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Influence of ultra-thin Au interface layers on the structure and magnetic anisotropy of Co films.

机译:超薄金界面层对Co膜结构和磁各向异性的影响。

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摘要

I have investigated the influence of an ultra-thin Au interface layer on the magnetic anisotropy of Co-Pd and Co-Cu structures. Sandwich structures of the form X/Co/Y/Cu/Si(111), with (X, Y) = (Pd, Pd), (Au, Pd), (Pd, Au), (Cu, Cu), (Au, Cu), and (Cu, Au) were studied. For each structure, a Au layer of systematically varied thickness (t{dollar}rmsb{lcub}Au{rcub}){dollar} was inserted at one Co interface. I also investigated Co/Pd and Co/Cu multilayer systems. For each Co-Pd sandwich structures a maximum is observed in the magnetic anisotropy for t{dollar}rmsb{lcub}Au{rcub}{dollar} = 1 to 1.5 atomic monolayer (ML). For the Co/Pd multilayer system, a maximum in coercivity occurs with t{dollar}rmsb{lcub}Au{rcub}{dollar} = 0.5 ML. For each Co-Cu sandwich structure except (X, Y) = (Cu, Au), a minimum in magnetic anisotropy is observed at t{dollar}rmsb{lcub}Au{rcub}{dollar} = 1 ML. For the Co/Cu multilayer system, a decrease in magnetoresistance was seen with increased t{dollar}rmsb{lcub}Au{rcub},{dollar} except in multilayers with a relatively thin Co layer thickness ({dollar}sim{dollar}3 ML) which display a peak in magnetoresistance is seen at t{dollar}rmsb{lcub}Au{rcub}{dollar} = 1 ML. I have also investigated the strain, surface alloying, and surface (interface) roughness of these systems using RHEED, XPS, and LAXD. Analysis of these measurements reveals some correlation between magnetic anisotropy and both strain and surface roughness. Based on my investigations, I conclude that the most likely cause for the non-monotonic changes seen in anisotropy is changes in the surface magnetocrystalline anisotropy. While strain and surface roughness may also play a role, I believe that the influence of the ultra-thin Au interlayer on the orbital hybridization and electronic environment at the interface is dominant.
机译:我研究了超薄金界面层对Co-Pd和Co-Cu结构的磁各向异性的影响。 X / Co / Y / Cu / Si(111)形式的夹心结构,(X,Y)=(Pd,Pd),(Au,Pd),(Pd,Au),(Cu,Cu),(研究了Au,Cu)和(Cu,Au)。对于每种结构,在一个Co界面处插入厚度有系统变化的Au层(t {dollar} rmsb {lcub} Au {rcub}){dollar}。我还研究了Co / Pd和Co / Cu多层系统。对于每个Co-Pd夹层结构,对于t {dollar} rmsb {lcub} Au {rcub} {dollar} = 1到1.5个原子单层(ML),在磁各向异性中观察到最大值。对于Co / Pd多层系统,矫顽力最大,t {dollar} rmsb {lcub} Au {rcub} {dollar} = 0.5 ML。对于除(X,Y)=(Cu,Au)以外的每个Co-Cu夹层结构,在t {dollar} rmsb {lcub} Au {rcub} {dollar} = 1ML时观察到最小的磁各向异性。对于Co / Cu多层系统,除了具有相对较薄的Co层厚度的多层({dollar} sim {dollar}),随着t {dollar} rmsb {lcub} Au {rcub},{dollar}的增加,磁阻降低。在t {dollar} rmsb {lcub} Au {rcub} {dollar} = 1 ML时,出现了磁阻峰值的3 ML)。我还使用RHEED,XPS和LAXD研究了这些系统的应变,表面合金化和表面(界面)粗糙度。对这些测量的分析揭示了磁各向异性与应变和表面粗糙度之间的某些相关性。根据我的调查,我得出结论,各向异性中非单调变化的最可能原因是表面磁晶各向异性的变化。尽管应变和表面粗糙度也可能起一定作用,但我认为超薄Au中间层对界面处的轨道杂交和电子环境的影响占主导地位。

著录项

  • 作者

    Eickmann, James Thomas.;

  • 作者单位

    The University of Arizona.;

  • 授予单位 The University of Arizona.;
  • 学科 Physics Electricity and Magnetism.; Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 1998
  • 页码 153 p.
  • 总页数 153
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 电磁学、电动力学;
  • 关键词

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