首页> 外文期刊>Physical Review, B. Condensed Matter >Femtosecond time-resolved electron-hole dynamics and radiative transitions in the double-layer quantum well of the CdS/(HgS)(2)/CdS quantum-dot-quantum-well nanoparticle - art. no. 035317
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Femtosecond time-resolved electron-hole dynamics and radiative transitions in the double-layer quantum well of the CdS/(HgS)(2)/CdS quantum-dot-quantum-well nanoparticle - art. no. 035317

机译:飞秒时间分辨的CdS /(HgS)(2)/ CdS量子点量子阱纳米粒子双层量子阱中的电子-空穴动力学和辐射跃迁-艺术。没有。 035317

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摘要

The femtosecond time-resolved exciton dynamics of the CdS/(HgS)(2)/CdS quantum-dot-quantum-well system (QDQW), which contains a double-layer HgS QW, was investigated and compared to the dynamics of the QDQW system with a single-layer HgS QW. The femtosecond hole-burning technique allowed us to resolve the energy of the different optically allowed excitonic states involved in the ultrafast relaxation pathway. The experimentally obtained exciton energies were in excellent agreement with the previously theoretically predicted values. The femtosecond time-resolved pump-probe measurements reveal a fast relaxation component of similar to5 ps at wavelengths less than or equal to 700 nm. At longer wavelengths, a slow decay component is found, which increases in decay time with increasing wavelength. The fast decay component (5 ps) was attributed to an energy relaxation process of the two 1P(e)-1P(h) exciton states, whereas the slow one was assigned to the decay of the dim 1S(e)-1S(3/2) state. The inhomogeneously broadened absorption band and the wide distribution of decay times in the low-energy region give strong evidence for a broad inhomogeneous energy distribution of the lowest energetic 1S(e)-1S(3/2) dim state. This is discussed in terms of the morphological structure of the quantum well. [References: 22]
机译:研究了包含双层HgS QW的CdS /(HgS)(2)/ CdS量子点量子阱系统(QDQW)的飞秒时间分辨激子动力学并将其与QDQW的动力学进行了比较单层HgS QW的系统。飞秒空穴燃烧技术使我们能够解析参与超快弛豫路径的不同光学允许的激子态的能量。实验获得的激子能量与先前的理论预测值非常吻合。飞秒时间分辨的泵浦探针测量结果表明,在小于或等于700 nm的波长处,快速弛豫分量类似于5 ps。在更长的波长处,发现了一个缓慢的衰减分量,衰减分量随波长的增加而增加。快速衰减分量(5 ps)归因于两个1P(e)-1P(h)激子态的能量弛豫过程,而慢速分量被分配给暗淡1S(e)-1S(3)的衰减/ 2)状态。低能区域中吸收带的不均匀加宽和衰减时间的广泛分布,为最低能量的1S(e)-1S(3/2)暗态的较宽的不均匀能量分布提供了有力的证据。这是根据量子阱的形态结构来讨论的。 [参考:22]

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