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Impacts of vacancy complexes on the room-temperature photoluminescence lifetimes of state-of-the-art GaN substrates, epitaxial layers, and Mg-implanted layers.

Authors :
Chichibu, Shigefusa F.
Shima, Kohei
Uedono, Akira
Ishibashi, Shoji
Iguchi, Hiroko
Narita, Tetsuo
Kataoka, Keita
Tanaka, Ryo
Takashima, Shinya
Ueno, Katsunori
Edo, Masaharu
Watanabe, Hirotaka
Tanaka, Atsushi
Honda, Yoshio
Suda, Jun
Amano, Hiroshi
Kachi, Tetsu
Nabatame, Toshihide
Irokawa, Yoshihiro
Koide, Yasuo
Source :
Journal of Applied Physics; 5/14/2024, Vol. 135 Issue 18, p1-20, 20p
Publication Year :
2024

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 (τ PL RT ) 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, τ PL RT was limited by the concentration of carbon on N sites or divacancies comprising a Ga vacancy (V<subscript>Ga</subscript>) and a N vacancy (V<subscript>N</subscript>), [V<subscript>Ga</subscript>V<subscript>N</subscript>], when carbon concentration was higher or lower, respectively, than approximately 10<superscript>16</superscript> cm<superscript>−3</superscript>. Here, carbon and V<subscript>Ga</subscript>V<subscript>N</subscript> act as major deep-state radiative and nonradiative recombination centers, respectively, while major MGRCs in bulk GaN crystals were identified as V<subscript>Ga</subscript>(V<subscript>N</subscript>)<subscript>3</subscript> vacancy clusters in Na-flux GaN and V<subscript>Ga</subscript> or V<subscript>Ga</subscript>V<subscript>N</subscript> buried by a hydrogen and/or V<subscript>Ga</subscript> decorated with oxygen on N sites, V<subscript>Ga</subscript>(O<subscript>N</subscript>)<subscript>3–4</subscript>, in ammonothermal GaN. The values of τ PL RT in n-GaN samples are compared with those of p-GaN, in which τ PL RT was limited by the concentration of V<subscript>Ga</subscript>(V<subscript>N</subscript>)<subscript>2</subscript> in Mg-doped epilayers and by the concentrations of V<subscript>Ga</subscript>V<subscript>N</subscript> and (V<subscript>Ga</subscript>V<subscript>N</subscript>)<subscript>3</subscript> in Mg-implanted GaN right after the implantation and after appropriate activation annealing, respectively. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00218979
Volume :
135
Issue :
18
Database :
Complementary Index
Journal :
Journal of Applied Physics
Publication Type :
Academic Journal
Accession number :
177227228
Full Text :
https://doi.org/10.1063/5.0201931