用自旋极化正电子湮灭研究铁磁性铁的电子动量分布和自旋密度

P. Genoud, Ashutosh Kumar Singh, A. Manuel, T. Jarlborg, E. Walker, M. Peter, M. Weller
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引用次数: 27

摘要

作者报告了利用极化正电子湮灭辐射的二维角相关对铁磁性铁的费米表面拓扑、电子动量密度和自旋动量密度的首次研究。用自洽线性松饼-锡轨道法在独立粒子模型下进行了计算。实验结果与计算结果的比较表明,由于电子-电子和电子-正电子的相关效应,两者存在明显的差异。实验分布分析表明,与自洽计算结果相比,不存在少数第三波段的n中心大孔袋。为了解释电子-电子相关效应,进行了参数化带结构计算。由此得到的分布比自洽分布更符合实验结果。电子-正电子相关效应的性质再次被发现与Sing等人对镍的观察相似。这证实了局域电子的电子-正电子相关效应的系统趋势。正确描述相对自旋动量密度分布需要对多数电子带和少数电子带进行不同的增强因子。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electron momentum distribution and spin density of ferromagnetic iron studied by spin-polarised positron annihilation
The authors report the first study of the Fermi surface topology, electron momentum density and spin momentum density in ferromagnetic iron using two-dimensional angular correlation of polarised positron annihilation radiation. A calculation made in the independent-particle model was obtained from the self-consistent linear muffin-tin orbital method. Comparison between experiment and calculation reveals marked discrepancies which are due to both electron-electron and electron-positron correlation effects. Analysis of experimental distributions shows that the large N-centred hole pocket of minority third band does not exist in contrast with the self-consistent calculation results. A parametrised band-structure calculation has been performed to account for the electron-electron correlation effects. Distributions resulting from this procedure were in better agreement with experiment than the self-consistent ones. Once again the nature of electron-positron correlation effects is found to resemble those observed by Sing et al. for nickel. This confirms the systematic trends of electron-positron correlation effects for localised d electrons. The correct description of the relative spin momentum density distribution requires different enhancement factors for majority and minority electron bands.
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