Photoelectric Measurements of the Modern Graphene-Insulator-Semiconductor (GIS) Test Structures

K. Piskorski, H. Przewlocki, V. Passi, J. Ruhkopf, M. Lemme
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Abstract

The fundamental property of any semiconductor device is its energy band diagram, which allows prediction of parameters and limitations of the device. The commonly used and most effective methods of band diagram determination are based on photoelectric measurements of specially prepared test structures, most often metal-insulator-semiconductor (MIS) capacitors. Such capacitors must have thin enough metal gates to make them semitransparent to light, which has to penetrate the gate and irradiate the substrate causing photoemission of carriers from both the gate and the substrate into the insulator. This way barrier heights (band offsets) on both sides of the insulator layer can be determined. In this paper we present the advantages of using in the photoelectric measurements the graphene-insulator-semiconductor (GIS) structures in which the metal gate is replaced by a graphene gate. Due to negligible thickness and high transparency of graphene photoelectric measurements allow determination of barrier heights for emission of both electrons and holes from the substrate into the insulator which allows direct determination of the insulator band gap. Using MIS structures it is practically impossible to measure the photocurrent due to hole emission from the substrate since it is overwhelmed by the large photocurrent due to electrons simultaneously emitted from the metal gate.
现代石墨烯-绝缘体-半导体(GIS)测试结构的光电测量
任何半导体器件的基本属性是其能带图,它允许预测器件的参数和限制。常用和最有效的带图测定方法是基于特殊制备的测试结构的光电测量,最常见的是金属-绝缘体-半导体(MIS)电容器。这样的电容器必须有足够薄的金属栅极,使其对光线半透明,光线必须穿透栅极并照射基片,从而使载流子从栅极和基片发射到绝缘体中。这样就可以确定绝缘层两侧的势垒高度(带偏移)。本文介绍了用石墨烯栅极代替金属栅极用于光电测量的石墨烯-绝缘体-半导体(GIS)结构的优点。由于石墨烯的厚度可忽略不计和高透明度,光电测量可以确定电子和空穴从衬底发射到绝缘体的势垒高度,从而可以直接确定绝缘体带隙。使用MIS结构几乎不可能测量基片空穴发射产生的光电流,因为基片被金属栅极同时发射的电子产生的大光电流淹没。
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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