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A study of spin-dependent electron inelastic mean free path and spin excitations in ferromagnetic metals.

机译:铁磁金属中自旋相关的电子非弹性平均自由程和自旋激发的研究。

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摘要

We explore the spin dependence of the inelastic mean free path of an excited electron and spin excitations in ferromagnetic transition metals. In chapter 1, we present simple one band Hubbard model calculations of the dependence of the inelastic mean free path (IMFP) on the spin direction and energy. The excited electron is assumed to reside in a plane wave state, while the metal electrons are modeled within the framework of a one band Hubbard model. We consider scattering by both Stoner excitations and by spin waves, and outline their relative importance in various energy ranges. In addition, we explore the dependence of the inelastic mean free path on the number of holes in the spin polarized energy bands of the substrate.; In chapter 2, we present explicit calculations based on the realistic model, for propagation in the bulk of the ferromagnetic metals Fe and Ni. The substrate electrons are modeled within the framework of an empirical tight binding description of the 3d, 4s and 4p bands combined with intra atomic Coulomb interactions between electrons in the 3d shell. The analysis of spin flip contributions to the inelastic mean free path incorporates the role of spin wave emission. We discuss the energy variation of the spin asymmetry in the mean free path, along with other issues. We find for electrons a few eV above the vacuum level that the mean free path of minority spin electrons is very short.; In chapter 3, we present theoretical calculations of the contribution to the spin polarized electron energy loss (SPEELS) spectrum of ferromagnetic Ni. We find, save for the wave vector transfer near the center of the Brillouin zone, the spin wave loss feature is obscured by low lying Stoner excitations, in contrast to Fe. Our calculations show that in inelastic neutron scattering studies of spin waves in Ni, the spin wave loss peak dominates. The physical reason for this difference is discussed.
机译:我们探讨了受激电子的非弹性平均自由程的自旋依赖性以及铁磁过渡金属中的自旋激发。在第一章中,我们介绍了简单的单频带Hubbard模型计算,该模型计算了非弹性平均自由程(IMFP)对自旋方向和能量的依赖性。假定被激发的电子处于平面波状态,而金属电子则在单带Hubbard模型的框架内建模。我们考虑了斯托纳激发和自旋波的散射,并概述了它们在各种能量范围内的相对重要性。此外,我们探索了非弹性平均自由程对基底自旋极化能带中空穴数量的依赖性。在第二章中,我们提出了基于实际模型的显式计算,用于大量铁磁性金属Fe和Ni的传播。在3d,4s和4p带的经验紧密结合描述的框架内,结合3d壳层中电子之间的原子内库仑相互作用,对基质电子进行建模。自旋翻转对非弹性平均自由程的贡献分析包含了自旋波发射的作用。我们讨论了平均自由程中自旋不对称的能量变化以及其他问题。我们发现,对于电子,比真空能级高出几个eV,少数自旋电子的平均自由程非常短。在第3章中,我们介绍了对铁磁Ni自旋极化电子能量损失(SPEELS)谱的贡献的理论计算。我们发现,除了在布里渊区中心附近的波矢量转移外,与Fe相比,自旋波损耗特征被低位的Stoner激发所掩盖。我们的计算表明,在Ni中自旋波的非弹性中子散射研究中,自旋波损耗峰占主导地位。讨论了造成这种差异的物理原因。

著录项

  • 作者

    Hong, Jisang.;

  • 作者单位

    University of California, Irvine.;

  • 授予单位 University of California, Irvine.;
  • 学科 Physics Condensed Matter.; Physics Electricity and Magnetism.
  • 学位 Ph.D.
  • 年度 2000
  • 页码 90 p.
  • 总页数 90
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 电磁学、电动力学;
  • 关键词

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