了一种同时获得大的磁致伸缩率和大的磁致伸缩磁化率的方法。将其应用于溅射的{Tb(Fe0.55Co0.45)(1.5)/(YxFe1-x)}(x = 0、0.1和0.2)多层。在沉积的样品中,TbFeCo层处于非晶态,但YxFe1-x层的微观结构不相同:在纯Fe层中观察到晶态(x = 0),而体心-立方铁纳米晶体共存于Y0.1Fe0.9层的YFe非晶基质中。当x = 0.1时,获得的平行磁致伸缩磁化率chi(λ平行于)大至29.4x10(-2)T-1,几乎是Metglas 2605SC的(79.6x10(-2)T-1)的一半。这归因于夹层的TbFeCo层和纳米结构的YFe层之间的交换耦合。 (C)2004美国物理研究所。

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