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Coulomb interactions in Hanbury Brown-Twiss experiments with electrons.

机译:Hanbury Brown-Twiss实验中的库仑与电子的相互作用。

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摘要

This dissertation examines the effect of Coulomb interactions in Hanbury Brown--Twiss (HBT) type experiments with electrons. HBT experiments deal with intensity interference, which is related to the second-order correlation function of the particle field. This is an extension of the usual amplitude interference experiment, such as Young's double-slit experiment and the Michelson interferometry, which are related to the first-order correlation function of the particle field. Depending on the exchange symmetry (or anti-symmetry) of the wave function for identical bosons (or fermions) at the detectors, the second-order correlation function shows an enhancement (or a reduction) at small separation with respect to the statistical independent value, i.e., a correlation of the intensities at small separation, either in real or momentum space.;Following this idea, several experiments have been done with electrons under various experimental conditions for the purpose of demonstrating the HBT effect with fermions, the effect due to the exchange anti-symmetry of the wave function for fermions, i.e., Fermi-Dirac statistics. The experiments, however, have been previously analyzed in the formalism of non-interacting fermions, neglecting the effect of Coulomb interactions between electrons. The experimental data need to be more carefully analyzed and the experiments better understood. We examine the experimental setup in detail and construct a classical model to show that Coulomb interaction is in fact dominant over quantum statistics under certain experimental conditions, and calculate the corrections due to Coulomb interactions in these cases.;The second-order correlation function, i.e., the intensity correlation function, is not the only characterization of the two-particle interference. There are other different yet equivalent characterizations, which we examine in this thesis. We investigate the relationship between different characterizations and illustrate the connections between them.
机译:本文研究了库伯相互作用在汉伯里布朗-特维斯(HBT)型电子实验中的作用。 HBT实验处理强度干扰,这与粒子场的二阶相关函数有关。这是常规振幅干涉实验的扩展,例如与粒子场的一阶相关函数有关的杨氏双缝实验和迈克尔逊干涉法。根据检测器处相同玻色子(或费米子)的波动函数的交换对称性(或反对称性),二阶相关函数相对于统计独立值在较小的间距处显示出增强(或减少)。遵循这个想法,为了证明费米子具有HBT效应,电子在各种实验条件下进行了几次实验,这是由于波函数对费米子的交换反对称性,即费米-狄拉克统计。然而,先前已经在非相互作用的费米子形式上对实验进行了分析,而忽略了电子之间的库仑相互作用的影响。需要更仔细地分析实验数据并更好地理解实验。我们将详细研究实验设置并构建一个经典模型,以表明在某些实验条件下,库仑相互作用实际上比量子统计更占优势,并在这些情况下计算出由于库仑相互作用而产生的校正量。二阶相关函数,即强度相关函数不是两个粒子干涉的唯一特征。在本文中我们还将研究其他不同但等效的特征。我们研究了不同特征之间的关系,并说明了它们之间的联系。

著录项

  • 作者

    Shen, Kan.;

  • 作者单位

    University of Illinois at Urbana-Champaign.;

  • 授予单位 University of Illinois at Urbana-Champaign.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2009
  • 页码 82 p.
  • 总页数 82
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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