Thin films of praseodymium sesquioxide: Martensitic character of the monoclinic to hexagonal phase transformation

1971 ◽  
Vol 34 (7) ◽  
pp. 437-438 ◽  
Author(s):  
C. Boulesteix ◽  
P.-E. Caro ◽  
M. Gasgnier ◽  
Ch.H. La Blanchetais ◽  
G. Schiffmacher
CrystEngComm ◽  
2018 ◽  
Vol 20 (43) ◽  
pp. 6919-6924 ◽  
Author(s):  
Hong Jia ◽  
Yiping Zhou ◽  
Xue Li ◽  
Yan Li ◽  
Weiying Zhang ◽  
...  

Herein, a thin film of hexagonal-phase NaGdF4:Yb–Er is fabricated by electro-deposition at moderate temperatures. The phase of NaGdF4:Yb–Er thin film can be controlled by adding PVP in the electrolyte.


1992 ◽  
Vol 7 (11) ◽  
pp. 3065-3071 ◽  
Author(s):  
Peir-Yung Chu ◽  
Isabelle Campion ◽  
Relva C. Buchanan

Phase transformation and preferred orientation in ZrO2 thin films, deposited on Si(111) and Si(100) substrates, and prepared by heat treatment from carboxylate solution precursors were investigated. The deposited films were amorphous below 450 °C, transforming gradually to the tetragonal and monoclinic phases on heating. The monoclinic phase developed from the tetragonal phase displacively, and exhibited a strong (111) preferred orientation at temperature as low as 550 °C. The degree of preferred orientation and the tetragonal-to-monoclinic phase transformation were controlled by heating rate, soak temperature, and time. Interfacial diffusion into the film from the Si substrate was negligible at 700 °C and became significant only at 900 °C, but for films thicker than 0.5 μm, overall preferred orientation exceeded 90%.


2021 ◽  
Vol 32 (8) ◽  
pp. 10018-10027
Author(s):  
M. A. Olgar ◽  
B. M. Başol ◽  
M. Tomakin ◽  
E. Bacaksız

2021 ◽  
Vol 266 ◽  
pp. 115078
Author(s):  
R. Ning ◽  
Z.P. Yang ◽  
Z.Y. Gao ◽  
X.Z. Cao ◽  
W. Cai

2020 ◽  
Vol 195 ◽  
pp. 109020
Author(s):  
Chun-Yuan Wang ◽  
Chin-I Wang ◽  
Sheng-Han Yi ◽  
Teng-Jan Chang ◽  
Chun-Yi Chou ◽  
...  

1985 ◽  
Vol 48 ◽  
Author(s):  
P. Alexopoulos ◽  
R. H. Geiss ◽  
M. Schlenker

ABSTRACTThin films of Co-10 at% Pt, ranging from 15 to 90 nm in thickness, have been DC-sputtered at various temperatures on to carbon-coated mica, carbon substrates on copper grids, or (001) silicon single crystals under 3 μm pressure of Ar, using targets of the alloy in the hexagonal phase, at growth rates of 9 nm/min. The samples were investigated by TEM, using bright-and dark-field imaging, lattice imaging, selected area diffraction and both Fresnel and focussed Lorentz modes. The primary structure of the films was found to be hexagonal, with a = 0.255 nm and c = 0.414 nm. For the samples sputtered at room temperature, the grain sizes were on the order of 0.μm on carbon-coated mica and carbon-substrate grids, and approximately an order of magnitude smaller on silicon substrates. Heavy streaking along the [001] of the hexagonal matrix was observed on diffraction patterns for grains having the [001] parallel to the surface; this streaking was found to be associated with the presence of a high density of faults parallel to the (001). In films sputtered on to carbon-coated mica at 225 °C, where a substantial reduction of the coercivity is observed, the overwhelming majority of the grains had the (001) basal plane parallel to the surface. Lorentz microscopy showed the magnetic domain structure in films grown on silicon to be markedly different from those grown on the carbon substrates, and further changes occurred for the films grown at elevated temperatures.


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