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In-situ determination of the flat band carrier concentration and surface charge density of individual semiconductor nanowires by a combination of electrical and field emission measurements

机译:结合电和场发射测量原位确定单个半导体纳米线的平带载流子浓度和表面电荷密度

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摘要

The carrier concentration of semiconductor nanowires is one of the most important parameters for their nanoelectronic and optoelectronic applications. Because of their nanoscale geometry, the carrier concentration of nanowires is related to their flat band carrier concentration and surface charge density. Usually, these fundamental properties can be derived from the electrical transport and capacitance measurements of a nanowire field effect transistor (FET). Considering that the FET fabrication process can easily affect the nanowire surface, in-situ determination of these properties is of great interest. In this work, a method based on the chemical adsorption-induced surface band bending and field emission penetration effect was proposed to fulfill this task. Using this technique, the flat band earner concentration and the surface charge density of a free-standing ZnO nanowire were obtained to be 0.7-2 x 10~(18)cm~(-3) and 1.07-3.73 x 10~(12)e/cm~2, respectively. Compared with the conventional method based on a nanowire FET, this result provides a simple and nondestructive way to study these fundamental electrical properties of a nanowire.
机译:半导体纳米线的载流子浓度是其纳米电子和光电应用的最重要参数之一。由于纳米线的几何形状,纳米线的载流子浓度与其平带载流子浓度和表面电荷密度有关。通常,这些基本属性可以从纳米线场效应晶体管(FET)的电传输和电容测量得出。考虑到FET的制造过程很容易影响纳米线表面,因此就地确定这些特性引起了极大的兴趣。在这项工作中,提出了一种基于化学吸附引起的表面带弯曲和场发射穿透效应的方法来完成此任务。使用该技术,获得的自支撑ZnO纳米线的平带载流子浓度和表面电荷密度分别为0.7-2 x 10〜(18)cm〜(-3)和1.07-3.73 x 10〜(12) e / cm〜2。与基于纳米线FET的常规方法相比,该结果提供了一种简单而无损的方法来研究纳米线的这些基本电学特性。

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  • 来源
    《Journal of Applied Physics》 |2017年第17期|174306.1-174306.6|共6页
  • 作者单位

    State Key Laboratory of Optoelectronic Materials and Technologies, Guangdong Province Key LaboraToiy of Display Material and Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China, School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275. People's Republic of China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Guangdong Province Key LaboraToiy of Display Material and Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China, School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275. People's Republic of China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Guangdong Province Key LaboraToiy of Display Material and Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China, School of Physics, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Guangdong Province Key LaboraToiy of Display Material and Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China, School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275. People's Republic of China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Guangdong Province Key LaboraToiy of Display Material and Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China, School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275. People's Republic of China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Guangdong Province Key LaboraToiy of Display Material and Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275, People's Republic of China, School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275. People's Republic of China;

    School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou, Guangdong 510275. People's Republic of China;

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  • 正文语种 eng
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