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基于指数型关联光电转换定律的记忆型光电晶体管。

Memory phototransistors based on exponential-association photoelectric conversion law.

机构信息

Institute of Functional Nano & Soft Materials (FUNSOM), Jiangsu Key Laboratory for Carbon-Based Functional Materials & Devices, Soochow University, Suzhou, Jiangsu, 215123, P. R. China.

School of Chemical and Environmental Engineering, Jiangsu University of Technology, Changzhou, Jiangsu, 213001, P. R. China.

出版信息

Nat Commun. 2019 Mar 20;10(1):1294. doi: 10.1038/s41467-019-09206-w.

DOI:10.1038/s41467-019-09206-w
PMID:30894530
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6426936/
Abstract

Ultraweak light detectors have wide-ranging important applications such as astronomical observation, remote sensing, laser ranging, and night vision. Current commercial ultraweak light detectors are commonly based on a photomultiplier tube or an avalanche photodiode, and they are incompatible with microelectronic devices for digital imaging applications, because of their high operating voltage and bulky size. Herein, we develop a memory phototransistor for ultraweak light detection, by exploiting the charge-storage accumulative effect in CdS nanoribbon. The memory phototransistors break the power law of traditional photodetectors and follow a time-dependent exponential-association photoelectric conversion law. Significantly, the memory phototransistors exhibit ultrahigh responsivity of 3.8 × 10 A W and detectivity of 7.7 × 10 Jones. As a result, the memory phototransistors are able to detect ultraweak light of 6 nW cm with an extremely high sensitivity of 4 × 10. The proposed memory phototransistors offer a design concept for ultraweak light sensing devices.

摘要

超弱光探测器在天文观测、遥感、激光测距、夜视等领域有着广泛的重要应用。目前的商用超弱光探测器通常基于光电倍增管或雪崩光电二极管,由于其工作电压高、体积庞大,与微电子数字成像应用的器件不兼容。在此,我们通过利用 CdS 纳米带的电荷存储累积效应,开发了一种用于超弱光检测的记忆型光电晶体管。该记忆型光电晶体管打破了传统光电探测器的幂律关系,遵循时间相关的指数关联光电转换定律。值得注意的是,记忆型光电晶体管表现出超高的响应率 3.8×10^A W 和探测率 7.7×10^12 Jones。因此,该记忆型光电晶体管能够以极高的灵敏度 4×10^12 检测低至 6 nW cm 的超弱光。所提出的记忆型光电晶体管为超弱光传感设备提供了一种设计理念。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/c9edcdfe0d65/41467_2019_9206_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/3ecf279d3547/41467_2019_9206_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/b2df7e421c85/41467_2019_9206_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/7f4c50f7e780/41467_2019_9206_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/4f7f0b744dc4/41467_2019_9206_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/c9edcdfe0d65/41467_2019_9206_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/3ecf279d3547/41467_2019_9206_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/b2df7e421c85/41467_2019_9206_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/7f4c50f7e780/41467_2019_9206_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/4f7f0b744dc4/41467_2019_9206_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/77d9/6426936/c9edcdfe0d65/41467_2019_9206_Fig5_HTML.jpg

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