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Theory of highly excited semiconductor nanostructures including Auger coupling: exciton-bi-exciton mixing in CdSe nanocrystals

机译:包括俄歇在内的高激发半导体纳米结构理论   耦合:激子 - 双激子在Cdse纳米晶体中混合

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摘要

We present a theory of highly excited interacting carriers confined in asemiconductor nanostructure, incorporating Auger coupling between excitedstates with different number of excitations. The Coulomb matrix elementsconnecting exciton, bi-exciton and tri-exciton complexes are derived and anintuitive picture of breaking neutral multi-exction complexes into positivelyand negatively charged multi-exciton complexes is given. The general approachis illustrated by analyzing the coupling of biexciton and exciton in CdSespherical nanocrystals. The electron and hole states are computed usingatomistic $sp^3d^5s^*$ tight binding Hamiltonian including an effective crystalfield splitting and surface passivation. For each number of electron-hole pairsthe many-body spectrum is computed in the configuration-interaction approach.The low-energy correlated biexciton levels are broken into charged complexes: ahole and a negatively charged trion and an electron and a positively chargedtrion. Out of a highly excited exciton spectrum a subspace coupled tobi-exciton levels via Auger processes is identified. The interaction betweencorrelated bi-exciton and exciton states is treated using exact diagonalizationtechniques. This allows to extract the spectral function of the biexciton andrelate its characteristic width and amplitude to the characteristic amplitudeand timescale of the coherent time evolution of the coupled system. It is shownthat this process can be described by the Fermi's Golden Rule only if a fastrelaxation of the excitonic subsystem is accounted for.
机译:我们提出了一种限制在半导体纳米结构中的高激发相互作用载流子的理论,并结合了具有不同数量激发的激发态之间的俄歇耦合。推导了连接激子,双激子和三激子复合物的库仑矩阵元素,给出了将中性多交换复合物分解为带正负电的多激子复合物的直观图。通过分析Cd球形纳米晶体中双激子和激子的耦合来说明一般方法。电子和空穴态的计算使用原子学上的$ sp ^ 3d ^ 5s ^ * $紧密结合的哈密顿量,包括有效的晶体分裂和表面钝化。对于每个数量的电子-空穴对,都采用构型-相互作用方法计算了多体光谱。低能相关的双激子能级被分解为带电复合物:空穴和带负电的三子,以及电子和带正电的三子。在高激发态激子谱中,确定了通过俄歇过程耦合双激子能级的子空间。相关的双激子态和激子态之间的相互作用使用精确的对角化技术进行处理。这允许提取双激子的谱函数并将其特征宽度和幅度与耦合系统的相干时间演化的特征幅度和时标相关。结果表明,只有考虑了激子子系统的快速松弛,才能用费米黄金定律描述这一过程。

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