Straddling Tunneling FETs and Broadband Photodetectors Based on HfS2/SnS2 van der Waals Heterostructure

异质结 材料科学 光电探测器 光电子学 量子隧道 半导体 光电导性 光电效应 偏压 紫外线 电介质 晶体管 范德瓦尔斯力 响应度 隧道效应 共发射极 光敏性 比探测率 场效应晶体管
作者
Xiangna Cong,Muhammad Najeeb Ullah Shah,Yuxiang Huang,Chengcai Wang,Wenlong He
出处
期刊:ACS Applied Materials & Interfaces [American Chemical Society]
卷期号:17 (38): 53951-53959 被引量:1
标识
DOI:10.1021/acsami.5c13429
摘要

Past studies have shown that vdWHs possess considerable potential for photodetector applications. However, the current performance of 2D material photodetectors falls short of practical demands due to pronounced interfacial recombination, insufficient photoconductive gain, and inefficient photocarrier collection. Straddling (type I) 2D vdWH notably diminishes interfacial trapping, amplifies the photoconductive gain, and facilitates anisotropic photocarrier collection. Tunnel FET (TFET), fabricated from these type I 2D materials, provides enhanced electrostatic control and the capability for substantially higher on-current densities and on/off ratios. However, gaining an understanding of the intricate tunneling mechanisms within type I heterostructures continues to present a significant challenge. In this study, we demonstrate gate-tunable type I tunnel heterostructures utilizing a HfS 2 /SnS 2 vdWHs. By employing a single electrostatic gating mechanism with hexagonal boron nitride (h-BN) as the dielectric layer, a variety of electrical transport behaviors, such as forward rectification, Esaki tunneling, and backward rectification, are realized within the same heterostructure at low gate voltage levels of ±3 V. The heterostructure demonstrates distinct room-temperature negative differential resistance (NDR) characteristics, evident at a low bias voltage of ±0.4 V. In darkness, direct tunneling (DT) is the dominant transport mechanism. However, under illumination, the heterostructure exhibits a shift to the Fowler–Nordheim tunneling (FNT) behavior. The type I heterostructures achieved a photoresponsivity ( R ) of 43 A W –1 under 455 nm illumination. Furthermore, the device shows an exceptional detectivity ( D *) of 4.3 × 10 11 Jones and broadband detection capabilities, covering the spectra from ultraviolet to visible light. Our work broadens the range of capabilities for 2D semiconductor devices, highlighting a compelling potential for their utilization in future optoelectronic systems.
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