偏置量子阱中产生极化电子-空穴对的太赫兹脉冲

P. Planken, M. Nuss, W. Knox, D. Miller, K. Goossen
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引用次数: 80

摘要

长期以来,人们一直认为半导体表面太赫兹脉冲的产生是由超短激光脉冲激发后与材料表面耗尽场平行的瞬态输运电流引起的。[1]最近,对这些实验给出了另一种解释,即耗尽场中的光学跃迁在已经极化的状态下产生电子和空穴。[2]这产生了一个极化P,它随着集成脉冲能量的增长而增长,因此辐射出一个符合E~∂2P/∂t2的电瞬态。然而,该过程重要性的最终证明只能在传输电流被抑制的样品中给出!
本文章由计算机程序翻译,如有差异,请以英文原文为准。
THz Pulses from the Creation of Polarized Electron-Hole Pairs in Biased Quantum Wells
The generation of THz pulses on the surface of semiconductors has long been believed to be caused by transient transport currents parallel to the surface depletion field of the material after excitation with an ultrashort laser pulse. [1] Recently, an additional explanation of those experiments was given, in which optical transitions in the depletion field create electrons and holes in states where they are already polarized. [2] This creates a polarization P that grows with the integrated pulse energy, and hence radiates an electrical transient according to E~∂2P/∂t2. The final proof of the importance of this process however, can only be given in a sample where transport current is inhibited!
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