材料科学
薄膜晶体管
AMOLED公司
原子层沉积
光电子学
有源矩阵
有机发光二极管
晶体管
二极管
薄膜
纳米技术
图层(电子)
电气工程
电压
工程类
作者
Seong Hun Yoon,Jaehun Cho,Iaan Cho,Min Jae Kim,Jae Seok Hur,Seon Woong Bang,Heung Jo Lee,Jong Uk Bae,Jiyoung Kim,Bonggeun Shong,Jae Kyeong Jeong
出处
期刊:Small methods
[Wiley]
日期:2024-01-08
卷期号:8 (8): e2301185-e2301185
被引量:20
标识
DOI:10.1002/smtd.202301185
摘要
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 M 2 O 3 (M = In or Ga) surface layer, partial conversion of the underlying M 2 O 3 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 ( µ FE ) of 29.3 cm2 Vs −1 (Case I: 84 mV decade −1 and 33.4 cm 2 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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