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Characterization of Trapping Effects Related to Carbon Doping Level in AlGaN Back-Barriers for AlGaN/GaN HEMTs

Castillo, Ragnar Ferrand Drake Del ; Chen, Ding Yuan ; Chen, Jr Tai ; Thorsell, Mattias ; Darakchieva, Vanya LU and Rorsman, Niklas (2024) In IEEE Transactions on Electron Devices 71(6). p.3596-3602
Abstract
The impact of different carbon concentrations in the Al 0.06 Ga 0.94 N graded back-barrier and GaN buffer of high electron mobility transistors (HEMTs) is investigated. Four epi-wafers with different carbon concentrations, ranging from 1 × 10 17 to 5 × 10 17 cm −3 , were grown by metal organic chemical vapor deposition (MOCVD). HEMTs with 100 and 200 nm gate lengths were fabricated and characterized with dc, Pulsed-IV, drain current transient spectroscopy (DCTS), and large-signal measurements at 30 GHz. It is shown that the back-barrier effectively prevents buffer-related electron trapping. The highest C-doping provides the best 2DEG confinement, while lower carbon doping levels are beneficial for a high output power and efficiency.... (More)
The impact of different carbon concentrations in the Al 0.06 Ga 0.94 N graded back-barrier and GaN buffer of high electron mobility transistors (HEMTs) is investigated. Four epi-wafers with different carbon concentrations, ranging from 1 × 10 17 to 5 × 10 17 cm −3 , were grown by metal organic chemical vapor deposition (MOCVD). HEMTs with 100 and 200 nm gate lengths were fabricated and characterized with dc, Pulsed-IV, drain current transient spectroscopy (DCTS), and large-signal measurements at 30 GHz. It is shown that the back-barrier effectively prevents buffer-related electron trapping. The highest C-doping provides the best 2DEG confinement, while lower carbon doping levels are beneficial for a high output power and efficiency. A C-doping of 1 × 10 17 cm −3 offers the highest output power at maximum power added efficiency (PAE) (1.8 W/mm), whereas 3 × 10 17 cm −3 doping provides the highest PAE ( > 40%). The C-profiles acquired by using secondary ion mass spectroscopy (SIMS), in combination with DCTS, is used to explain the electron trapping effects. Traps associated with the C-doping in the back-barrier are identified and the bias ranges for the trap activation are discussed. The study shows the importance of considering the C-doping level in the back-barrier of microwave GaN HEMTs for power amplification and generation. (Less)
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author
; ; ; ; and
organization
publishing date
type
Contribution to journal
publication status
published
subject
keywords
AlGaN/GaN, Aluminum gallium nitride, back-barrier, dispersion, double heterostructure, Electrons, Epitaxial growth, HEMTs, high electron mobility transistors (HEMTs), Logic gates, MODFETs, short channel effect (SCE), Wide band gap semiconductors
in
IEEE Transactions on Electron Devices
volume
71
issue
6
pages
7 pages
publisher
IEEE - Institute of Electrical and Electronics Engineers Inc.
external identifiers
  • scopus:85192168603
ISSN
0018-9383
DOI
10.1109/TED.2024.3392177
language
English
LU publication?
yes
id
210b7968-e6b8-42bb-b01a-d10b21077303
date added to LUP
2024-05-16 12:49:53
date last changed
2025-04-04 14:59:33
@article{210b7968-e6b8-42bb-b01a-d10b21077303,
  abstract     = {{The impact of different carbon concentrations in the Al 0.06 Ga 0.94 N graded back-barrier and GaN buffer of high electron mobility transistors (HEMTs) is investigated. Four epi-wafers with different carbon concentrations, ranging from 1  ×  10 17  to 5  ×  10 17  cm −3 , were grown by metal organic chemical vapor deposition (MOCVD). HEMTs with 100 and 200 nm gate lengths were fabricated and characterized with dc, Pulsed-IV, drain current transient spectroscopy (DCTS), and large-signal measurements at 30 GHz. It is shown that the back-barrier effectively prevents buffer-related electron trapping. The highest C-doping provides the best 2DEG confinement, while lower carbon doping levels are beneficial for a high output power and efficiency. A C-doping of 1  ×  10 17  cm −3 offers the highest output power at maximum power added efficiency (PAE) (1.8 W/mm), whereas 3  ×  10 17  cm −3  doping provides the highest PAE ( > 40%). The C-profiles acquired by using secondary ion mass spectroscopy (SIMS), in combination with DCTS, is used to explain the electron trapping effects. Traps associated with the C-doping in the back-barrier are identified and the bias ranges for the trap activation are discussed. The study shows the importance of considering the C-doping level in the back-barrier of microwave GaN HEMTs for power amplification and generation.}},
  author       = {{Castillo, Ragnar Ferrand Drake Del and Chen, Ding Yuan and Chen, Jr Tai and Thorsell, Mattias and Darakchieva, Vanya and Rorsman, Niklas}},
  issn         = {{0018-9383}},
  keywords     = {{AlGaN/GaN; Aluminum gallium nitride; back-barrier; dispersion; double heterostructure; Electrons; Epitaxial growth; HEMTs; high electron mobility transistors (HEMTs); Logic gates; MODFETs; short channel effect (SCE); Wide band gap semiconductors}},
  language     = {{eng}},
  number       = {{6}},
  pages        = {{3596--3602}},
  publisher    = {{IEEE - Institute of Electrical and Electronics Engineers Inc.}},
  series       = {{IEEE Transactions on Electron Devices}},
  title        = {{Characterization of Trapping Effects Related to Carbon Doping Level in AlGaN Back-Barriers for AlGaN/GaN HEMTs}},
  url          = {{http://dx.doi.org/10.1109/TED.2024.3392177}},
  doi          = {{10.1109/TED.2024.3392177}},
  volume       = {{71}},
  year         = {{2024}},
}