Tailoring Subthreshold Swing in A-IGZO Thin-Film Transistors for Amoled Displays: Impact of Conversion Mechanism on Peald Deposition Sequences
- Authors
- Yoon, Seong Hun; Cho, Jae Hun; Cho, Iaan; Kim, Min Jae; Hur, Jae Seok; Bang, Seon Woong; Lee, Heung Jo; Bae, Jong Uk; Kim, Jiyoung; Shong, Bonggeun; Jeong, Jae Kyeong
- Issue Date
- Aug-2024
- Publisher
- WILEY-V C H VERLAG GMBH
- Keywords
- atomic layer deposition; conversion mechanism; defect mechanism; density functional theory; field-effect transistor; indium gallium zinc oxide; precursor; TCAD simulation
- Citation
- Small Methods, v.8, no.8, pp 1 - 12
- Pages
- 12
- Indexed
- SCIE
SCOPUS
- Journal Title
- Small Methods
- Volume
- 8
- Number
- 8
- Start Page
- 1
- End Page
- 12
- URI
- https://scholarworks.bwise.kr/hanyang/handle/2021.sw.hanyang/206322
- DOI
- 10.1002/smtd.202301185
- ISSN
- 2366-9608
2366-9608
- Abstract
- Amorphous IGZO (a-IGZO) thin-film transistors (TFTs) are standard backplane electronics to power active-matrix organic light-emitting diode (AMOLED) televisions due to their high carrier mobility and negligible low leakage characteristics. Despite their advantages, limitations in color depth arise from a steep subthreshold swing (SS) (≤ 0.1 V/decade), necessitating costly external compensation for IGZO transistors. For mid-size mobile applications such as OLED tablets and notebooks, it is important to ensure controllable SS value (≥ 0.3 V/decade). In this study, a conversion mechanism during plasma-enhanced atomic layer deposition (PEALD) is proposed as a feasible route to control the SS. When a pulse of a diethylzinc (DEZn) precursor is exposed to the M2O3 (M = In or Ga) surface layer, partial conversion of the underlying M2O3 to ZnO is predicted on the basis of density function theory calculations. Notably, significant distinctions between In-Ga-Zn (Case I) and In-Zn-Ga (Case II) films are observed: Case II exhibits a lower growth rate and larger Ga/In ratio. Case II TFTs with a-IGZO (subcycle ratio of In:Ga:Zn = 3:1:1) show reasonable SS values (313 mV decade−1) and high mobility (µFE) of 29.3 cm2 Vs−1 (Case I: 84 mV decade−1 and 33.4 cm2 Vs−1). The rationale for Case II's reasonable SS values is discussed, attributing it to the plausible formation of In-Zn defects, supported by technology computer-aided design (TCAD) simulations.
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