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通过氮插入和拓扑化学萃取合成单相L1-FeNi磁粉。

Synthesis of single-phase L1-FeNi magnet powder by nitrogen insertion and topotactic extraction.

作者信息

Goto Sho, Kura Hiroaki, Watanabe Eiji, Hayashi Yasushi, Yanagihara Hideto, Shimada Yusuke, Mizuguchi Masaki, Takanashi Koki, Kita Eiji

机构信息

Advanced Research and Innovation Center, DENSO Corporation, Aichi, 470-0111, Japan.

Institute of Applied Physics, University of Tsukuba, Ibaraki, 305-8573, Japan.

出版信息

Sci Rep. 2017 Oct 16;7(1):13216. doi: 10.1038/s41598-017-13562-2.

DOI:10.1038/s41598-017-13562-2
PMID:29038579
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5643398/
Abstract

Tetrataenite (L1-FeNi) is a promising candidate for use as a permanent magnet free of rare-earth elements because of its favorable properties. In this study, single-phase L1-FeNi powder with a high degree of order was synthesized through a new method, nitrogen insertion and topotactic extraction (NITE). In the method, FeNiN, which has the same ordered arrangement as L1-FeNi, is formed by nitriding A1-FeNi powder with ammonia gas. Subsequently, FeNiN is denitrided by topotactic reaction to derive single-phase L1-FeNi with an order parameter of 0.71. The transformation of disordered-phase FeNi into the L1 phase increased the coercive force from 14.5 kA/m to 142 kA/m. The proposed method not only significantly accelerates the development of magnets using L1-FeNi but also offers a new synthesis route to obtain ordered alloys in non-equilibrium states.

摘要

四方铁镍矿(L1-FeNi)因其优良性能,是一种很有前景的无稀土永磁体候选材料。在本研究中,通过一种新方法——氮插入和拓扑化学萃取(NITE),合成了具有高度有序性的单相L1-FeNi粉末。在该方法中,与L1-FeNi具有相同有序排列的FeNiN,是通过用氨气氮化A1-FeNi粉末形成的。随后,通过拓扑化学反应对FeNiN进行脱氮,得到有序参数为0.71的单相L1-FeNi。无序相FeNi向L1相的转变使矫顽力从14.5 kA/m增加到142 kA/m。所提出的方法不仅显著加速了使用L1-FeNi的磁体的开发,还提供了一种获得非平衡态有序合金的新合成途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d5d402d195f5/41598_2017_13562_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d1d89d4b9109/41598_2017_13562_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d77da19b772e/41598_2017_13562_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/1a68f174e786/41598_2017_13562_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/037669a73e70/41598_2017_13562_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d5d402d195f5/41598_2017_13562_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d1d89d4b9109/41598_2017_13562_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d77da19b772e/41598_2017_13562_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/1a68f174e786/41598_2017_13562_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/037669a73e70/41598_2017_13562_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8671/5643398/d5d402d195f5/41598_2017_13562_Fig5_HTML.jpg

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4
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ACS Omega. 2023 Apr 10;8(15):13690-13701. doi: 10.1021/acsomega.2c07869. eCollection 2023 Apr 18.
5
Direct Formation of Hard-Magnetic Tetrataenite in Bulk Alloy Castings.块状合金铸件中硬磁四方铁纹石的直接形成
Adv Sci (Weinh). 2022 Oct 25;10(1):e2204315. doi: 10.1002/advs.202204315.
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