论文标题

GAAS金属n型纳米线的电荷和自旋运输在纪录距离上:ii非线性电荷传输

Charge and spin transport over record distances in GaAs metallic n-type nanowires : II nonlinear charge transport

论文作者

Hijazi, Hadi, Paget, Daniel, Monier, Guillaume, Grégoire, Gabin, Leymarie, Joël, Gil, Evelyne, Cadiz, Fabian, Robert-Goumet, Christine, André, Yamina

论文摘要

我们已经研究了在N型金属GAAS纳米线(〜10^17 cm^-3掺杂水平)中的光载体电荷转运,该载体由Si(111)底物上的Hydride Vapor蒸气相外交(HVPE)生长。分析光谱中选定能量的发光强度空间曲线,使我们能够确定光电子,少数族裔光孔和费米海的电子的空间分布,这是距光激发点的距离的函数。该分析表明,尽管预期在供体浓度的统计波动产生的潜在波动中,但电荷可以在6K时以大于25(微)m的记录距离(微型)m的速度运输。结果表明,由于大型内部电场的积累,该运输几乎不受波动的影响,从而强烈增加了孔和电子迁移率,因此可以运输。比较由于热电子和费米海引起的排放的空间曲线提供了至少三个空间区域的证据,包括在激发点附近过量的内在电子和耗尽的区域,这些距离大于2-10(微型)M,根据激发功率。内部向外电场增加了波动中光孔的动能,因此在与激发点的给定距离之后,会在波动上发生弹道传输。

We have investigated the photocarrier charge transport in n-type metallic GaAs nanowires (~ 10^17 cm^-3 doping level), grown by hydride vapor phase epitaxy (HVPE) on Si(111) substrates. Analysis of the luminescence intensity spatial profiles for selected energies in the spectrum allows us to determine the spatial distribution of photoelectrons, minority photoholes and electrons of the Fermi sea as a function of distance from the light excitation spot. This analysis shows that charge can be transported over record distances larger than 25 (micro)m at 6K, in spite of the expected localization of minority holes in the potential fluctuations generated by statistical fluctuations of the donor concentration. It is shown that transport is little affected by the fluctuations because of the build up of large internal electric fields which strongly increase the hole and electron mobilities and therefore enable transport. Comparison of the spatial profiles of the emissions due to hot electrons and to the Fermi sea gives evidence for at least three spatial zones, including a zone of excess intrinsic electrons near the excitation spot and a zone of depletion of these electrons at a distance larger than 2-10 (micro)m depending on excitation power. The internal outward electric field increases the kinetic energy of photoholes in the fluctuations so that after a given distance to the excitation spot, there occurs ballistic transport over the fluctuations.

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