A Vacuum Insulator Negative Electron Affinity Electron Emitter with High Quantum Efficiency

J. S. Vazquez, A. T. Priyoti, Ragib Ahsan, Hyun Uk Chae, R. Kapadia
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Abstract

Previous studies of planar graphene-oxide-semiconductor (GOS) structures have highlighted Fowler-Nordheim (FN) tunneling through the oxide layer as the dominant mechanism for electron emission[1]. Scattering within the oxide layer limits electron emission but can be counteracted by generating hot-electrons through optical excitation in the underlying semiconductor[2]. Still, the scattering in the oxide persists, limiting the current emission efficiency. Additionally, trapping of electrons causes broadening of the emitted electron energy spectrum. A novel graphene-vacuum-semiconductor (GVS) structure is developed. By eliminating the oxide layer, the tunneling mechanisms can be reduced to Fowler-Nordheim exclusively. As a result, emitted electrons will have an energy spread limited by that of the semiconductor and scattering in the graphene[2]. Additionally, electron trapping in the oxide is eliminated. Field-emission is also increased as the electric field increased by controllably reducing the height of the vacuum gap. Here we will explore the fabrication of vacuum hot electron light assisted cathodes (VHELACs).
一种高量子效率的真空绝缘体负电子亲和电子发射器
先前对平面石墨烯-氧化半导体(GOS)结构的研究强调,通过氧化层的Fowler-Nordheim (FN)隧穿是电子发射的主要机制[1]。氧化物层内的散射限制了电子发射,但可以通过在底层半导体中通过光激发产生热电子来抵消[2]。然而,氧化物中的散射仍然存在,限制了当前的发射效率。此外,电子的俘获引起发射电子能谱的展宽。提出了一种新型石墨烯-真空半导体(GVS)结构。通过消除氧化层,隧道机制可以简化为Fowler-Nordheim专属。因此,发射的电子的能量扩散将受到石墨烯中半导体和散射的限制[2]。此外,消除了氧化物中的电子捕获。通过可控地降低真空间隙的高度,电场的增加也增加了场发射。本文将探讨真空热电子光辅助阴极(VHELACs)的制备方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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