Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor
Abstract Gate-controlled amplifiable ultraviolet phototransistors have been demonstrated using AlGaN/GaN high-electron-mobility transistors (HEMTs) with very thin AlGaN barriers. In the AlGaN/GaN HEMTs, the dark current between the source and drain increases with increasing thickness of the AlGaN ba...
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doaj-780a418e1f8c4a059ec1398e8e7efe682021-04-04T11:33:36ZengNature Publishing GroupScientific Reports2045-23222021-03-011111910.1038/s41598-021-86575-7Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistorSeung-Hye Baek0Gun-Woo Lee1Chu-Young Cho2Sung-Nam Lee3Department of Nano and Semiconductor Engineering, Korea Polytechnic UniversityDepartment of Nano and Semiconductor Engineering, Korea Polytechnic UniversityNanodevices Lab., Korea Advanced Nano Fab CenterDepartment of Nano and Semiconductor Engineering, Korea Polytechnic UniversityAbstract Gate-controlled amplifiable ultraviolet phototransistors have been demonstrated using AlGaN/GaN high-electron-mobility transistors (HEMTs) with very thin AlGaN barriers. In the AlGaN/GaN HEMTs, the dark current between the source and drain increases with increasing thickness of the AlGaN barrier from 10 to 30 nm owing to the increase in piezoelectric polarization-induced two-dimensional electron gas (2-DEG). However, the photocurrent of the AlGaN/GaN HEMT decreases with increasing thickness of the AlGaN barrier under ultraviolet exposure conditions. It can be observed that a thicker AlGaN barrier exhibits a much higher 2-DEG than the photogenerated carriers at the interface between AlGaN and GaN. In addition, regardless of the AlGaN barrier thickness, the source–drain dark current increases as the gate bias increases from − 1.0 to + 1.0 V. However, the photocurrent of the phototransistor with the 30 nm thick AlGaN barrier was not affected by the gate bias, whereas that of the phototransistor with 10 nm thick AlGaN barrier was amplified from reduction of the gate bias. From these results, we suggest that by controlling the gate bias, a thin AlGaN barrier can amplify/attenuate the photocurrent of the AlGaN/GaN HEMT-based phototransistor.https://doi.org/10.1038/s41598-021-86575-7 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Seung-Hye Baek Gun-Woo Lee Chu-Young Cho Sung-Nam Lee |
spellingShingle |
Seung-Hye Baek Gun-Woo Lee Chu-Young Cho Sung-Nam Lee Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor Scientific Reports |
author_facet |
Seung-Hye Baek Gun-Woo Lee Chu-Young Cho Sung-Nam Lee |
author_sort |
Seung-Hye Baek |
title |
Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor |
title_short |
Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor |
title_full |
Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor |
title_fullStr |
Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor |
title_full_unstemmed |
Gate-controlled amplifiable ultraviolet AlGaN/GaN high-electron-mobility phototransistor |
title_sort |
gate-controlled amplifiable ultraviolet algan/gan high-electron-mobility phototransistor |
publisher |
Nature Publishing Group |
series |
Scientific Reports |
issn |
2045-2322 |
publishDate |
2021-03-01 |
description |
Abstract Gate-controlled amplifiable ultraviolet phototransistors have been demonstrated using AlGaN/GaN high-electron-mobility transistors (HEMTs) with very thin AlGaN barriers. In the AlGaN/GaN HEMTs, the dark current between the source and drain increases with increasing thickness of the AlGaN barrier from 10 to 30 nm owing to the increase in piezoelectric polarization-induced two-dimensional electron gas (2-DEG). However, the photocurrent of the AlGaN/GaN HEMT decreases with increasing thickness of the AlGaN barrier under ultraviolet exposure conditions. It can be observed that a thicker AlGaN barrier exhibits a much higher 2-DEG than the photogenerated carriers at the interface between AlGaN and GaN. In addition, regardless of the AlGaN barrier thickness, the source–drain dark current increases as the gate bias increases from − 1.0 to + 1.0 V. However, the photocurrent of the phototransistor with the 30 nm thick AlGaN barrier was not affected by the gate bias, whereas that of the phototransistor with 10 nm thick AlGaN barrier was amplified from reduction of the gate bias. From these results, we suggest that by controlling the gate bias, a thin AlGaN barrier can amplify/attenuate the photocurrent of the AlGaN/GaN HEMT-based phototransistor. |
url |
https://doi.org/10.1038/s41598-021-86575-7 |
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