X-ray, optical and electrical characterization of doped nanocrystalline titanium oxide thin films

2004 ◽  
Vol 109 (1-3) ◽  
pp. 249-251 ◽  
Author(s):  
J Domaradzki ◽  
E.L Prociow ◽  
D Kaczmarek ◽  
T Berlicki ◽  
A Podhorodecki ◽  
...  
1990 ◽  
Vol 37 (1) ◽  
pp. 141-144
Author(s):  
Tsunekazu Iwata ◽  
Akihiko Yamaji ◽  
Youichi Enomoto

2006 ◽  
Vol 99 (10) ◽  
pp. 103704 ◽  
Author(s):  
Yim Fun Loo ◽  
Stephen Taylor ◽  
Robert T. Murray ◽  
Anthony C. Jones ◽  
Paul R. Chalker

1990 ◽  
pp. 773-776
Author(s):  
T. Iwata ◽  
Y. Enomoto ◽  
S. Kubo ◽  
K. Moriwaki ◽  
A. Yamaji

2004 ◽  
Vol 341 (1-3) ◽  
pp. 68-76 ◽  
Author(s):  
D Manno ◽  
A Serra ◽  
G Micocci ◽  
T Siciliano ◽  
E Filippo ◽  
...  

2004 ◽  
Vol 27 (3) ◽  
pp. 169-181 ◽  
Author(s):  
K. Hafidi ◽  
M. Azizan ◽  
Y. Ijdiyaou ◽  
E. L. Ameziane

Deposited titanium oxide thin films are used as optical protector films for several materials and as energy converters for solar cells. In this work, titanium oxide thin films are deposited on c-Si and glass substrates by reactive radiofrequency sputtering. All the deposits are grown at ambient temperature and the sputtering gas is a mixture of oxygen and argon with an overall pressure of10−2mbar. The oxygen partial pressure ratios varies from 5% to 20%.Characterization of deposited films is made by grazing incidence X-ray diffraction (GIXD), grazing incidence X-ray reflection (GIXR), X-ray photoemission spectroscopy (XPS) and optical transmission spectroscopy. The characterization results reveal that deposited films of TiO2 are polycrystalline and present both rutile and anatase phases. The chemical composition of raw films in Ti:O ratio is equal to 1:2.02, and the titanium at surface is completely oxidized. In fact, the Ti2p core level behavior shows that the oxidization state of Ti is equal to+4.The specularily reflected intensity according to incidence angle of the X-ray on TiO2/glass structure shows one critical angle attributed to the TiO2 film equal to 0.283º. This angle value involves film density between rutile and anatase phases. The optical characterization shows that TiO2 thin films obtained are transparent in visible range, and have a refraction index value equal to 2.45 and when extrapolated to infrared range, it is equal to 2.23. The value of gap energy (3.35 eV) is deduced from variation of absorption coefficient versus incident radiation energy.


2017 ◽  
Vol 12 (1) ◽  
pp. 42-46
Author(s):  
H. P. De Araújo ◽  
S. G. Dos Santos Filho

This work presents the characterization of birefringent properties of titanium-oxide thin films using spectrophotometry and double-cavity Fabry-Perot structures. All films were deposited by DC sputtering over tilted substrates and the birefringence was characterized as a function of the deposition angle by the numerical difference between the refractive indexes for s- and p-polarized light beams. As a result, the highest value of birefringence (0.03) was obtained for samples tilted at 21º (having the normal axis as reference). A polarizing narrow-band Fabry-Perot filter centered at 400 and 700nm was designed by means of numerical simulations of the multilayer structures using a MATLAB© toolbox to solve the classical optical equations. Using this designed double-cavity Fabry-Perot structure [Ag(40nm) / TiO2(160nm) / Ag(40nm) / TiO2(164nm) / Ag(40nm)], transmittance ratios (Tp/Ts) for p- and s-polarized light beams resulted 1.70 at a wavelength of 699nm and 1.36 at another wavelength of 393nm (centers of the two narrow-band peaks), which corroborated the birefringent characteristics of the nearly-stoichiometric titania (TiO2) thin films.


2007 ◽  
Vol 515 (13) ◽  
pp. 5381-5385 ◽  
Author(s):  
J. Santos‐Cruz ◽  
G. Torres‐Delgado ◽  
R. Castanedo‐Perez ◽  
C.I. Zúñiga‐Romero ◽  
O. Zelaya‐Angel

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