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Volume contribution to perpendicular anisotropy in Fe_(0.5)Co_(0.5) alloy films on Pd(001), Ir(001), and Rh(001)

机译:Pd(001),Ir(001)和Rh(001)上Fe_(0.5)Co_(0.5)合金膜中垂直各向异性的体积贡献

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摘要

In tetragonally distorted Fe_(0.5)Co_(0.5) alloy films grown epitaxially on Pd(001), Ir(001), and Rh(001) substrates the crystal field locates the electronic states near the Fermi level (E_F) with one being below E_F and the other above E_F with an energy separation smaller than in bulk nondistorted material. This results in a strong uniaxial anisotropy and an easy magnetization axis perpendicular to the film plane up to the thickness up to which the films remain tetragonally distorted. The strongest perpendicular anisotropy is achieved when the Fe_(0.5)Co_(0.5) films are grown on Rh(001) (c/a= 1.24); it systematically decreases for Ir(001) (c/a= 1.18) and Pd(001) (c/a=1.13) substrates. The phenomenon can be understood as a result of an increasing uniaxial anisotropy with an increasing c/a ratio up to the maximum at c/a= 1.24 for which the maximum uniaxial magnetic anisotropy has been theoretically predicted.
机译:在Pd(001),Ir(001)和Rh(001)衬底上外延生长的四方畸变的Fe_(0.5)Co_(0.5)合金膜中,晶体场将电子态定位在费米能级(E_F)附近,其中一个低于E_F和E_F之上的另一个,其能量间隔比未变形的散装材料小。这导致很强的单轴各向异性和易于垂直于膜平面的磁化轴,直至膜保持四方畸变的厚度。当Fe_(0.5)Co_(0.5)薄膜在Rh(001)上生长时,可获得最强的垂直各向异性(c / a = 1.24);对于Ir(001)(c / a = 1.18)和Pd(001)(c / a = 1.13)底物,它会系统地降低。可以理解为该现象是由于单轴各向异性的增加,而c / a的比值不断增加,直到在c / a = 1.24时达到最大值,理论上已经预测到了最大单轴磁各向异性。

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  • 来源
    《Journal of Applied Physics》 |2009年第3期|693-695|共3页
  • 作者单位

    Max-Planck-Institut fuer Mikrostrukturphysik, Weinberg 2, 06120 Halle, Germany;

    Max-Planck-Institut fuer Mikrostrukturphysik, Weinberg 2, 06120 Halle, Germany;

    Max-Planck-Institut fuer Mikrostrukturphysik, Weinberg 2, 06120 Halle, Germany;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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