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Optical two-dimensional Fourier transform spectroscopy of semiconductors.

机译:半导体的光学二维傅里叶变换光谱。

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摘要

Optical two-dimensional (2D) Fourier transform spectroscopy (FTS) is implemented in the near-IR regime and employed for the study of exciton dynamics, many-body interactions, and disorders in semiconductors. As the optical analog of multidimensional nuclear magnetic resonance, 2D FTS is based on a highly enhanced transient four-wave mixing (FWM) experiment. A FWM signal is generated by a non-collinear three-pulse sequence and heterodyne-detected with a reference to provide both amplitude and phase. With active interferometric stabilization and scanning, the evolution of FWM electric field is coherently tracked and presented on a 2D map of the absorption and emission frequencies. With capabilities that include disentangling congested spectra, identifying resonant coupling, isolating coherent pathways, determining inhomogeneous broadening, and separating complex spectra into real and imaginary parts, 2D FTS is a powerful tool to resolve problems in traditional FWM spectroscopies.;In a typical 2D spectrum of semiconductor quantum wells, diagonal peaks arise from exciton resonances and cross peaks represent their coupling, with features such as cross peak strength and absorption of continuum dominated by many-body interactions. Based on the modified optical Bloch equations with phenomenological terms including excitation-induced dephasing, excitation-induced shift, and local field effect, numerical calculations are performed to reproduce these features and determine the microscopic origin of many-body effects by comparing to the experimental amplitude and real part spectra. The dependence of 2D spectra on the excitation polarization is employed to further explore the many-body interactions. In comparison with microscopic calculations with contributions of Pauli blocking, Hartree-Fock approximation, and higher-order Coulomb correlations, it is found that exciton correlations play the dominant role in the case of cocircular-polarized excitation. With an alternative 2D projection, Raman coherences between excited excitons are isolated. The experimental and calculated 2D spectra in this form also demonstrate the similar result on exciton correlations.
机译:光学二维(2D)傅里叶变换光谱(FTS)在近红外条件下实现,并用于研究激子动力学,多体相互作用和半导体中的无序现象。作为多维核磁共振的光学类似物,二维FTS基于高度增强的瞬态四波混合(FWM)实验。 FWM信号由非共线三脉冲序列生成,并通过参考进行外差检测以提供幅度和相位。通过主动干涉稳定和扫描,可以连贯地跟踪FWM电场的演变,并在吸收和发射频率的二维图上显示出来。 2D FTS具有解决复杂FWM光谱问题的强大功能,包括解开拥塞光谱,识别共振耦合,隔离相干路径,确定不均匀展宽以及将复杂光谱分为实部和虚部,这些功能非常强大。在半导体量子阱中,对角峰是由激子共振产生的,交叉峰代表它们的耦合,具有诸如交叉峰强度和吸收多体相互作用占主导的连续谱之类的特征。基于带有现象学术语的改进的光学布洛赫方程,包括激发诱发的相移,激发诱发的位移和局部场效应,进行了数值计算以再现这些特征,并通过与实验振幅进行比较来确定多体效应的微观起源和实部光谱。利用二维光谱对激发极化的依赖性进一步研究了多体相互作用。与具有Pauli阻塞,Hartree-Fock近似和高阶库仑相关性的微观计算相比,发现在激圆相关性中,激子相关性起着主导作用。使用替代的2D投影,可以分离激发激子之间的拉曼相干性。以这种形式进行的实验和计算二维光谱也证明了激子相关性的相似结果。

著录项

  • 作者

    Zhang, Tianhao.;

  • 作者单位

    University of Colorado at Boulder.;

  • 授予单位 University of Colorado at Boulder.;
  • 学科 Physics Condensed Matter.;Physics Optics.
  • 学位 Ph.D.
  • 年度 2008
  • 页码 157 p.
  • 总页数 157
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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