Effects of Al2O3 surface passivation on the radiation hardness of IGTO thin films for thin-film transistor applications

2021 ◽  
pp. 152096
Author(s):  
Seong-Hyun Hwang ◽  
Kie Yatsu ◽  
Dong-Ho Lee ◽  
Ick-Joon Park ◽  
Hyuck-In Kwon
2003 ◽  
Vol 769 ◽  
Author(s):  
Seong Deok Ahn ◽  
Seung Youl Kang ◽  
Yong Eui Lee ◽  
Meyoung Ju Joung ◽  
Chul Am Kim ◽  
...  

AbstractWe have investigated the growth mechanism and thin film morphology of pentacene thin films by the process of low-pressure gas assisted organic vapor deposition (LP-GAOVD). As the source temperature, flow rate of the carrier gas, substrate temperature and chamber pressure were varied, the growth rate, morphology and grain size of the films were differently obtained. The electrical properties of pentacene thin films for applications in organic thin film transistor and electrophoretic displays were discussed


2020 ◽  
Vol 116 (18) ◽  
pp. 182104 ◽  
Author(s):  
Dun-Bao Ruan ◽  
Po-Tsun Liu ◽  
Kai-Jhih Gan ◽  
Yu-Chuan Chiu ◽  
Chih-Chieh Hsu ◽  
...  

RSC Advances ◽  
2019 ◽  
Vol 9 (54) ◽  
pp. 31386-31397 ◽  
Author(s):  
Nico Koslowski ◽  
Rudolf C. Hoffmann ◽  
Vanessa Trouillet ◽  
Michael Bruns ◽  
Sabine Foro ◽  
...  

Transformation of a new molecular precursor allows the formation of yttrium oxide under moderate conditions displaying high voltage breakthrough behaviour.


2015 ◽  
Vol 4 (3) ◽  
pp. Q26-Q30 ◽  
Author(s):  
Min Liao ◽  
Zewen Xiao ◽  
Fan-Yong Ran ◽  
Hideya Kumomi ◽  
Toshio Kamiya ◽  
...  

AIP Advances ◽  
2016 ◽  
Vol 6 (1) ◽  
pp. 015112 ◽  
Author(s):  
Fan-Yong Ran ◽  
Zewen Xiao ◽  
Hidenori Hiramatsu ◽  
Keisuke Ide ◽  
Hideo Hosono ◽  
...  

2009 ◽  
Vol 1153 ◽  
Author(s):  
Ruud E.I. Schropp ◽  
Zomer Silvester Houweling ◽  
Vasco Verlaan

AbstractHot Wire Chemical Vapor Deposition (HWCVD) is a fast deposition technique with high potential for homogeneous deposition of thin films on large area panels or on continuously moving substrates in an in-line manufacturing system. As there are no high-frequency electromagnetic fields, scaling up is not hampered by finite wavelength effects or the requirement to avoid inhomogeneous electrical fields. Since 1996 we have been investigating the application of the HWCVD process for thin film transistor manufacturing. It already appeared then that these Thin Film Transistors (TFTs) were electronically far more stable than those with Plasma Enhanced (PE) CVD amorphous silicon. Recently, we demonstrated that very compact SiNx layers can be deposited at high deposition rates, up to 7 nm/s. The utilization of source gases in HWCVD of a-Si3N4 films deposited at 3 nm/s is 75 % and 7 % for SiH4 and NH3, respectively. Thin films of stoichiometric a-Si3N4 deposited at this rate have a high mass-density of 3.0 g/cm3. The dielectric properties have been evaluated further in order to establish their suitability for incorporation in TFTs. Now that all TFT layers, namely, the SiNx insulator, the a-Si:H or μc Si:H layers, and the n-type doped thin film silicon can easily be manufactured by HWCVD, the prospect of “all HWCVD” TFTs for active matrix production is within reach. We tested the 3 nm/s SiNx material combined with our protocrystalline Si:H layers deposited at 1 nm/s in ‘all HW’ TFTs. Results show that the TFTs are state of the art with a field-effect mobility of 0.4 cm2/Vs. In order to assess the feasibility of large area deposition we are investigating in-line HWCVD for displays and solar cells.


2013 ◽  
Vol 284-287 ◽  
pp. 225-229 ◽  
Author(s):  
Chao Nan Chen ◽  
Jung Jie Huang ◽  
Gwo Mei Wu ◽  
How Wen Chien

Silicon nitride (SiNx), an important material used as a dielectric layer and passivation layer in thin film transistor liquid crystal display (TFT LCD) was patterned by a non-lithographic process. SiNx was deposited by plasma enhanced chemical vapor deposition (PECVD) on glass substrate. Laser photoablation can effectively pattern 5 µm diameter with 200 nm depth hole in SiNx thin films with laser photoablation. The threshold remove fluence is 1350 mJ/cm2 with 1 laser irradiation shot. The contact-hole taper angle as a function of the laser irradiation shot number. The taper angle increased with increasing the laser irradiation shot number. The contact-hole taper angle etched profile was successfully controlled by vary the laser irradiation shot number.


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