用消相碰撞增强GaAs量子阱中二维激子的辐射寿命

J. Kuhl, A. Honold, L. Schultheis, C. Tu
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引用次数: 0

摘要

半导体中激子的非线性光学特性和超快动力学是目前半导体研究的一个重要领域。激子非线性在未来光通信系统中作为超快光开关器件的潜在应用解释了这种兴趣。在最近的一篇理论论文中,Hanamura /1/讨论了量子阱中激子作为一种结合大三阶非线性磁化率χ(3)和快速响应的非线性光学介质的优点。其χ(3)的强增强解释为量子阱中激子的宏观跃迁偶极矩和受限激子的快速辐射衰减的结果。Hanamura计算出QW中的激子应该在几皮秒内通过其宏观偶极子跃迁瞬间进行超辐射衰减。然而,这种超辐射衰减需要材料的相干偏振,如果被激发激子的空间和时间相干性被激子与其环境的相互作用破坏,则会大大减少。费尔德曼等人最近预测了辐射寿命τ r与减相T2之间的紧密联系。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Enhancement of the Radiative Lifetime of 2D Excitons in a GaAs Quantum Well by Dephasing Collisions
The nonlinear optical properties and the ultrafast dynamics of excitons in semiconductors are a major field of present semiconductor research. This interest is explained by the potential applications of excitonic nonlinearities as ultrafast optical switching devices in future optical communication systems. In a recent theoretical paper Hanamura /1/ discussed the advantages of excitons in a quantum well (QW) as a nonliner optical medium combining large 3rd order nonlinear susceptibility χ(3) with a fast response. The strong enhancement of is χ(3) explained as a consequence of both the macroscopic transition dipole moment of the exciton in a QW and the rapid radiative decay of the confined excitons. Hanamura calculated that an exciton in a QW should decay superradiantly through its macroscopic dipole transition moment within a few picoseconds. This superradiant decay requires, however, a coherent polarization of the material and will be strongly reduced if the spatial and temporal coherence of the excited excitons is destroyed by interaction of the excitons with their environment. Such a tight connection between the radiative lifetime τ r and the dephasing T2 has been recently predicted by Feldmann et al. /2/.
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