模拟半导体的载流子动力学以理解它们的太赫兹发射(会议报告)

E. Castro-Camus, M. Alfaro-Gomez, S. C. Corzo-Garcia, A. Hernandez-Serrano, O. Mitrofanov
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引用次数: 0

摘要

我们使用蒙特卡罗模型模拟了块体InAs, InGaAs和GaAs在超快光激发后导致太赫兹发射的半经典光载流子动力学。这个详细的模型使我们能够理解太赫兹发射过程的各个方面,包括实验观察到的近场分布,过量激发光子能量的作用,以及表面场驱动,扩散(photodember)和弹道电流的相对重要性。为了理解近场发射,我们将有限差分时域程序耦合到载流子动力学模拟中,通过这样做,我们能够分析由这些载流子的运动引起的近太赫兹场发射,即使在正常入射激发时也是如此。我们发现,传统上认为不参与发射的平行电流和垂直于界面的电流在太赫兹产生中都起着相关的作用。我们对不同的带隙和激发光子能量进行了另一组模拟,以比较所有三种半导体的发射功率作为激发光子能量的函数,发现载流子多余的激发能量比它们的运动率更能解释它们的性能差异。我们得出结论,光激发后的弹道输运是太赫兹发射的主要机制,而不是扩散驱动或表面场驱动的电荷分离,这是传统上被认为最相关的机制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Modelling the carrier dynamics of semiconductors to understand their terahertz emission (Conference Presentation)
We use a Monte-Carlo model to simulate semi-classical photo-carrier dynamics on bulk InAs, InGaAs and GaAs that leads to terahertz emission after ultrafast photoexcitation. This detailed model has allowed us to understand various aspects of the THz emission process, including the near-field distribution which has been experimentally observed, the role of the excess excitation photon energy, and the relative importance of the surface field driven, diffusive (photo-Dember) and ballistic currents. In order to understand the near-field emission we coupled a finite-difference time-domain routine to the carrier dynamics simulation, by doing this, we were able to analyse the near terahertz field emission caused by the motion of such carriers even when the excitation is performed at normal incidence. We found that both the current parallel, which has traditionally been assumed not to take part in the emission, and normal to the interface take a relevant role in the terahertz generation. We performed another set of simulations for different bandgaps and excitation-photon energies in order to compare the emission power of all three semiconductors as function of excitation photon energy finding that the carrier excess excitation energy is more relevant to explain their performance difference than their motilities. We conclude that ballistic transport after photoexcitation is the dominant mechanism for terahertz emission instead of diffusion driven or surface field driven charge separation, which were traditionally considered the most relevant mechanisms.
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