Laves相
基态
铁磁性
材料科学
从头算
反铁磁性
凝聚态物理
磁矩
结晶学
物理
金属间化合物
原子物理学
化学
量子力学
复合材料
合金
作者
Xing‐Qiu Chen,W. Wolf,R. Podloucky,P. Rogl,Martijn Marsman
标识
DOI:10.1103/physrevb.72.054440
摘要
By an ab initio density functional approach the structural and phase stability, electronic and magnetic properties, elastic constants, phonon dispersion, and defect formation of the Laves-phase compound $\mathrm{Zr}{\mathrm{Mn}}_{2}$ for the C15, C14, and C36 crystal structures were investigated. In order to study the stability of magnetic phases, nonmagnetic and spin polarized calculations for ferro- and antiferromagnetic orderings were performed. At low temperatures, the ferromagnetic cubic C15 phase was obtained as the ground state, with the ferromagnetic hexagonal C14 and C36 phases being almost degenerate in energy. From the calculated temperature-dependent free energies a structural transformation from C15 to C14 at about ${T}_{tr}=200\phantom{\rule{0.3em}{0ex}}\mathrm{K}$ is predicted, confirming the experimentally observed C14 structure at elevated temperatures. Elastic properties were investigated for the nonmagnetic and ferromagnetic C14 and C15 phases. Structural stability studies based on the calculated temperature-dependent free vibrational energies very strongly favor the existence of ferromagnetic phases. Point defect formation properties for vacancies and antiste defects were calculated by combining a supercell approach with a statistical mechanics model. Mn antisites are the most favorable defects broadening the homogeneity range of the $\mathrm{Zr}{\mathrm{Mn}}_{2}$ phase toward the Mn-rich side. The existence of ordered Mn-rich compounds is predicted. Large magnetic moment of $3\phantom{\rule{0.3em}{0ex}}{\ensuremath{\mu}}_{B}$ for Mn antisite defects are derived.
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