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首页> 外文期刊>Physica status solidi >Surface behavior based on ion-induced secondary electron emission from semi-insulating materials in breakdown evolution
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Surface behavior based on ion-induced secondary electron emission from semi-insulating materials in breakdown evolution

机译:击穿过程中基于离子诱导的半绝缘材料二次电子发射的表面行为

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摘要

This Much focuses on analyses of secondary electron emission (SEE) at semiconductor surfaces when (he sufficient conditions of space-time distribution occur. Experimental measurements and calculations with the approach of Townsend coefficients, which include the evaluations of ionization coefficient (α) and SEE coefficient (γ) were performed in high-ohmie InP. GaAs. and Si semiconductor cathodes with argon and air environments in a wide range of E/N (300-10 000 Td). The direct calculations of γ were carried out to determine the behavior of cold-semiconductor cathode current in a wide range of microgaps (45 - 525 μm). Paschen curves are interpreted in the dependence of large pd range on breakdown voltage through γ and α/N. Ion-induced secondary electrons exhibit the direct behaviors affecting the timeseale of breakdown evolution in the vicinity of the Paschen minimum during the natural bombardment process with ions of semiconductor cathodes. Also, when α/N rapidly drops and the excitations of gas atoms densely occupy the gas volume, we determined that the photoelectric effect provides a growth for electron emission from semicon-ductor surfaces at the breakdown stage at the reduced values ol E/N. At all pressures, the emission magnitudes of electrons liberated by semiconductor cathodes into vacuum are found as γ_(InP) > γ_(GaAs) > γ_(Si) in breakdown evolution.
机译:本文着重于分析(当有足够的时空分布条件时)半导体表面的二次电子发射(SEE)的分析。采用Townsend系数方法进行的实验测量和计算,包括电离系数(α)和SEE的评估在高E / N(300-10 000 Td)的氩气和空气环境下,在高电阻InP。GaAs。和Si半导体阴极中进行系数(γ)的计算,直接计算γ得出冷半导体阴极电流在大范围(45-525μm)范围内的行为。帕申曲线解释为大dd范围对通过γ和α/ N的击穿电压的依赖性。离子诱导的二次电子表现出直接行为在自然轰击过程中,随着半导体阴极离子的轰击,影响帕申极小值附近击穿演化的时间;此外,当α/ N迅速下降并激发时,大量的气体原子密集地占据了气体体积,我们确定光电效应为击穿阶段的半导体表面上的电子发射提供了增长,且电子发射强度降低了ol E / N。在击穿过程中,在所有压力下,半导体阴极释放到真空中的电子的发射量级为γ_(InP)>γ_(GaAs)>γ_(Si)。

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