首页> 外文期刊>Solid State Communications >Anisotropic magnetoresistance and magnetostriction of [Fe15Ni85/Fe25Ni75] and [Co35Ni65/Fe25Ni75] multilayers
【24h】

Anisotropic magnetoresistance and magnetostriction of [Fe15Ni85/Fe25Ni75] and [Co35Ni65/Fe25Ni75] multilayers

机译:[Fe15Ni85 / Fe25Ni75]和[Co35Ni65 / Fe25Ni75]多层膜的各向异性磁阻和磁致伸缩

获取原文
获取原文并翻译 | 示例
           

摘要

We have made a series of [A(x)B(60-)x](n) multilayers and another series of [CxB60-x](n) multilayers, where A = Fe15Ni85, B = Fe25Ni75, C = Co35Ni65, n = 2 is the period, and x(A) (or x(C)) is the thickness of layer A (or layer C) in nanometer, respectively. The deposition temperature T-s was 340 degreesC. The magnetic properties, such as anisotropic magnetoresistance Deltarho/Deltarho(o), saturation magnetostriction lambda(s), and anisotropy field H-k, were measured. Although Deltarho/Deltarho(o). of the [C-60](2) film is larger than that of the [B-60](2) film, Hk of the former is also much larger. Therefore, the magnetoresistance (MR) sensitivity S, defined as the slope at the point of inflection of the MR curve, is not gained for either single-layered film. A similar situation exists between the [A(60)](2) and [B-60](2) films, except H-k of the former is only slightly larger. Besides, lambda(s) < 0 for Fe15Ni85 alloy (the [A(60)](2) film), lambda(s) < 0 for Co35Ni65 alloy (the [C-60](2) film), and lambda(s) > 0 for Fe25Ni75 alloy (the [B-60](2) film). Despite these unfavorable facts, we think that if the multi-layered [NB60-x](n), or [CxB60-x](n) film could be formed, it is possible to find the optimal sample, with either the composition X-A(0) or X-C(0), which exhibits good MR sensitivity S, while at the same time zero lambda(s). Indeed, we found that: (1) when X-A(0) = 50 nm, S can be as high as 1.9%/Oe, and (2) when X-C(0) = 35 nm, S is 0.40%/Oe. More importantly, we have shown that T-s = 340 degreesC is the best choice for the [A/B] multilayers, when a more precise control Of x(A) is required in order to get the linear dependence of lambda(s) on x(A). (C) 2004 Elsevier Ltd. All rights reserved.
机译:我们制作了一系列[A(x)B(60-)x](n)多层和另一系列[CxB60-x](n)多层,其中A = Fe15Ni85,B = Fe25Ni75,C = Co35Ni65,n = 2是周期,x(A)(或x(C))分别是层A(或层C)的纳米厚度。沉积温度T-s为340℃。测量了诸如各向异性磁阻Deltarho / Deltarho(o),饱和磁致伸缩λ和各向异性场H-k的磁性。虽然是Deltarho / Deltarho(o)。 [C-60](2)膜的膜厚比[B-60](2)膜的膜厚大,前者的Hk也大得多。因此,对于任一单层膜都没有获得定义为MR曲线拐点处的斜率的磁阻(MR)灵敏度S。在[A(60)](2)和[B-60](2)膜之间也存在类似情况,只是前者的H-k稍大。此外,对于Fe15Ni85合金([A(60)](2)膜,λ<0),对于Co35Ni65合金([C-60](2)膜,λ<0)。对于Fe25Ni75合金([B-60](2)膜),s)> 0。尽管存在这些不利的事实,我们认为,如果可以形成多层[NB60-x](n)或[CxB60-x](n)膜,则可以找到成分为XA的最佳样品(0)或XC(0),表现出良好的MR灵敏度S,而同时零λ。实际上,我们发现:(1)当X-A(0)= 50 nm时,S可以高达1.9%/ Oe;以及(2)当X-C(0)= 35 nm时,S为0.40%/ Oe。更重要的是,当需要更精确地控制x(A)以获得λ对x的线性相关性时,我们表明Ts = 340°C是[A / B]多层的最佳选择(一个)。 (C)2004 Elsevier Ltd.保留所有权利。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号