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首页> 外文期刊>Journal of Applied Physics >Ferromagnetic Resonance Linewidth and Internal Biasing Field in Ni‐Fe Films as a Function of Dispersion in the Anisotropy Field Magnitude
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Ferromagnetic Resonance Linewidth and Internal Biasing Field in Ni‐Fe Films as a Function of Dispersion in the Anisotropy Field Magnitude

机译:Ni-Fe薄膜中铁磁谐振线宽和内部偏置场与各向异性场幅度中色散的关系

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摘要

Ferromagnetic resonance techniques have been used to measure the magnetic properties of Ni‐Fe films in the 50–1500 Mc/sec range. Resonance was observed in the plane of films 8 mm in diameter and 600–2600 Å thick. The primary purpose of the investigation was to obtain a correlation between the resonance linewidth extrapolated to zero frequency (ΔH)0, and the dispersion in anisotropy field magnitude Δ90. The zero‐frequency linewidths found were about 2.8 times the values calculated theoretically from values of anisotropy field magnitude dispersion independently obtained in this laboratory. Plots of the resonance frequency squared as a function of resonance field showed a shift, or internal bias Hi, toward positive field values as others have observed. There was little or no shift for films with Δ90 less than about 0.2, but for larger dispersion, the shift increased approximately linearly with Δ90. A very good linear correlation was found between Hi and α0, the high‐frequency damping parameter. It is suggested that the internal biasing field may be associated with the magnetization rippling that Fuller and Hale and Feldtkeller have observed in electron micrographs. Also, it may be possible that the larger‐than‐expected values of (ΔH)0, and the wide variation in α0 values (0.006–0.03) reported here are caused by the energy loss, which Feldtkeller has termed ``ripple hysteresis,'''' associated with the movement of the small‐angle walls, which result from the magnetization rippling.
机译:铁磁共振技术已用于测量50-1500 Mc / sec范围内的Ni-Fe膜的磁性。在直径8毫米,厚600-2600埃的薄膜平面上观察到共振。研究的主要目的是获得外推到零频率(ΔH)0的谐振线宽与各向异性场幅度Δ90的离散之间的相关性。发现的零频线宽大约是从该实验室独立获得的各向异性场幅值色散值理论计算得出的值的2.8倍。共振频率的平方作为共振场的函数,显示出正电场值向正电场值的偏移,如其他观察到的。对于具有小于约0.2的Δ90的膜,几乎没有或没有偏移,但是对于较大的分散,偏移随Δ90近似线性地增加。在Hi和高频阻尼参数α0之间发现了很好的线性相关性。建议内部偏置场可能与富勒,黑尔和费尔德凯勒在电子显微图中观察到的磁化波纹有关。同样,此处报告的(ΔH)0值大于预期,α0值(0.006-0.03)的较大变化也可能是由能量损失引起的,Feldtkeller称之为``波纹磁滞, ''''与小角度壁的运动有关,这是由磁化波纹引起的。

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  • 来源
    《Journal of Applied Physics 》 |1964年第3期| 共2页
  • 作者

    Nelson Roger H.;

  • 作者单位

    UNIVAC, Division of Sperry Rand Corporation, St. Paul, Minnesota;

  • 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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