Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures

The existence of the two-dimensional electron gas (2DEG) and two-dimensional hole gas (2DHG) in the same III-nitride heterostructure is advantageous for the development of complementary nitride electronics. However, it is still unclear whether the buried-2DHG and the top 2DEG can coexist in the same...

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Main Authors: Lingaparthi, R., Dharmarasu, Nethaji, Radhakrishnan, K.
Other Authors: School of Electrical and Electronic Engineering
Format: Article
Language:English
Published: 2023
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Online Access:https://hdl.handle.net/10356/169147
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Institution: Nanyang Technological University
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spelling sg-ntu-dr.10356-1691472023-07-06T15:31:54Z Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures Lingaparthi, R. Dharmarasu, Nethaji Radhakrishnan, K. School of Electrical and Electronic Engineering Temasek Laboratories @ NTU Center for Micro/Nano-electronics (CMNE) UMI3288 CINTRA, (CNRS/NTU/THALES) Engineering::Electrical and electronic engineering Acceptor State Distribution Models The existence of the two-dimensional electron gas (2DEG) and two-dimensional hole gas (2DHG) in the same III-nitride heterostructure is advantageous for the development of complementary nitride electronics. However, it is still unclear whether the buried-2DHG and the top 2DEG can coexist in the same III-nitride heterostructure. This study has addressed this long-standing question. Using charge distribution model, a systematic analysis is done and proposed surface acceptor states as the origin of the two-dimensional hole gas (2DHG). Using this centralized analysis, factors affecting the formation of both surface and buried-2DHG in the nitride heterostructures are presented. Furthermore, it is proved that the buried-2DHG is absent in III-nitride heterostructures, particularly under the 2DEG. In the absence of buried-2DHG at the GaN/AlXGa1-XN interface, a hole trap is observed, which not only balances the charge distribution but also reduces the electric field in the GaN channel layer. Published version 2023-07-03T08:32:19Z 2023-07-03T08:32:19Z 2023 Journal Article Lingaparthi, R., Dharmarasu, N. & Radhakrishnan, K. (2023). Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures. Applied Physics Letters, 122(17), 172103-1-172103-5. https://dx.doi.org/10.1063/5.0149550 0003-6951 https://hdl.handle.net/10356/169147 10.1063/5.0149550 2-s2.0-85158112069 17 122 172103-1 172103-5 en Applied Physics Letters © 2023 Author(s). Published under an exclusive license by AIP Publishing. All rights reserved. This article may be downloaded for personal use only. Any other use requires prior permission of the author(s) and AIP Publishing. This article appeared in Lingaparthi, R., Dharmarasu, N. & Radhakrishnan, K. (2023). Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures. Applied Physics Letters, 122(17), 172103-1 - 172103-5 and may be found at https://doi.org/10.1063/5.0149550 application/pdf
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
topic Engineering::Electrical and electronic engineering
Acceptor State
Distribution Models
spellingShingle Engineering::Electrical and electronic engineering
Acceptor State
Distribution Models
Lingaparthi, R.
Dharmarasu, Nethaji
Radhakrishnan, K.
Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures
description The existence of the two-dimensional electron gas (2DEG) and two-dimensional hole gas (2DHG) in the same III-nitride heterostructure is advantageous for the development of complementary nitride electronics. However, it is still unclear whether the buried-2DHG and the top 2DEG can coexist in the same III-nitride heterostructure. This study has addressed this long-standing question. Using charge distribution model, a systematic analysis is done and proposed surface acceptor states as the origin of the two-dimensional hole gas (2DHG). Using this centralized analysis, factors affecting the formation of both surface and buried-2DHG in the nitride heterostructures are presented. Furthermore, it is proved that the buried-2DHG is absent in III-nitride heterostructures, particularly under the 2DEG. In the absence of buried-2DHG at the GaN/AlXGa1-XN interface, a hole trap is observed, which not only balances the charge distribution but also reduces the electric field in the GaN channel layer.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Lingaparthi, R.
Dharmarasu, Nethaji
Radhakrishnan, K.
format Article
author Lingaparthi, R.
Dharmarasu, Nethaji
Radhakrishnan, K.
author_sort Lingaparthi, R.
title Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures
title_short Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures
title_full Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures
title_fullStr Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures
title_full_unstemmed Origin of the two-dimensional hole gas and criteria for its existence in the III-nitride heterostructures
title_sort origin of the two-dimensional hole gas and criteria for its existence in the iii-nitride heterostructures
publishDate 2023
url https://hdl.handle.net/10356/169147
_version_ 1772826803221561344