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铝掺杂α-GaO纳米棒阵列的水热生长及其在基于光电化学电池的自供电日盲紫外光探测中的应用。

Hydrothermal Growth of an Al-Doped α-GaO Nanorod Array and Its Application in Self-Powered Solar-Blind UV Photodetection Based on a Photoelectrochemical Cell.

作者信息

Guo Jing-Chun, Sun Guang-Wu, Fan Ming-Ming, Fu Xu-Cheng, Yao Jia-Jia, Wang Yu-Dong

机构信息

Department of Experimental and Practical Teaching Management, West Anhui University, Lu'an 237012, China.

Mechanical and Electrical Engineering College, Hainan Vocational University of Science and Technology, Haikou 571126, China.

出版信息

Micromachines (Basel). 2023 Jun 29;14(7):1336. doi: 10.3390/mi14071336.

DOI:10.3390/mi14071336
PMID:37512647
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10384112/
Abstract

Herein, we successfully fabricated an Al-doped α-GaO nanorod array on FTO using the hydrothermal and post-annealing processes. To the best of our knowledge, it is the first time that an Al-doped α-GaO nanorod array on FTO has been realized via a much simpler and cheaper way than that based on metal-organic chemical vapor deposition, magnetron sputtering, molecular beam epitaxy, and pulsed laser deposition. And, a self-powered Al-doped α-GaO nanorod array/FTO photodetector was also realized as a photoanode at 0 V (vs. Ag/AgCl) in a photoelectrochemical (PEC) cell, showing a peak responsivity of 1.46 mA/W at 260 nm. The response speed of the Al-doped device was 0.421 s for rise time, and 0.139 s for decay time under solar-blind UV (260 nm) illumination. Compared with the undoped device, the responsivity of the Al-doped device was ~5.84 times larger, and the response speed was relatively faster. When increasing the biases from 0 V to 1 V, the responsivity, quantum efficiency, and detectivity of the Al-doped device were enhanced from 1.46 mA/W to 2.02 mA/W, from ~0.7% to ~0.96%, and from ~6 × 10 Jones to ~1 × 10 Jones, respectively, due to the enlarged depletion region. Therefore, Al doping may provide a route to enhance the self-powered photodetection performance of α-GaO nanorod arrays.

摘要

在此,我们通过水热法和退火后处理工艺成功地在FTO上制备了Al掺杂的α-GaO纳米棒阵列。据我们所知,这是首次通过比基于金属有机化学气相沉积、磁控溅射、分子束外延和脉冲激光沉积的方法更简单、更便宜的方式在FTO上实现Al掺杂的α-GaO纳米棒阵列。并且,还制备了一种自供电的Al掺杂α-GaO纳米棒阵列/FTO光电探测器,该探测器在光电化学(PEC)电池中作为光阳极,在0 V(相对于Ag/AgCl)时,在260 nm处显示出1.46 mA/W的峰值响应率。在日盲紫外(260 nm)光照下,Al掺杂器件的上升时间响应速度为0.421 s,下降时间为0.139 s。与未掺杂器件相比,Al掺杂器件的响应率大约大5.84倍,且响应速度相对更快。当偏压从0 V增加到1 V时,由于耗尽区扩大,Al掺杂器件的响应率、量子效率和探测率分别从1.46 mA/W提高到2.02 mA/W,从约0.7%提高到约0.96%,从约6×10琼斯提高到约1×10琼斯。因此,Al掺杂可能为提高α-GaO纳米棒阵列的自供电光探测性能提供一条途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/b78aae95aa2e/micromachines-14-01336-g005a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/bcabaa5a09b0/micromachines-14-01336-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/771e7ac2a1da/micromachines-14-01336-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/94c52ff1f691/micromachines-14-01336-g003a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/df38f6318561/micromachines-14-01336-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/b78aae95aa2e/micromachines-14-01336-g005a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/bcabaa5a09b0/micromachines-14-01336-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/771e7ac2a1da/micromachines-14-01336-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/94c52ff1f691/micromachines-14-01336-g003a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/df38f6318561/micromachines-14-01336-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/802f/10384112/b78aae95aa2e/micromachines-14-01336-g005a.jpg

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本文引用的文献

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Pt/(InGa)O/-Si Heterojunction-Based Solar-Blind Ultraviolet Photovoltaic Detectors with an Ideal Absorption Cutoff Edge of 280 nm.基于Pt/(InGa)O/-Si异质结的日盲紫外光伏探测器,其理想吸收截止边缘为280纳米。
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