多层平面纳米结构SSE阴极

V. Semet, V. Binh, J.P. Zhang, J. Yang, M.A. Khan, R. Tsu
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引用次数: 0

摘要

研究了多层平面纳米结构固体场控发射(SSE)。SSE是通过监测表面超薄层的空间电荷值来控制电子发射的有效表面势垒,或者通过改变下表层的电子性质来降低有效表面势垒。在SiC衬底上沉积了一层厚度为0.15 /spl mu/m的掺硅AlGaN层,al含量为40% ~ 15%。它起到导电缓冲层的作用。利用原子力显微镜对加工后的表面进行了原子光滑的表征。使用扫描阳极场发射显微镜(SAFEM)进行I-V测量。发现存在两种机制,第一种是通过降低功函数来隧穿场发射。给定电流密度J/sub FN/,电子通过场发射机制从GaN量子阱内部的量子化子带发射。第二种机制发生在温度升高时,即k/sub B/T > 0.8 eV,此时热电子可以跳过位于导电衬底和Al/sub 0.5/Ga/sub 0.5/N超薄层之间的第一个势垒。由于表面的第二势垒较低(由于空间电荷小于0.5 eV),这些电子将直接发射。这第一个势垒控制发射电流J/sub TH/随温度的变化。在这个双势垒模型中,测量的总发射电流J/sub mes/将是两个贡献的总和,J/sub mes/ = J/sub FN/ + J/sub TH/。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Multilayer planar nanostructured SSE cathodes
Multilayer planar nanostructured solid-state field-controlled emission (SSE) are studied. SSE is an approach to control the effective surface barrier for electron emission by monitoring the space charge value of an ultra-thin layer at the surface, or in other terms to lower the effective surface barrier by modifying the electronic properties of the underneath surface layer. A 0.15 /spl mu/m-thick Si-doped AlGaN layer with Al-content graded from 40% to 15% was deposited on a SiC substrate. It served as the conducting buffer layer. The finished surface was characterized to be atomically smooth by atomic force microscope. The I-V measurements were performed with a scanning anode field emission microscope (SAFEM). Two mechanisms were found to be present, first is tunneling field emission through a lowering work function. The electrons are emitted by a field emission mechanism from the quantized sub-bands inside the GaN quantum well, given a current density J/sub FN/. The second mechanism occurs for elevated temperatures, i.e. k/sub B/T > 0.8 eV, when hot electrons can jump over the first barrier located between the conductive substrate and the Al/sub 0.5/Ga/sub 0.5/N ultra-thin layer. As the second barrier at the surface is lower (less than 0.5 eV due to space charge) these electrons will emit directly. This first barrier controls the variation of the emitted current J/sub TH/ with temperature. In this dual-barrier model, the measured total emission current, J/sub mes/, will be the sum of both contributions, J/sub mes/ = J/sub FN/ + J/sub TH/.
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