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Influence of isochronal annealing on the microstructure and magnetic properties of Cu-free HITPERM Fe40.5Co40.5Nb7B12 alloy

机译:等时退火对无Cu HITPERM Fe40.5Co40.5Nb7B12合金的组织和磁性能的影响

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摘要

Systematic study of the effect of isochronal annealing on the structure and magnetic properties of Cu-free HITPERM alloy (Fe40.5Co40.5Nb7B12) is described herein. Mo¨ssbauer spectroscopy (MS) and anomalous x-ray diffraction (XRD) measurement at Fe K-edge (7.112 keV) jointly provide clear evidence for the presence of atomically ordered a0-FeCo (B2 structure) phase as a nanocrystalline ferromagnetic phase. Being a short range order probe, Mo¨ssbauer spectroscopy also confirms the development of an additional non-magnetic Nb-rich phase in the nanocrystalline specimens (annealed above 723 K) with simultaneous lowering of the volume fraction of ferromagnetic phases. The fraction of Fe atoms in the non-magnetic phase is rv15% upon annealing at 773 K for 1 h, which increases gradually and reaches to as high as rv19% after annealing at 923 K. This phase was not detected by XRD and transmission electron microscopy (TEM) measurements, which may be attributed to tiny crystallite size and/or high degree of disorder. In the second stage of crystallization, i.e., above 923 K, the alloy becomes fully crystalline and a stable, hard magnetic fcc-(FeCo)23B6 type phase was observed as a main boride phase along with soft magnetic a0-FeCo phase and Nb rich non-magnetic phase. Thermo magnetic measurement evidenced re-crystallization process as a considerable decrease in magnetization at the second transformation stage. Simultaneous lowering of the volume fraction of magnetic phases with the formation of non-magnetic phase provides convincing origin for the decrease in magnetization at the second crystallization stage
机译:本文介绍了等时退火对无铜HITPERM合金(Fe40.5Co40.5Nb7B12)的结构和磁性的影响的系统研究。在Fe K边缘(7.112 keV)上进行的Mossbauer光谱(MS)和异常X射线衍射(XRD)测量共同为存在原子序的a0-FeCo(B2结构)相作为纳米晶铁磁相提供了明确的证据。作为短程有序探针,穆斯堡尔光谱法还证实了在纳米晶样品(退火至723 K以上)中另外一种非磁性富Nb相的发展,同时降低了铁磁相的体积分数。在773 K退火1 h后,非磁性相中的Fe原子分数为rv15%,在923 K退火后逐渐增加并高达rv19%。XRD和透射电子均未检测到该相显微镜(TEM)测量,这可能归因于微晶尺寸小和/或高度无序。在结晶的第二阶段,即高于923 K,合金变为完全结晶,并且观察到稳定的硬磁fcc-(FeCo)23B6型相与软磁a0-FeCo相和富Nb一起作为主要的硼化物相。非磁性相。热磁测量表明再结晶过程是第二相变阶段的磁化强度显着降低。形成非磁性相同时降低磁性相的体积分数,为第二个结晶阶段磁化强度降低提供了令人信服的起点

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