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Electrical spin generation by the spin Hall effect in semiconductors.

机译:半导体中的自旋霍尔效应产生电自旋。

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摘要

Electrical generation of spin polarization by the spin Hall effect is imaged with both spatial and temporal resolution using Kerr rotation microscopy in bulk zincblende semiconductors. The spin Hall effect, which arises due to the spin-orbit coupling, refers to the generation of a pure spin current transverse to a charge current driven by an electric field which causes a spontaneous quasi-equilibrium spin accumulation near sample boundaries without the need for magnetic fields or magnetic materials. Bulk current-induced in-plane spin polarization and out-of-plane spin accumulation from the spin Hall effect are observed in the II-VI semiconductor ZnSe despite no evidence for a spin-orbit induced internal magnetic field, which are only observed sub-critical thickness ZnSe with enhanced k-linear Hamiltonian terms due to biaxial strain. The wide band gap of ZnSe enables the first observation of electrical spin generation at room temperature. The spatial dependence of steady-state spin accumulation from the spin Hall effect is addressed in channels made of the III-V semiconductor GaAs. One- and two-dimensional spatially-resolved diffusion modeling clarifies the important role of drift and diffusion in transporting spin generated at sample boundaries to the interior of the device. Driving spin accumulation with an electrical pulse and probing with a frequency-synchronized ultrafast laser enables time-resolved measurement of the spin Hall effect. Probing the dynamical processes of spin accumulation and diffusion reveals spatially-dependent nanosecond timescales comparable to the electric-field dependent spin coherence time. Prospects are considered for an all-electrical measurement of the spin Hall effect which should enable more accurate determination of the magnitude of the spin Hall conductivity and illuminate the microscopic mechanisms governing the spin Hall effect in GaAs.
机译:使用块状闪锌矿半导体中的Kerr旋转显微镜,通过自旋霍尔效应产生的自旋极化电以空间和时间分辨率进行成像。由于自旋-轨道耦合而产生的自旋霍尔效应是指产生与电场驱动的电荷电流横向的纯自旋电流,该电场导致在样品边界附近自发的准平衡自旋累积,而无需磁场或磁性材料。尽管没有证据表明自旋轨道引起的内部磁场,但在II-VI半导体ZnSe中仍观察到了大电流引起的面内自旋极化和自旋霍尔效应引起的面外自旋累积,尽管没有证据表明自旋轨道产生了内部磁场。临界厚度ZnSe由于双轴应变而具有增强的k线性哈密顿项。 ZnSe的宽带隙使人们能够首次观察到室温下电自旋的产生。自旋霍尔效应引起的稳态自旋累积的空间依赖性在由III-V半导体GaAs制成的通道中得到解决。一维和二维空间分辨扩散模型阐明了漂移和扩散在将样品边界处产生的自旋传输到器件内部的重要作用。利用电脉冲驱动自旋累积并使用频率同步的超快激光进行探测,可以实现时间分辨的自旋霍尔效应测量。探测自旋积累和扩散的动力学过程揭示了与电场相关的自旋相干时间可比的空间相关纳秒时标。考虑了自旋霍尔效应的全电测量的前景,这应该能够更准确地确定自旋霍尔电导率的大小,并阐明控制GaAs中自旋霍尔效应的微观机制。

著录项

  • 作者

    Stern, Nathaniel P.;

  • 作者单位

    University of California, Santa Barbara.;

  • 授予单位 University of California, Santa Barbara.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2008
  • 页码 316 p.
  • 总页数 316
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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