Magnetic hardness of hexagonal and orthorhombic Fe$_{3}$C, Co$_{3}$C, (Fe-Co)$_{3}$C, and their alloys with boron, nitrogen, and transition metals: A first-principles study

Justyn Snarski-Adamski, Mirosław Werwiński, Justyna Rychły-Gruszecka
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Abstract

In this study, we considered a large set of materials that are closely related to orthorhombic Fe$_3$C (cementite) with the aim of characterizing trends in their intrinsic magnetic properties and identifying alloys that are optimal for applications. A comprehensive analysis was conducted on the full concentration ranges of hexagonal ($\epsilon$) and orthorhombic ($\theta$) phases of (Fe-Co)$_3$C, (Fe-Co)$_3$(B-C), (Fe-Co)$_3$(C-N), and their alloys with 3$d$, 4$d$ and 5$d$ transition metals. The calculations were performed using the density functional theory implemented in the full-potential local-orbital code (FPLO). Calculated properties included formation energies, Curie temperatures, magnetic moments, magnetocrystalline anisotropy energies (MAE), and magnetic hardnesses. The considered compositions exhibit a range of magnetic properties, including soft, semi-hard, and hard magnetic. The materials most promising for hard-magnetic applications are orthorhombic Co$_3$C compound, together with selected Co-rich orthorhombic (Fe,Co)$_3$C and hexagonal (Fe,Co)$_3$C alloys. The calculation results do not indicate that substituting with transition metals increases the potential of the alloys for permanent magnet applications. A significant drawback of alloying orthorhombic $\theta$-Fe$_3$C (cementite) with transition metals is the notable decline in the Curie temperature. We found that a considerable proportion of the orthorhombic Co$_3$(B-C-N) alloys are magnetically hard, of which boron substitution raises the Curie temperature and improves stability. By mapping the dependence of MAE on the concentration of elements covering both the 3$d$ (from Fe to Co) and 2$p$ (from B, through C, to N) positions, we have demonstrated for the first time the near isoelectronic nature of MAE. The latter observation may be particularly useful in designing compositions of new magnetically hard materials.
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六方和正方Fe$_{3}$C、Co$_{3}$C、(Fe-Co)$_{3}$C及其与硼、氮和过渡金属合金的磁硬性:第一原理研究
在这项研究中,我们考虑了大量与正方体 Fe$_3$C(水泥石)密切相关的材料,目的是描述它们内在磁性能的变化趋势,并确定最适合应用的合金。对(Fe-Co)$_3$C、(Fe-Co)$_3$(B-C)、(Fe-Co)$_3$(C-N)的六方相($\epsilon$)和正方相($\theta$)以及它们与 3d、4d 和 5d 过渡金属的合金的全浓度范围进行了全面分析。计算采用了全势能局域轨道代码(FPLO)中的密度泛函理论。计算得出的特性包括形成能、居里温度、磁矩、磁晶各向异性能(MAE)和磁硬度。所考虑的成分表现出一系列磁性能,包括软磁、半硬磁和硬磁。最有希望用于硬磁性应用的材料是正交钴$_3$C 化合物,以及选定的富钴正交(Fe,Co)$_3$C 和六方(Fe,Co)$_3$C 合金。计算结果并没有表明添加过渡金属会增加合金在永磁应用中的潜力。将正交θ-Fe$_3$C(雪明石)与过渡金属进行合金化的一个显著缺点是居里温度明显下降。我们发现,相当一部分正方晶 Co$_3$(B-C-N)合金具有磁硬性,其中硼的加入可提高居里温度并改善稳定性。通过绘制 MAE 与涵盖 3$d$(从铁到钴)和 2$p$(从 B 到 C 再到 N)位置的元素浓度的关系图,我们首次证明了 MAE 的近似等电子性质。这一观察结果可能对设计新的磁性硬材料成分特别有用。
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