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Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si

Xingzhao Ma, Libin Tang Orcid Logo, Menghan Jia, Yuping Zhang, Wenbin Zuo, Yuhua Cai, Rui Li, Liqing Yang, Vincent Teng Orcid Logo

Advanced Electronic Materials, Volume: 10, Issue: 9

Swansea University Author: Vincent Teng Orcid Logo

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DOI (Published version): 10.1002/aelm.202300909

Abstract

Ultraviolet (UV) photodetectors have gained much attention due to their numerous important applications ranging from environmental monitoring to space communication. To date, most p-NiO/n-Si heterojunction photodetectors (HPDs) exhibit poor UV responsivity and slow response. This is mainly due to a...

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Published in: Advanced Electronic Materials
ISSN: 2199-160X 2199-160X
Published: Wiley 2024
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URI: https://cronfa.swan.ac.uk/Record/cronfa68357
first_indexed 2024-11-27T19:46:36Z
last_indexed 2025-01-13T20:34:22Z
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spelling 2025-01-13T14:38:30.8872974 v2 68357 2024-11-27 Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si 98f529f56798da1ba3e6e93d2817c114 0000-0003-4325-8573 Vincent Teng Vincent Teng true false 2024-11-27 ACEM Ultraviolet (UV) photodetectors have gained much attention due to their numerous important applications ranging from environmental monitoring to space communication. To date, most p-NiO/n-Si heterojunction photodetectors (HPDs) exhibit poor UV responsivity and slow response. This is mainly due to a small valence band offset (ΔEV) at the NiO/Si interface and a high density of dangling bonds at the silicon surface. Herein, an UV HPD consisting of NiO/Al2O3/n-Si is fabricated using magnetron sputtering technique. The HPD has a large rectification ratio of 2.4 × 105. It also exhibits excellent UV responsivity (R) of 15.8 A/W at −5 V and and detectivity (D*) of 1.14 × 1013 Jones at −4 V, respectively. The excellent performance of the HPD can be attributed to the defect passivation at the interfaces of the heterojunction and the efficient separation of photogenerated carriers by the Al2O3 nanolayer. The external quantum efficiency (EQE) of the HPD as high as 5.4 × 103%, hence implying a large optical gain due to carrier proliferation resulting from impact ionization. Furthermore, the ultrafast response speed with a rise time of 80 µs and a decay time of 184 µs are obtained. Journal Article Advanced Electronic Materials 10 9 Wiley 2199-160X 2199-160X Al2O3; heterojunction; NiO; UV photodetector 1 9 2024 2024-09-01 10.1002/aelm.202300909 COLLEGE NANME Aerospace, Civil, Electrical, and Mechanical Engineering COLLEGE CODE ACEM Swansea University Another institution paid the OA fee National Key Research and Development Program of China. Grant Number: 2019YFB2203404 Yunnan Province Innovation Team Project. Grant Number: 2018HC020 2025-01-13T14:38:30.8872974 2024-11-27T13:56:37.5105358 Faculty of Science and Engineering School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Electronic and Electrical Engineering Xingzhao Ma 1 Libin Tang 0000-0002-7174-2963 2 Menghan Jia 3 Yuping Zhang 4 Wenbin Zuo 5 Yuhua Cai 6 Rui Li 7 Liqing Yang 8 Vincent Teng 0000-0003-4325-8573 9
title Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
spellingShingle Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
Vincent Teng
title_short Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
title_full Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
title_fullStr Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
title_full_unstemmed Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
title_sort Ultrahigh Performance UV Photodetector by Inserting an Al<sub>2</sub>O<sub>3</sub> Nanolayer in NiO/n‐Si
author_id_str_mv 98f529f56798da1ba3e6e93d2817c114
author_id_fullname_str_mv 98f529f56798da1ba3e6e93d2817c114_***_Vincent Teng
author Vincent Teng
author2 Xingzhao Ma
Libin Tang
Menghan Jia
Yuping Zhang
Wenbin Zuo
Yuhua Cai
Rui Li
Liqing Yang
Vincent Teng
format Journal article
container_title Advanced Electronic Materials
container_volume 10
container_issue 9
publishDate 2024
institution Swansea University
issn 2199-160X
2199-160X
doi_str_mv 10.1002/aelm.202300909
publisher Wiley
college_str Faculty of Science and Engineering
hierarchytype
hierarchy_top_id facultyofscienceandengineering
hierarchy_top_title Faculty of Science and Engineering
hierarchy_parent_id facultyofscienceandengineering
hierarchy_parent_title Faculty of Science and Engineering
department_str School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Electronic and Electrical Engineering{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Electronic and Electrical Engineering
document_store_str 0
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description Ultraviolet (UV) photodetectors have gained much attention due to their numerous important applications ranging from environmental monitoring to space communication. To date, most p-NiO/n-Si heterojunction photodetectors (HPDs) exhibit poor UV responsivity and slow response. This is mainly due to a small valence band offset (ΔEV) at the NiO/Si interface and a high density of dangling bonds at the silicon surface. Herein, an UV HPD consisting of NiO/Al2O3/n-Si is fabricated using magnetron sputtering technique. The HPD has a large rectification ratio of 2.4 × 105. It also exhibits excellent UV responsivity (R) of 15.8 A/W at −5 V and and detectivity (D*) of 1.14 × 1013 Jones at −4 V, respectively. The excellent performance of the HPD can be attributed to the defect passivation at the interfaces of the heterojunction and the efficient separation of photogenerated carriers by the Al2O3 nanolayer. The external quantum efficiency (EQE) of the HPD as high as 5.4 × 103%, hence implying a large optical gain due to carrier proliferation resulting from impact ionization. Furthermore, the ultrafast response speed with a rise time of 80 µs and a decay time of 184 µs are obtained.
published_date 2024-09-01T14:38:40Z
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score 11.048042