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基于TiO NPs修饰的三维石墨烯场效应晶体管的高灵敏度紫外探测。

High sensitivity ultraviolet detection based on three-dimensional graphene field effect transistors decorated with TiO NPs.

作者信息

Li Shasha, Yin Weijie, Li Yuning, Sun Jingye, Zhu Mingqiang, Liu Zewen, Deng Tao

机构信息

School of Electronic and Information Engineering, Beijing Jiaotong University, Beijing 100044, China.

出版信息

Nanoscale. 2019 Aug 8;11(31):14912-14920. doi: 10.1039/c9nr04475b.

Abstract

A three-dimensional (3D) ultraviolet (UV) photodetector was fabricated by decorating a tubular graphene field-effect transistor (GFET) with titanium dioxide (TiO2) nanoparticles (NPs). The unique tubular architecture not only provides a natural 3D optical resonant microcavity to enhance the optical field inside it, but also increases the light-matter interaction area. Strong UV absorption in the TiO2 NPs creates a number of electron-hole pairs, where the electrons are transferred to graphene, while the holes are trapped within the TiO2 NPs, leading to a strong photogating effect on the graphene channel conductance. The photoresponsivity of our 3D GFET photodetector decorated with TiO2 NPs was demonstrated up to 475.5 A W-1 at 325 nm, which is about 2 orders of magnitude higher than that of a 3D GFET photodetector without the TiO2 NP decoration (1 A W-1), and over 3 orders of magnitude higher than that of a recently reported UV photodetector based on the graphene/vertical Ga2O3 nanowire array heterojunction (0.185 A W-1). Moreover, the photoresponsivity and photoresponse speed of the device can be easily tuned by applying a small gate bias (≤3 V) and/or changing the source-drain bias. These results indicate that the photoresponsivities of graphene-based photodetectors can be significantly improved by exploiting 3D graphene structures and integrating graphene with semiconducting light harvesters simultaneously.

摘要

通过用二氧化钛(TiO₂)纳米颗粒(NPs)修饰管状石墨烯场效应晶体管(GFET)制备了一种三维(3D)紫外(UV)光电探测器。独特的管状结构不仅提供了一个天然的3D光学谐振微腔来增强其内部的光场,还增加了光与物质的相互作用面积。TiO₂ NPs中的强紫外吸收产生了大量的电子 - 空穴对,其中电子转移到石墨烯上,而空穴被困在TiO₂ NPs内,从而对石墨烯沟道电导产生强烈的光门控效应。我们用TiO₂ NPs修饰的3D GFET光电探测器在325 nm处的光响应度高达475.5 A W⁻¹,这比没有TiO₂ NP修饰的3D GFET光电探测器(1 A W⁻¹)高约2个数量级,比最近报道的基于石墨烯/垂直Ga₂O₃纳米线阵列异质结的紫外光电探测器(0.185 A W⁻¹)高超过3个数量级。此外,通过施加小的栅极偏置(≤3 V)和/或改变源漏偏置,可以轻松调节器件的光响应度和光响应速度。这些结果表明,通过利用3D石墨烯结构并同时将石墨烯与半导体光收集器集成,可以显著提高基于石墨烯的光电探测器的光响应度。

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