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The creation and transport of spin -polarized carriers in semiconductor heterostructures.

机译:半导体异质结构中自旋极化载流子的产生和传输。

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摘要

In this dissertation we present a theory of the creation and transport of spin-polarized carriers in semiconductor heterostructures. We first present the theory of spin-dependent reflection of semiconductor electrons off the semiconductor-ferromagnet interface. A simplified one-dimensional effective-mass approximation model of the interface is used to elucidate the key physical features in the quantum-mechanical scattering off the spin-dependent ferromagnet band-structure. Spin-dependence under reflection is calculated for both electrical and optical excitation of carriers at or above the Fermi level in the semiconductor, and shows that high spin-polarizations are possible through proper tailoring of the interface properties through material selection or doping. The creation of spin-polarization through reflection is then calculated for the ferromagnet-semiconductor junction under an applied bias. A full three-dimensional calculation shows that efficient spin creation is possible through all-electrical means. We then study systems in which the semiconductor electrons are confined at the interface, specifically in the naturally formed surface layer and in the gate-bias induced inversion layer in the silicon field-effect transistor system. Due to the carriers being confined at the interface, the wavefunction penetrates into the ferromangetic gate and creates the spin-dependent properties. The transport of the spin-polarization through the two-dimensional electron gas is calculated including the effects of carrier leakage into the gate, drift due to an in-plane bias, and diffusion due to a gradient in the two-dimensional electron gas density. Finally, we introduce a device proposal, in which the single ferromagnet is replaced by two adjacent ferromagnets. The channel conductivity can be controlled by the relative orientation of the two ferromagnets' magnetizations (parallel vs. antiparallel), a device which could perform the role of magnetic non-volatile memory on the semiconductor chip.
机译:在这篇论文中,我们提出了一种在半导体异质结构中产生和传输自旋极化载流子的理论。我们首先提出半导体电子从半导体-铁磁体界面上的自旋相关反射的理论。界面的简化一维有效质量近似模型用于阐明自旋相关铁磁体能带结构的量子力学散射中的关键物理特征。对于半导体中费米能级以上的载流子的电和光激发,都计算了反射下的自旋相关性,表明通过材料选择或掺杂适当调整界面特性,可以实现高自旋极化。然后,在施加的偏压下,为铁磁体-半导体结计算通过反射产生的自旋极化。完整的三维计算表明,通过全电方式可以有效地创建自旋。然后,我们研究了其中半导体电子被限制在界面处的系统,特别是在硅场效应晶体管系统中自然形成的表面层和栅极偏置感应的反型层中。由于载流子被限制在界面上,波函数渗透到铁电闸中并产生自旋相关的特性。计算自旋极化通过二维电子气的传输,包括载流子泄漏到栅极,由于面内偏压引起的漂移,以及由于二维电子气密度的梯度引起的扩散的影响。最后,我们介绍一种设备方案,其中单个铁磁体被两个相邻的铁磁体代替。通道电导率可以通过两个铁磁体的磁化强度的相对方向(平行与反平行)来控制,该器件可以在半导体芯片上执行非易失性磁性存储器的作用。

著录项

  • 作者

    McGuire, James P.;

  • 作者单位

    University of California, San Diego.;

  • 授予单位 University of California, San Diego.;
  • 学科 Condensed matter physics.
  • 学位 Ph.D.
  • 年度 2004
  • 页码 98 p.
  • 总页数 98
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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