Shigefusa F. Chichibu
(Institute of Multidisciplinary Research for Advanced Materials, Tohoku University)
;
Kohei Shima
(Institute of Multidisciplinary Research for Advanced Materials, Tohoku University)
;
Akira Uedono
(Department of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8573, Japan)
;
Shoji Ishibashi
(AIST)
;
Hiroko Iguchi
(TOYOTA CENTRAL R&D LABS., INC.)
;
Tetsuo Narita
(TOYOTA CENTRAL R&D LABS., INC.)
;
Keita Kataoka
(TOYOTA CENTRAL R&D LABS., INC.)
;
Ryo Tanaka
(Fuji Electric Corporation)
;
Shinya Takashima
(Fuji Electric Corporation)
;
Katsunori Ueno
(Fuji Electric Corporation)
;
Masaharu Edo
(Fuji Electric Corporation)
;
Hirotaka Watanabe
(Institute of Materials and Systems for Sustainability, Nagoya University)
;
Atsushi Tanaka
(Institute of Materials and Systems for Sustainability, Nagoya University)
;
Yoshio Honda
(Institute of Materials and Systems for Sustainability, Nagoya University)
;
Jun Suda
(Institute of Materials and Systems for Sustainability, Nagoya University)
;
Hiroshi Amano
(Institute of Materials and Systems for Sustainability, Nagoya University)
;
Tetsu Kachi
(Institute of Materials and Systems for Sustainability, Nagoya University)
;
Toshihide Nabatame
(Research Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science
)
;
Yoshihiro Irokawa
(Research Center for Electronic and Optical Materials/Functional Materials Field/Next-generation Semiconductor Group, National Institute for Materials Science
)
;
Yasuo Koide
(Research Center for Electronic and Optical Materials/Functional Materials Field/Next-generation Semiconductor Group, National Institute for Materials Science
)
Description:
(abstract)For rooting the development of GaN-based optoelectronic devices, understanding the roles of midgap recombination centers (MGRCs), namely nonradiative recombination centers and deep-state radiative recombination centers, on the carrier recombination dynamics is an essential task. By using the combination of time-resolved photoluminescence and positron annihilation spectroscopy (PAS) measurements, the origins of major MGRCs in the state-of-the-art GaN epilayers, bulk crystals, and Mg-implanted layers were identified and their concentrations were quantified for deriving the capture coefficients of minority carriers. In this article, potential standardization of the room-temperature photoluminescence lifetime for the near-band-edge emission (𝜏PLRT) as the concentration of major MGRCs well below the detection limit of PAS is proposed. For n-GaN substrates and epilayers grown from the vapor phase, 𝜏PLRT was limited by the concentration of carbon on N sites or divacancies comprising a Ga vacancy (VGa) and a N vacancy (VN), [VGaVN], when carbon concentration was higher or lower, respectively, than approximately 1016 cm-3. Here, carbon and VGaVN act as major deep-state radiative and nonradiative recombination centers, respectively. While, major MGRCs in bulk GaN crystals were identified as VGa(VN)3 vacancy clusters in Na-flux GaN and VGa or VGaVN buried by a hydrogen and/or VGa decorated with oxygen on N sites, VGa(ON)3-4, inammonothermal GaN. The values of 𝜏PLRT in n-GaN samples are compared with those of p-GaN, in which 𝜏PLRT was limited by the concentration of VGa(VN)2 in Mg-doped epilayers while by the concentrations of VGaVN and (VGaVN)3 in Mg-implanted GaN right after the implantation and after appropriate activation annealings, respectively.
Rights:
Keyword: GaN
Date published: 2024-05-14
Publisher: American Institute of Physics
Journal:
Funding:
Manuscript type: Publisher's version (Version of record)
MDR DOI:
First published URL: https://doi.org/10.1063/5.0201931
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Updated at: 2024-05-09 16:30:16 +0900
Published on MDR: 2024-05-09 16:30:17 +0900
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