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首页> 外文期刊>Journal of magnetism and magnetic materials >Temperature induced ferromagnetic resonance frequency change and resonance line broadening of a Fe-Co-Hf-N film with in-plane uniaxial anisotropy - a theoretical and experimental study
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Temperature induced ferromagnetic resonance frequency change and resonance line broadening of a Fe-Co-Hf-N film with in-plane uniaxial anisotropy - a theoretical and experimental study

机译:面内单轴各向异性的Fe-Co-Hf-N薄膜的温度感应铁磁共振频率变化和共振线展宽-理论与实验研究

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摘要

A soft ferromagnetic Fe-Co-Hf-N film was produced by reactive r.f. magnetron sputtering, in order to study its high-frequency behaviour by means of frequency domain permeability measurements up to the GHz range. It resulted in the composition Fe_(33)Co_(43)Hf_(10)N_(14) and exhibits a saturation polarisation J_s of around 1.35 T. The film is consequently considered as being uniformly magnetised due to an in-plane uniaxial anisotropy of approximately μ_0·H_u ≈ 4.5 mT after annealing it at 400 ℃ in a static magnetic field for 1 h. While heating the film from room temperature to 300 ℃ during the high-frequency measurement procedure a marked ferromagnetic resonance peak shift (maximum of the imaginary part of the frequency-dependent permeability) from 2.35 GHz down to 1.84 GHz is conspicuous. This is in a very good agreement with the theory established by taking the "real" ferromagnetic resonance formula for ferromagnetic films into account. Simultaneously, the full width at half maximum (FWHM) △f_(FMR) of the resonance line, which is a consequence of precession damping of the magnetic moments, clearly increases. This behaviour does not correlate with the ferromagnetic resonance value decrease, and is qualitatively discussed in terms of exchange interaction with the intrinsic spin-lattice relaxation process due to not totally supressed orbital momenta (〈L〉≠0) of Fe~(2+) and Co~(2+) or the occupation change of their spectral levels within the induced uniaxial anisotropy field.
机译:通过反应射频制备软铁磁Fe-Co-Hf-N膜。磁控溅射,以便通过高达GHz范围的频域磁导率测量来研究其高频性能。它的成分为Fe_(33)Co_(43)Hf_(10)N_(14),饱和极化J_s约为1.35T。因此,由于该膜的面内单轴各向异性,该膜被均匀地磁化了。将其在静磁场中于400℃退火1 h后,大约为μ_0·H_u≈4.5 mT。在高频测量过程中将薄膜从室温加热到300℃时,从2.35 GHz到1.84 GHz的明显铁磁共振峰位移(频率相关磁导率的虚部最大值)明显。这与通过考虑铁磁膜的“真实”铁磁谐振公式而建立的理论非常吻合。同时,由于磁矩的进动阻尼而导致的谐振线的半峰全宽(FWHM)△f_(FMR)明显增加。该行为与铁磁共振值的降低无关,由于Fe〜(2+)的轨道矩量(≠0)没有完全抑制,因此与本征自旋晶格弛豫过程交换相互作用进行了定性讨论。和Co〜(2+)或它们的光谱能级在感应单轴各向异性场内的变化。

著录项

  • 来源
    《Journal of magnetism and magnetic materials》 |2014年第11期|142-146|共5页
  • 作者单位

    Karlsruhe Institute of Technology KIT (Campus North), Institute for Applied Materials, Hermann-von-Helmholtz-Platz 1,76344 Eggenstein-Leopoldshafen, Germany;

    Karlsruhe Institute of Technology KIT (Campus North), Institute for Applied Materials, Hermann-von-Helmholtz-Platz 1,76344 Eggenstein-Leopoldshafen, Germany;

    Karlsruhe Institute of Technology KIT (Campus North), Institute for Applied Materials, Hermann-von-Helmholtz-Platz 1,76344 Eggenstein-Leopoldshafen, Germany;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Ferromagnetic film; Temperature-dependent FMR; Line broadening; Intrinsic damping;

    机译:铁磁膜;温度相关的FMR;线展宽;固有阻尼;

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