Polymetallic citric complexes as precursors for spray-pyrolysis deposition of thin LaFeO3 films

2014 ◽  
Vol 562 ◽  
pp. 43-48 ◽  
Author(s):  
M. Milanova ◽  
J. Zaharieva ◽  
R. Todorovska ◽  
D. Todorovsky
2011 ◽  
Vol 257 (17) ◽  
pp. 7821-7826 ◽  
Author(s):  
M. Milanova ◽  
I. Koleva ◽  
R. Todorovska ◽  
J. Zaharieva ◽  
M. Кostadinov ◽  
...  

2002 ◽  
Vol 56 (5) ◽  
pp. 770-774 ◽  
Author(s):  
R.V Todorovska ◽  
St Groudeva-Zotova ◽  
D.S Todorovsky

2016 ◽  
Vol 319 ◽  
pp. 48-55 ◽  
Author(s):  
L. dos Santos-Gómez ◽  
J.M. Porras-Vázquez ◽  
F. Martín ◽  
J.R. Ramos-Barrado ◽  
E.R. Losilla ◽  
...  

2004 ◽  
Vol 2 (1) ◽  
pp. 188-195
Author(s):  
N. Mihailov ◽  
O. Vankov ◽  
N. Petrova ◽  
D. Kovacheva

AbstractThin films (50–1200 nm) of YFeO3 were deposited on fused silica substrates by spray-pyrolysis using ethylene glycol solution of Y-Fe(III) citric complexes. The films were post deposition annealed at 750°C in static air for 2 h. Films obtained in this way were afterwards irradiated by a burst mode operated Nd-YAG laser (pulse energy 650 mJ, pulse duration 700 μs, energy density 110 mJ/cm2). The laser’s onset was synchronized with that of a magnetic field pulse of nearly square shape (magnetic induction 0.5 T, pulse duration 900 μs). The samples were placed normally to the direction of the magnetic field. The treatment does not affect the phase composition of the film but significantly increases the crystallite sizes of the phases presenting in the sample. The saturation magnetization of the films decreases as a result of the laser and magnetic field treatment and the coercive force increases by 50%.


2013 ◽  
Vol 04 (01) ◽  
pp. 142-145 ◽  
Author(s):  
Noriyuki Kitagawa ◽  
Seigo Ito ◽  
Duy-Cuong Nguyen ◽  
Hitoshi Nishino

1995 ◽  
Vol 403 ◽  
Author(s):  
V. Foglietti ◽  
A. Galbato ◽  
A. Bearzotti ◽  
A. Galloppa ◽  
P. Maltese

AbstractBismuth-doped tin oxide films have been deposited using a new spray-pyrolysis deposition system. Among the properties are the possibility of depositing thin films over very large areas with good uniformity and the relatively small cost compared with other types of deposition systems. The apparatus is divided in two major parts, the aerosol chamber and the deposition chamber. The deposition chamber consists of a flat rotating hot plate that can house substrates up to 18 cm in diameter. Deposition temperature ranges from 290 °C to 350 °C. The SEM pictures show a phase transition from amorphous to polycrystalline which also strongly affects the transport properties of the film. The high values of the surface resistivity obtained are consistent with those ones required to develop an analog grey scale ferroelectric liquid crystal display. The sample shows a 20% uniformity in the value of surface resistivity over an area of 140 cm2, and the results obtained until now show a satisfactory reproducibility. Bismuth and Tin concentration versus deposition temperature have been determined by ICP mass spectrometry. Our work is supported by the ESPRIT project “PROFELICITA”.


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