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High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector
The InAs/GaSb superlattice infrared detector has been developed with tremendous effort. However, the performance of it, especially long-wavelength infrared detectors (LWIR), is still limited by the electrical performance and optical quantum efficiency (QE). Forcing the active region to be p-type thr...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Springer US
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8164656/ https://www.ncbi.nlm.nih.gov/pubmed/34052936 http://dx.doi.org/10.1186/s11671-021-03550-x |
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author | Sun, Ju Li, Nong Jia, Qing-Xuan Zhang, Xuan Jiang, Dong-Wei Wang, Guo-Wei Niu, Zhi-Chuan |
author_facet | Sun, Ju Li, Nong Jia, Qing-Xuan Zhang, Xuan Jiang, Dong-Wei Wang, Guo-Wei Niu, Zhi-Chuan |
author_sort | Sun, Ju |
collection | PubMed |
description | The InAs/GaSb superlattice infrared detector has been developed with tremendous effort. However, the performance of it, especially long-wavelength infrared detectors (LWIR), is still limited by the electrical performance and optical quantum efficiency (QE). Forcing the active region to be p-type through proper doping can highly improve QE, and the gating technique can be employed to greatly enhance electrical performance. However, the saturation bias voltage is too high. Reducing the saturation bias voltage has broad prospects for the future application of gate voltage control devices. In this paper, we report that the gated P(+)–π–M–N(+) InAs/GaSb superlattice long-wavelength infrared detectors exhibit different π region doping levels that have a reduced minimum saturation bias at − 10 V with a 200-nm SiO(2) layer after a simple and effective anodic vulcanization pretreatment. The saturation gate bias voltage is much lower than − 40 V that reported with the same thickness of a 200-nm SiO(2) passivation layer and similar structure. The optical and electrical characterization indicates that the electrical and optical performance of the device would be weakened by excessive doping concentration. At 77 K, the 50% cutoff wavelength of the device is about 8 µm, the 100% cutoff wavelength is 10 µm, the maximum quantum efficiency is 62.4%, the maximum of responsivity is 2.26 A/W at 5 µm, and the maximum RA of the device is 1259.4 Ω cm(2). Besides, the specific detectivity of Be 780 °C-doped detector without gate electrode exhibits a peak of 5.6 × 10(10) cm Hz(1/2)/W at 5 µm with a 70-mv reverse bias voltage, which is more than three times that of Be 820 °C-doped detector. Moreover, the peak specific detectivity could be further increased to 1.3 × 10(11) cm Hz(1/2)/W at 5 µm with a 10-mv reserve bias voltage that has the bias of − 10 V at the gate electrode. |
format | Online Article Text |
id | pubmed-8164656 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | Springer US |
record_format | MEDLINE/PubMed |
spelling | pubmed-81646562021-06-17 High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector Sun, Ju Li, Nong Jia, Qing-Xuan Zhang, Xuan Jiang, Dong-Wei Wang, Guo-Wei Niu, Zhi-Chuan Nanoscale Res Lett Nano Express The InAs/GaSb superlattice infrared detector has been developed with tremendous effort. However, the performance of it, especially long-wavelength infrared detectors (LWIR), is still limited by the electrical performance and optical quantum efficiency (QE). Forcing the active region to be p-type through proper doping can highly improve QE, and the gating technique can be employed to greatly enhance electrical performance. However, the saturation bias voltage is too high. Reducing the saturation bias voltage has broad prospects for the future application of gate voltage control devices. In this paper, we report that the gated P(+)–π–M–N(+) InAs/GaSb superlattice long-wavelength infrared detectors exhibit different π region doping levels that have a reduced minimum saturation bias at − 10 V with a 200-nm SiO(2) layer after a simple and effective anodic vulcanization pretreatment. The saturation gate bias voltage is much lower than − 40 V that reported with the same thickness of a 200-nm SiO(2) passivation layer and similar structure. The optical and electrical characterization indicates that the electrical and optical performance of the device would be weakened by excessive doping concentration. At 77 K, the 50% cutoff wavelength of the device is about 8 µm, the 100% cutoff wavelength is 10 µm, the maximum quantum efficiency is 62.4%, the maximum of responsivity is 2.26 A/W at 5 µm, and the maximum RA of the device is 1259.4 Ω cm(2). Besides, the specific detectivity of Be 780 °C-doped detector without gate electrode exhibits a peak of 5.6 × 10(10) cm Hz(1/2)/W at 5 µm with a 70-mv reverse bias voltage, which is more than three times that of Be 820 °C-doped detector. Moreover, the peak specific detectivity could be further increased to 1.3 × 10(11) cm Hz(1/2)/W at 5 µm with a 10-mv reserve bias voltage that has the bias of − 10 V at the gate electrode. Springer US 2021-05-29 /pmc/articles/PMC8164656/ /pubmed/34052936 http://dx.doi.org/10.1186/s11671-021-03550-x Text en © The Author(s) 2021 https://creativecommons.org/licenses/by/4.0/Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Nano Express Sun, Ju Li, Nong Jia, Qing-Xuan Zhang, Xuan Jiang, Dong-Wei Wang, Guo-Wei Niu, Zhi-Chuan High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector |
title | High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector |
title_full | High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector |
title_fullStr | High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector |
title_full_unstemmed | High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector |
title_short | High-Performance Anodic Vulcanization-Pretreated Gated P(+)–π–M–N(+) InAs/GaSb Superlattice Long-Wavelength Infrared Detector |
title_sort | high-performance anodic vulcanization-pretreated gated p(+)–π–m–n(+) inas/gasb superlattice long-wavelength infrared detector |
topic | Nano Express |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8164656/ https://www.ncbi.nlm.nih.gov/pubmed/34052936 http://dx.doi.org/10.1186/s11671-021-03550-x |
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