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New phases of two-dimensional electrons in excited Landau levels.

机译:激发朗道能级的二维电子新相。

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摘要

The subject of this dissertation is the experimental discovery and investigation of a new class of collective phases in two-dimensional electron systems. The experiments mainly involve magnetotransport measurements in very high quality GaAs/AlGaAs semiconductor heterostructures, where a large perpendicular magnetic field serves to resolve the electrons' energy spectrum into discrete Landau levels. The most dramatic evidence of a new many-body phase is the huge and unprecedented resistance anisotropy observed only below 150 mK and around the half-filling points of the highly excited Landau levels N ≥ 2. Associated with these anisotropic states are other novel electron phases whose transport signature is a vanishing longitudinal conductivity occurring in the flanks of the same excited Landau levels. Although reminiscent of the well-understood integer quantum Hall states, the insulating phases are exceptional for being driven by electron interactions rather than single-particle localization. A persuasive theoretical picture based on "stripe" and "bubble" charge density wave formation in high Landau levels can account for many of the experimental results. For example, the broken orientational symmetry of the stripe state may underlie the observed transport anisotropy, while disorder-induced pinning of the bubble lattice could give rise to the insulating regions in high Landau levels. Further investigation of the anisotropic transport characteristics has elucidated possible symmetry-breaking mechanisms of the purported stripe phase and has provided evidence that the stripes may be more accurately described as a quantum electronic liquid crystal. In addition, experiments involving the breakdown of the insulating regions at high voltage biases may point to a depinning transition of the bubble phase. These results have spurred intense interest in the field of correlated electron systems in two dimensions and may be an indication of the variety of new phenomena in condensed matter systems still awaiting discovery.
机译:本文的主题是二维电子系统中一类新的集体相的实验发现和研究。实验主要涉及在非常高质量的GaAs / AlGaAs半导体异质结构中的磁传输测量,其中大的垂直磁场用于将电子的能谱解析为离散的Landau能级。新的多体相的最戏剧性证据是仅在150 mK以下且在高激发朗道能级N≥2的半填充点附近观察到巨大而前所未有的电阻各向异性。与这些各向异性态相关的还有其他新颖的电子相在相同的朗道能级下,其传输特征是纵向电导率消失。尽管让人联想到众所周知的整数量子霍尔态,但绝缘相却非常适合由电子相互作用而非单粒子局部化驱动。在高朗道水平上基于“条带”和“气泡”电荷密度波形成的有说服力的理论图片可以解释许多实验结果。例如,条带状态的破碎取向对称性可能是观察到的传输各向异性的基础,而气泡晶格的无序诱导钉扎则可能导致高朗道水平的绝缘区域。对各向异性输运特性的进一步研究阐明了所称条纹相的可能的对称破坏机理,并提供了证据,可以将条纹更准确地描述为量子电子液晶。此外,涉及绝缘区在高电压偏压下击穿的实验可能指向气泡相的固定转变。这些结果引起了二维相关电子系统领域的浓厚兴趣,可能表明凝聚态系统中仍在等待发现的新现象的多样性。

著录项

  • 作者

    Cooper, Ken B.;

  • 作者单位

    California Institute of Technology.;

  • 授予单位 California Institute of Technology.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 219 p.
  • 总页数 219
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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