Excellent Optoelectronic Properties and Low Contact Resistance of Graphene/MoS2 Heterostructure Optoelectronic Devices: First-Principles Calculation and Experimental Verification

材料科学 石墨烯 光电子学 肖特基势垒 响应度 异质结 接触电阻 光电流 量子隧道 晶体管 场效应晶体管 纳米技术 光电探测器 电压 二极管 图层(电子) 电气工程 工程类
作者
Panke Li,Huitian Guo,Ran Duan,Guoliang Ru,Weihong Qi
出处
期刊:ACS applied electronic materials [American Chemical Society]
卷期号:5 (3): 1676-1687 被引量:7
标识
DOI:10.1021/acsaelm.2c01726
摘要

Two-dimensional (2D) materials have enormous applications and are widely studied in the field of electronics and optoelectronic devices. The electrical contacts between the 2D materials and the electrodes seriously affect the performance of the 2D material optoelectronic devices. Exploring the electronic structure and transport behavior at the interface between 2D materials and electrodes and the underlying physical causes will contribute to the development of 2D material integrated circuits and optoelectronic fields. In this study, the charge transport barriers at the Au/MoS2 and graphene/MoS2 interfaces were investigated from both the Schottky and tunneling barriers through theoretical calculations, which demonstrated that the graphene/MoS2 interface has not only a very low Schottky barrier but also a low tunneling barrier compared to the Au/MoS2 interface. Then, three types of optoelectronic devices, Au/MoS2/Au, graphene/MoS2/graphene, and graphene/MoS2/Au field-effect transistors (FETs), were fabricated. Compared with the Au/MoS2/Au device, the graphene/MoS2/graphene device shows an excellent optical response (R = 654 mA W–1 at 532 nm laser with a power density of 4.8 mW cm–2) and ultrafast response time (rise time 9.8 ms, 12.8 ms fall time). The graphene/MoS2/Au device exhibits excellent rectification behavior and optoelectronic response, with almost no current and photocurrent gain and cutoff state under reverse bias, excellent optoelectronic response under positive bias (responsivity R = 293.4 mA W–1 at a power density of 4.8 mW cm–2 for a 532 nm wavelength laser), and excellent response time (rise time 12.55 ms, fall time 15.44 ms). Our studies are expected to bring opportunities for highly sensitive, high-speed, and energy-efficient photodetectors for comprehensive applications.
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