首页> 外文期刊>Applied Physics Letters >The magnetization behavior and open recoil loops of hot-deformed Nd-Fe-B magnets infiltrated by low melting point PrNd-Cu alloys
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The magnetization behavior and open recoil loops of hot-deformed Nd-Fe-B magnets infiltrated by low melting point PrNd-Cu alloys

机译:低熔点PrNd-Cu合金渗透的Nd-Fe-B热变形Nd-Fe-B磁体的磁化行为和开放的反冲环

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摘要

Ultrahigh coercivity of hot-deformed Nd-Fe-B magnets was obtained by low melting point PrNd-Cu alloys diffusion process. The coercivity was largely increased from 15.35 to 27.30 kOe. Magnetic isolation by nonmagnetic phases should be the primary explanation for the enhancement of coercivity. High susceptibility of the recoil loops at low field indicated that magnetic domain wall motion within grains was easy, while a near-zero reversible susceptibility of recoil loops implied that domain wall strong pinning at grain boundaries was dominant at higher field in initial magnetization process. Open recoil loops were also obtained in the infiltrated magnets and disappeared when the external field exceeded about 16 kOe lightly higher than the coercivity of the magnet without diffusion process. The inhomogeneous distribution of infiltrated phases that led to the grains aggregation and single grains with softer and harder magnetic characteristics, respectively, may be the primary reason for the phenomenon. The stray field produced by isolated single grains plays a critical role in the magnetization behavior. A phenomenological model for the magnetization reversal was built to interpret the open recoil loops in a recoil loop process.
机译:通过低熔点的PrNd-Cu合金扩散过程获得了热变形Nd-Fe-B磁体的超高矫顽力。矫顽力从15.35 kOe大大提高。非磁性相的磁隔离应是增强矫顽力的主要解释。反冲环在低磁场下的高磁化率表明晶粒内的磁畴壁运动很容易,而反冲环的接近零可逆磁化率表明在初始磁化过程中,在较高磁场下,畴壁强钉扎在晶界处占主导地位。在渗入的磁体中也获得了开放的反冲环,当外场超过约16 kOe时略大于未扩散过程的磁体的矫顽力时,反冲环消失了。渗透相的不均匀分布可能分别导致晶粒聚集和具有较软和较硬磁性特征的单晶粒,这可能是造成这种现象的主要原因。由孤立的单个晶粒产生的杂散场在磁化行为中起关键作用。建立了磁化反转的现象学模型,以解释反冲环过程中的开放反冲环。

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  • 来源
    《Applied Physics Letters》 |2015年第20期|202403.1-202403.5|共5页
  • 作者单位

    Key Laboratory of Magnetic Materials and Devices, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China ,Rare Earth Magnetic Materials Laboratory, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China;

    Key Laboratory of Magnetic Materials and Devices, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China ,Rare Earth Magnetic Materials Laboratory, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China;

    Key Laboratory of Magnetic Materials and Devices, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China ,Rare Earth Magnetic Materials Laboratory, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China;

    Key Laboratory of Magnetic Materials and Devices, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China ,Rare Earth Magnetic Materials Laboratory, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China;

    University of Dayton, Dayton, Ohio 45469, USA;

    Key Laboratory of Magnetic Materials and Devices, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China ,Rare Earth Magnetic Materials Laboratory, Ningbo Institute of Material Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, People's Republic of China;

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  • 正文语种 eng
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