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Activation Process of GaAs NEA Photocathode and Its Spectral Sensitivity

机译:GaAs Nea光电阴极的激活过程及其光谱敏感性

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Negative electron affinity (NEA) Gallium Arsenide (GaAs) photocathodes with high photo-electric conversion quantum efficiency (QE) and high response speed are expected as an electron source for THz frequency vacuum devices. To achieve high QE and high response speed, further understanding of the electron emission mechanism on NEA GaAs photo-cathodes is necessary. This study focuses on the formation process of NEA photo-electric surface on a GaAs photocathode. The results suggest that NEA photo-electric surface allows the electron emission from both the Γ and L valleys in the conduction band. On the contrary, in the Cs or O excess state, vacuum level is between the conduction band level at Γ and L point, and electrons can emit only from L valley, and cannot be emit-ted from the Γ valley due to the barrier of vacuum level. Contribution of Γ and L valleys to the emission current was confirmed, of which balance depended on photo-electric surface conditions and excitation wavelength.
机译:负电子亲和力(NEA)砷化镓(GaAs)具有高光电转换量子效率(QE)和高响应速度的光电阴极,预计为THz频率真空装置的电子源。为了实现高QE和高响应速度,需要进一步了解NEA GaAs光阴极上的电子发射机制。本研究侧重于GaAs光电阴极上Nea光电表面的形成过程。结果表明,NEA光电表面允许导电带中的γ和L谷的电子发射。相反,在CS或O过量状态下,真空水平在γ和L点的导通带水平之间,电子可以仅从L谷发射,并且由于屏障而不能从γ谷发射真空水平。确认了γ和L谷对发射电流的贡献,其中平衡依赖于光电表面条件和激发波长。

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