Al2O3 Obtained through Resistive Evaporation for Use as Insulating Layer in Transparent Field Effect Transistor

2014 ◽  
Vol 975 ◽  
pp. 248-253 ◽  
Author(s):  
Miguel Henrique Boratto ◽  
Luis Vicente de Andrade Scalvi ◽  
Diego Henrique de Oliveira Machado

Alumina thin films have been obtained by resistive evaporation of Al layer, followed by thermal oxidation achieved by annealing in appropriate atmosphere (air or O2-rich), with variation of annealing time and temperature. Optical and structural properties of the investigated films reveal that the temperature of 550°C is responsible for fair oxidation. Results of surface electrical resistivity, Raman and infrared spectroscopies are in good agreement with this finding. X-ray and Raman data also suggest the crystallization of Si nuclei at glass substrate-alumina interface, which would come from the soda-lime glass used as substrate. The main goal in this work is the deposition of alumina on top of SnO2 to build a transparent field-effect transistor. Some microscopy results of the assembled SnO2/Al2O3 heterostructure are also shown.

2014 ◽  
Vol 2 (44) ◽  
pp. 9359-9363 ◽  
Author(s):  
Juan Zhu ◽  
Wenchong Wang ◽  
Qigang Zhong ◽  
Liqiang Li ◽  
Chuan Du ◽  
...  

The patterned growth of crystalline rubrene films directly on electrodes is demonstrated. In addition, organic films with close packed and porous structures are locally achieved by controlling the electrode spaces, resulting in a two orders of magnitude difference in carrier mobility.


2018 ◽  
Vol 96 (7) ◽  
pp. 804-809 ◽  
Author(s):  
Harun Güney ◽  
Demet İskenderoğlu

The undoped and 1%, 2%, and 3% Cd-doped MgO nanostructures were grown by SILAR method on the soda lime glass substrate. X-ray diffractometer (XRD), ultraviolet–visible spectrometer, scanning electron microscope, photoluminescence (PL), and X-ray photoelectron spectroscopy measurements were taken to investigate Cd doping effects on the structural, optical, and morphological properties of MgO nanostructures. XRD measurements show that the samples have cubic structure and planes of (200), (220) of MgO and (111), (200), and (220) of CdO. It was observed that band gaps increase with rising Cd doping rate in MgO thin film. The surface morphology of samples demonstrates that MgO nanostructures have been affected by the Cd doping. PL measurements show that undoped and Cd-doped MgO thin films can radiate in the visible emission region.


2005 ◽  
Vol 15 (3) ◽  
pp. 375-380 ◽  
Author(s):  
F. Cicoira ◽  
C. Santato ◽  
F. Dinelli ◽  
M. Murgia ◽  
M. A. Loi ◽  
...  

2010 ◽  
Vol 107 (2) ◽  
pp. 024101 ◽  
Author(s):  
Meiyong Liao ◽  
Yasuhito Gotoh ◽  
Hiroshi Tsuji ◽  
Kiyomi Nakajima ◽  
Masataka Imura ◽  
...  

1993 ◽  
Vol 3 (1) ◽  
pp. 1987-1990 ◽  
Author(s):  
L. Zhang ◽  
N. Yoshikawa ◽  
M. Sugahara

2013 ◽  
Vol 716 ◽  
pp. 325-327
Author(s):  
Xiao Yan Dai ◽  
Cheng Wu Shi ◽  
Yan Ru Zhang ◽  
Min Yao

In this paper, CdTe thin films were deposited on soda-lime glass substrates using CdTe powder as a source by close-spaced sublimation at higher source temperature of 700°C. The influence of the deposition time and the source-substrate distance on the chemical composition, crystal phase, surface morphology and optical band gap of CdTe thin films was systemically investigated by energy dispersive X-ray spectroscopy, X-ray diffraction, scanning electron microscope and the ultraviolet-visible-near infrared absorption spectra, respectively. At the deposition time of 60 min and the source-substrate distance of 5 mm, the CdTe thin films had pyramid appearance with the grain size of 15 μm.


2013 ◽  
Vol 15 (47) ◽  
pp. 20611 ◽  
Author(s):  
Ritsuko Eguchi ◽  
Xuexia He ◽  
Shino Hamao ◽  
Hidenori Goto ◽  
Hideki Okamoto ◽  
...  

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