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Inelastic electron and light scattering from the elementary electronic excitations in quantum wells: Zero magnetic field

机译:量子阱中基本电子激发的非弹性电子和光散射:零磁场

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The most fundamental approach to an understanding of electronic, optical, and transport phenomena which the condensed matter physics (of conventional as well as nonconventional systems) offers is generally founded on two experiments: the inelastic electron scattering and the inelastic light scattering. This work embarks on providing a systematic framework for the theory of inelastic electron scattering and of inelastic light scattering from the electronic excitations in GaAs/Ga1?x Al x As quantum wells. To this end, we start with the Kubo's correlation function to derive the generalized nonlocal, dynamic dielectric function, and the inverse dielectric function within the framework of Bohm-Pines’ random-phase approximation. This is followed by a thorough development of the theory of inelastic electron scattering and of inelastic light scattering. The methodological part is then subjected to the analytical diagnoses which allow us to sense the subtlety of the analytical results and the importance of their applications. The general analytical results, which know no bounds regarding, e.g., the subband occupancy, are then specified so as to make them applicable to practicality. After trying and testing the eigenfunctions, we compute the density of states, the Fermi energy, the full excitation spectrum made up of intrasubband and intersubband – single-particle and collective (plasmon) – excitations, the loss functions for all the principal geometries envisioned for the inelastic electron scattering, and the Raman intensity, which provides a measure of the real transitions induced by the (laser) probe, for the inelastic light scattering. It is found that the dominant contribution to both the loss peaks and the Raman peaks comes from the collective (plasmon)excitations. As to the single-particle peaks, the analysis indicates a long-lasting lack of quantitative comparison between theory and experiments. It is inferred that the inelastic electron scattering can be a potential alternative of the inelastic light scattering for investigating elementary electronic excitations in quantum wells.
机译:凝聚态物理(常规系统和非常规系统)提供的了解电子,光学和传输现象的最基本方法通常基于两个实验:非弹性电子散射和非弹性光散射。这项工作着手为GaAs / Ga1xx Al x As量子阱中电子激发的非弹性电子散射和非弹性光散射理论提供系统的框架。为此,我们从Kubo的相关函数开始,以在Bohm-Pines随机相位近似的框架内得出广义的非局部动态介电函数和逆介电函数。随后,对非弹性电子散射和非弹性光散射理论进行了全面的发展。然后对方法论部分进行分析诊断,这使我们能够感觉到分析结果的微妙之处及其应用的重要性。然后规定了一般的分析结果,该结果没有关于例如子带占用的限制,因此使其适用于实用性。在尝试并测试了本征函数之后,我们计算了状态密度,费米能量,由子带内和子带间(单粒子和集体(等离激元))激发组成的完整激发光谱,针对所有主要几何构想的损耗函数非弹性电子散射和拉曼强度,用于测量非激光散射的(激光)探针引起的实际跃迁。发现对损失峰和拉曼峰的主要贡献来自集体(等离子体激元)激发。对于单颗粒峰,分析表明理论和实验之间长期缺乏定量比较。可以推断,非弹性电子散射可以作为非弹性光散射的潜在替代物,用于研究量子阱中的基本电子激发。

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