scholarly journals Voltage-Polarity Dependent Programming Behaviors of Amorphous In–Ga–Zn–O Thin-Film Transistor Memory with an Atomic-Layer-Deposited ZnO Charge Trapping Layer

2019 ◽  
Vol 14 (1) ◽  
Author(s):  
Dan-Dan Liu ◽  
Wen-Jun Liu ◽  
Jun-Xiang Pei ◽  
Lin-Yan Xie ◽  
Jingyong Huo ◽  
...  

AbstractAmorphous In–Ga–Zn-O (a-IGZO) thin-film transistor (TFT) memories are attracting many interests for future system-on-panel applications; however, they usually exhibit a poor erasing efficiency. In this article, we investigate voltage-polarity-dependent programming behaviors of an a-IGZO TFT memory with an atomic-layer-deposited ZnO charge trapping layer (CTL). The pristine devices demonstrate electrically programmable characteristics not only under positive gate biases but also under negative gate biases. In particular, the latter can generate a much higher programming efficiency than the former. Upon applying a gate bias pulse of +13 V/1 μs, the device shows a threshold voltage shift (ΔVth) of 2 V; and the ΔVth is as large as −6.5 V for a gate bias pulse of −13 V/1 μs. In the case of 12 V/1 ms programming (P) and −12 V/10 μs erasing (E), a memory window as large as 7.2 V can be achieved at 103 of P/E cycles. By comparing the ZnO CTLs annealed in O2 or N2 with the as-deposited one, it is concluded that the oxygen vacancy (VO)-related defects dominate the bipolar programming characteristics of the TFT memory devices. For programming at positive gate voltage, electrons are injected from the IGZO channel into the ZnO layer and preferentially trapped at deep levels of singly ionized oxygen vacancy (VO+) and doubly ionized oxygen vacancy (VO2+). Regarding programming at negative gate voltage, electrons are de-trapped easily from neutral oxygen vacancies because of shallow donors and tunnel back to the channel. This thus leads to highly efficient erasing by the formation of additional ionized oxygen vacancies with positive charges.

2011 ◽  
Vol 99 (2) ◽  
pp. 022104 ◽  
Author(s):  
Te-Chih Chen ◽  
Ting-Chang Chang ◽  
Tien-Yu Hsieh ◽  
Wei-Siang Lu ◽  
Fu-Yen Jian ◽  
...  

2010 ◽  
Vol 96 (12) ◽  
pp. 123301 ◽  
Author(s):  
Chang Hyun Kim ◽  
Min Hee Choi ◽  
Sun Hee Lee ◽  
Jin Jang ◽  
Stephan Kirchmeyer

2011 ◽  
Vol 2011 ◽  
pp. 1-12 ◽  
Author(s):  
S. Maikap ◽  
W. Banerjee ◽  
T. C. Tien ◽  
T. Y. Wang ◽  
J. R. Yang

Physical and memory characteristics of the atomic-layer-depositedRuOxmetal nanocrystal capacitors in an n-Si/SiO2/HfO2/RuOx/Al2O3/Pt structure with different postdeposition annealing temperatures from 850–1000°C have been investigated. TheRuOxmetal nanocrystals with an average diameter of 7 nm and a highdensity of 0.7 × 1012/cm2are observed by high-resolution transmission electron microscopy after a postdeposition annealing temperature at 1000°C. The density ofRuOxnanocrystal is decreased (slightly) by increasing the annealing temperatures, due to agglomeration of multiple nanocrystals. The RuO3nanocrystals and Hf-silicate layer at the SiO2/HfO2interface are confirmed by X-ray photoelectron spectroscopy. For post-deposition annealing temperature of 1000°C, the memory capacitors with a small equivalent oxide thickness of ~9 nm possess a large hysteresis memory window of >5 V at a small sweeping gate voltage of ±5 V. A promising memory window under a small sweeping gate voltage of ~3 V is also observed due to charge trapping in theRuOxmetal nanocrystals. The program/erase mechanism is modified Fowler-Nordheim (F-N) tunneling of the electrons and holes from Si substrate. The electrons and holes are trapped in theRuOxnanocrystals. Excellent program/erase endurance of 106cycles and a large memory window of 4.3 V with a small charge loss of ~23% at 85°C are observed after 10 years of data retention time, due to the deep-level traps in theRuOxnanocrystals. The memory structure is very promising for future nanoscale nonvolatile memory applications.


RSC Advances ◽  
2017 ◽  
Vol 7 (83) ◽  
pp. 52517-52523 ◽  
Author(s):  
Jun Li ◽  
Chuan-Xin Huang ◽  
Jian-Hua Zhang

Solution-processed semiconducting single-walled carbon nanotube (s-SWCNT) thin film transistors (TFTs) based on different atomic layer deposited AlZrOx insulators are fabricated and characterized.


2011 ◽  
Vol 26 (8) ◽  
pp. 085007 ◽  
Author(s):  
Byeong-Yun Oh ◽  
Young-Hwan Kim ◽  
Hee-Jun Lee ◽  
Byoung-Yong Kim ◽  
Hong-Gyu Park ◽  
...  

2019 ◽  
Vol 9 (23) ◽  
pp. 5150 ◽  
Author(s):  
Xiaochen Zhang ◽  
Xianzhe Liu ◽  
Kuankuan Lu ◽  
Honglong Ning ◽  
Dong Guo ◽  
...  

In this work, a thin film transistor (TFT) with Zr-doped aluminum-zinc-tin oxide (Zr-AZTO) semiconductor as active layer was investigated. The Zr-AZTO thin films were co-sputtered by ZrO2 and AZTO targets (RF-Sputter) in Ar, and annealed at 350 °C in air atmosphere. With the discharge power of AZTO increasing from 100 W to 120 W, the content of Zr element decreases from 0.63 ± 0.01 at.% to 0.34 ± 0.01 at.%, and the oxygen vacancy decreases from (19.0 ± 0.1)% to (17.3 ± 0.8)%. The results of Zr-AZTO thin film show that the main factor is the co-sputter power of ZrO2 target. With the co-sputter power of ZrO2 increasing from 15 W to 45 W, the content of Zr element increases from 0.63 ± 0.01 at.% to 2.79 ± 0.01 at.%, the content of oxygen vacancy decreases from (19.0 ± 0.1)% to (14.1 ± 0.1)%, Eg increases from 2.76 eV to 2.86 eV, and the root mean square (RMS) roughness firstly decreases from 0.402 nm to 0.387 nm and then increases to 0.490 nm. The Micro Wave Photo Conductivity Decay (μ-PCD, LTA-1620SP) was used to measure the quality of Zr-AZTO thin film and the mean peak and D value decreases from 139.3 mV to 80.9 mV and from 1.54 to 0.77 as the co-sputter power of ZrO2 increases from 15 W to 45 W, which means it has highest localized states and defects in high ZrO2 co-sputter power. The devices prepared at 15 W (ZrO2)/100 W (AZTO) co-sputter show a best performance, with a μsat of 8.0 ± 0.6 cm2/(V∙S), an Ion/Ioff of (2.01 ± 0.34) × 106, and a SS of 0.18 ± 0.03 V/dec. The device of Sample B has a 0.5 V negative shift under −20 V NBS and 9.6 V positive shift under 20 V PBS.


Author(s):  
William Cheng-Yu Ma ◽  
Po-Jen Chen ◽  
Yan-Shiuan Chang ◽  
Jhe-Wei Jhu ◽  
Ting-Hsuan Chang

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