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First-principles investigation of magnetism and electronic structures of substitutional $3d$ transition-metal impurities in bcc Fe

机译:磁性和电子结构的第一性原理研究   bcc Fe中的替代$ 3d $过渡金属杂质

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摘要

The magnetic and electronic structures of $3d$ impurity atoms from Sc to Znin ferromagnetic body-centered cubic iron are investigated using theall-electron full-potential linearized augmented plane-wave method based on thegeneralized gradient approximation (GGA). We found that in general, the GGAresults are closer to the experimental values than those of the local spindensity approximation. The calculated formation enthalpy data indicate theimportance of a systematic study on the ternary Fe-C-$X$ systems rather thanthe binary Fe-$X$ systems, in steel design. The lattice parameters areoptimized and the conditions for spin polarization at the impurity sites arediscussed in terms of the local Stoner model. Our calculations, which areconsistent with previous work, imply that the local spin-polarizations at Sc,Ti, V, Cu, and Zn are induced by the host Fe atoms. The early transition-metalatoms couple antiferromagnetically, while the late transition-metal atomscouple ferromagnetically, to the host Fe atoms. The calculated totalmagnetization ($M$) of bcc Fe is reduced by impurity elements from Sc to Cr asa result of the antiferromagnetic interaction, with the opposite effect forsolutes which couple ferromagnetically. The changes in $M$ are attributed tonearest neighbor interactions, mostly between the impurity and host atoms. Theatom averaged magnetic moment is shown to follow generally the well-knownSlater-Pauling curve, but our results do not follow the linearity of theSlater-Pauling curve. We attribute this discrepancy to the weak ferromagneticnature of bcc Fe. The calculated Fermi contact hyperfine fields follow thetrend of the local magnetic moments. The effect of spin-orbit coupling is foundnot to be significant although it comes into prominence at locations far fromthe impurity sites.
机译:利用基于广义梯度近似(GGA)的全电子全势线性化增强平面波方法研究了从Sc到锌的三价body原子从Sc到Zn的磁性和电子结构。我们发现,一般而言,GGA结果比局部自旋密度近似值更接近实验值。计算得出的地层焓数据表明,在钢设计中系统研究三元Fe-C- $ X $系统而不是二元Fe- $ X $系统的重要性。根据局部斯托纳模型,优化了晶格参数,讨论了杂质位点的自旋极化条件。我们的计算与先前的工作一致,这表明Sc,Ti,V,Cu和Zn处的局部自旋极化是由主体Fe原子引起的。早期的过渡金属原子反铁磁耦合,而后期的过渡金属原子铁磁耦合至主体Fe原子。由于反铁磁相互作用,杂质元素从Sc还原为Cr,计算出的bcc Fe的总磁化强度($ M $)减少了,而溶质以铁磁耦合的方式则具有相反的效果。 $ M $的变化归因于最近的邻居相互作用,主要是杂质和主体原子之间的相互作用。原子平均磁矩通常显示为遵循众所周知的Slater-Pauling曲线,但我们的结果不遵循Slater-Pauling曲线的线性。我们将此差异归因于bcc Fe的弱铁磁性。计算出的费米接触超精细场遵循局部磁矩的趋势。尽管自旋-轨道耦合的作用在远离杂质位点的位置上已经很突出,但它的作用并不显着。

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