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Polaron effect on Raman scattering in semiconductor quantum dots

机译:极化子对半导体量子点中拉曼散射的影响

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Strong coupling of a confined exciton to optical phonons in semiconductor quantum dots (QDs) leading to the formation of a polaron is considered for a model system including two lowest exciton states and several optical phonon modes. Both intra- and inter-level terms are taken into account. The Hamiltonian has been exactly diagonalized including a finite number of phonons allowed for each mode, large enough to guarantee that the result can be considered exact in the physically important region of energies. Based on this polaron spectrum, the Raman scattering probability is obtained, which is compared with the one calculated using the standard perturbation theory approach. It is shown that, when either diagonal or non-diagonal coupling is sufficiently strong, the Raman spectrum line shape and especially its resonant behaviour differ considerably from the perturbation theory predictions. The dependence of the scattering intensity on the excitation wavelength contains features similar to those expected in the optical absorption spectra of QDs.
机译:对于包括两个最低激子态和几种光学声子模的模型系统,考虑了约束激子与半导体量子点(QDs)中光子的强耦合导致极化子的形成。级别内和级别间的术语都被考虑在内。哈密​​顿量已精确对角化,包括每种模式所允许的有限数量的声子,其大小足以确保在能量的物理重要区域中可以认为结果是精确的。基于该极化子谱,获得拉曼散射概率,并将其与使用标准微扰理论方法计算的拉曼散射概率进行比较。结果表明,当对角或非对角耦合足够强时,拉曼光谱线的形状,尤其是其共振行为与微扰理论的预测有很大不同。散射强度对激发波长的依赖性包含与QD的光吸收光谱中预期的特征相似的特征。

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