利用增强面内扩散输运法超高速恢复杂态n-i-p-i

A. Smirl, D. McCallum, A. N. Cartwright, X. R. Huang, T. Boggess, T. Hasenberg
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引用次数: 0

摘要

Hetero n-i-p-i是几种使用二阶电光效应的半导体量子阱器件之一,并且在低功耗二维开关阵列和全光空间光调制器的可能应用中继续引起人们的兴趣。异态n-i-p-i器件的导通时间通常由垂直于量子阱的输运决定。更具体地说,它是由量子阱中产生的载流子逃离量子阱并移动到屏蔽内置电场从而移动激子所需的时间决定的。因此,典型的导通时间约为几ps。相比之下,当用于传统的单光束几何结构时,异态n-i-p-i的恢复(或关断)时间由掺杂区域中空间分离电荷的缓慢重组决定,通常在µs-ms范围内。然而,如果我们为器件使用双光束混合几何(其中光栅通过两束的干涉写入材料中),则信号的衰减或关闭由微米尺寸上的平面内传输光栅的衰减决定。在这里,我们使用瞬态光栅技术来测量这种光折变和光吸收光栅的恢复,这些光栅写在全二进制异质n-i-p-i's中。在这种几何结构中,我们表明,光产生电荷的分离实际上通过将有效的面内双极性扩散系数提高大约一个数量级来加速恢复(与单束几何结构相反,电荷分离延长了复合和恢复时间)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Ultrafast Recovery of Hetero n-i-p-i's by Enhanced In-plane Diffusive Transport
Hetero n-i-p-i's are one of several semiconductor quantum-well devices that use second-order electro-optic effects and that continue to attract interest for possible applications to low-power two-dimensional switching arrays and all-optical spatial light modulators. The turn-on time for a hetero n-i-p-i device is usually determined by transport perpendicular to the quantum wells. More specifically, it is determined by the time required for carriers generated in the quantum wells to escape the wells and to move to screen the built-in electric field, thus shifting the exciton. Consequently, typical turn-on times are of the order of a few ps. By contrast, when used in the conventional single-beam geometry, the recovery (or turn-off) time of hetero n-i-p-i's is determined by the slow recombination of the spatially-separated charges in the doped regions and is typically in the range of µs-ms. If instead, however, we use a two-beam mixing geometry for the device (where gratings are written in the material by the interference of the two beams), then the decay or turn off of the signal is determined by the decay of the gratings by in-plane transport over micron dimensions. Here, we use transient grating techniques to measure the recovery of such photorefractive and photoabsorptive gratings written in all-binary hetero n-i-p-i's. In this geometry, we show that the separation of photo-generated charge actually speeds the recovery by enhancing the effective in-plane ambipolar diffusion coefficient by roughly an order of magnitude (in contrast to the single beam geometry where charge separation elongates the recombination and recovery time).
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