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Confined polar optical phonons in semiconductor double heterostructures: an improved continuum approach

机译:半导体双异质结构中的受限极性光子:一种改进的连续谱方法

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Confined polar optical phonons are studied in a semiconductor double heterostructure (SDH) by using a generalization of the well-known continuous medium model theory. The treatment considers the coupling between the electro-mechanical oscillations and involves dispersive phonon modes. This approach has provided confined phonon frequency dispersions rather different from the dielectric continuum model, where just the electric aspect of these oscillations is analysed. In previous works, the theory had been used to analyse the phonon dispersions within a quadratic (parabolic) approximation, while presently we added the linear contributions by using a straightforward extension of the fundamental equations. This generalized version of the mentioned theoretical treatment leads to a long wavelength polar optical phonon description that shows a closer agreement with experimental data and with calculations along atomistic models. This is particularly important for systems where the linear contribution to dispersion becomes predominant. We present a systematic derivation of the underlying equations and their solutions for bulk and SDH cases. The results provide us with a complete description of the dispersive phonon modes and the associated electron-phonon Hamiltonian. The theory is applied to the case of a EuS/PbS/EuS quantum well.
机译:通过使用众所周知的连续介质模型理论的推广,在半导体双异质结构(SDH)中研究了受限的极性光子。该处理考虑了机电振荡之间的耦合,并涉及了色散声子模式。这种方法提供了局限的声子频率色散,与介电连续模型完全不同,后者仅分析了这些振荡的电方面。在以前的工作中,该理论已用于分析二次(抛物线)近似内的声子色散,而目前,我们使用基本方程的直接扩展来添加线性贡献。所提到的理论处理的这种广义形式导致了长波长极性光学声子的描述,该描述与实验数据和沿原子模型的计算更加吻合。这对色散的线性贡献占主导的系统尤其重要。我们为批量和SDH案例提供了基础方程及其解决方案的系统推导。结果为我们提供了色散声子模态和相关的电子声子哈密顿量的完整描述。该理论适用于EuS / PbS / EuS量子阱的情况。

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