As-Deposited Superconducting Y-Ba-Cu-O Thin Films on Si, SiO2, GaAs and Ni/Cu Substrates by High Pressure DC Sputtering Process

Author(s):  
R. J. Lin ◽  
P. T. Wu
1996 ◽  
Vol 9 (2) ◽  
pp. 171-174 ◽  
Author(s):  
S. P. Chowdhury ◽  
V. Vasudeva Rao

1989 ◽  
Vol 169 ◽  
Author(s):  
R.J. Lin ◽  
Y.L. Lin ◽  
F.M. Pan ◽  
P.T. Wu

AbstractSuperconducting Y‐Ba‐Cu‐0 thin films on (100)GaAs substrate have been successfully prepared by the high pressure DC sputtering process without further post‐annealing treatment. The target was compound Y1Ba2Cu3Ox made by solid‐state reaction. The sputtering gas was Ar‐50%02, and total pressure was 1.5 torr. The substrate temperature was lower than 450°C. The best superconductivity of the film is Tc(onset) = 95K and Tc(R=0) = 40K. There are no mi‐crocracks on the film surface. The interdiffusion between the film and GaAs is limited.


1997 ◽  
Vol 10 (3) ◽  
pp. 221-226 ◽  
Author(s):  
P. B. Mozhaev ◽  
P. V. Komlssinski ◽  
N. P. Kukhta ◽  
A. Kühle ◽  
G. A. Ovsyannikoy ◽  
...  

Author(s):  
O. Eibl ◽  
G. Gieres ◽  
H. Behner

The microstructure of high-Tc YBa2Cu3O7-X thin films deposited by DC-sputtering on SrTiO3 substrates was analysed by TEM. Films were either (i) deposited in the amorphous state at substrate temperatures < 450°C and crystallised by a heat treatment at 900°C (process 1) or (ii) deposited at around 740°C in the crystalline state (process 2). Cross sections were prepared for TEM analyses and are especially useful for studying film substrate interdiffusion (fig.1). Films deposited in process 1 were polycristalline and the grain size was approximately 200 nm. Films were porous and the size of voids was approximately 100 nm. Between the SrTiO3 substrate and the YBa2Cu3Ox film a densly grown crystalline intermediate layer approximately 150 nm thick covered the SrTiO3 substrate. EDX microanalyses showed that the layer consisted of Sr, Ba and Ti, however, did not contain Y and Cu. Crystallites of the layer were carefully tilted in the microscope and diffraction patterns were obtained in five different poles for every crystallite. These patterns were consistent with the phase (Ba1-XSrx)2TiO4. The intermediate layer was most likely formed during the annealing at 900°C. Its formation can be understood as a diffusion of Ba from the amorphously deposited film into the substrate and diffusion of Sr from the substrate into the film. Between the intermediate layer and the surface of the film the film consisted of YBa2Cu3O7-x grains. Films prepared in process 1 had Tc(R=0) close to 90 K, however, critical currents were as low as jc = 104A/cm2 at 77 K.


Coatings ◽  
2021 ◽  
Vol 11 (6) ◽  
pp. 724
Author(s):  
Sara Massardo ◽  
Alessandro Cingolani ◽  
Cristina Artini

Rare earth-doped ceria thin films are currently thoroughly studied to be used in miniaturized solid oxide cells, memristive devices and gas sensors. The employment in such different application fields derives from the most remarkable property of this material, namely ionic conductivity, occurring through the mobility of oxygen ions above a certain threshold temperature. This feature is in turn limited by the association of defects, which hinders the movement of ions through the lattice. In addition to these issues, ionic conductivity in thin films is dominated by the presence of the film/substrate interface, where a strain can arise as a consequence of lattice mismatch. A tensile strain, in particular, when not released through the occurrence of dislocations, enhances ionic conduction through the reduction of activation energy. Within this complex framework, high pressure X-ray diffraction investigations performed on the bulk material are of great help in estimating the bulk modulus of the material, and hence its compressibility, namely its tolerance toward the application of a compressive/tensile stress. In this review, an overview is given about the correlation between structure and transport properties in rare earth-doped ceria films, and the role of high pressure X-ray diffraction studies in the selection of the most proper compositions for the design of thin films.


2009 ◽  
Vol 94 (22) ◽  
pp. 222110 ◽  
Author(s):  
S. S. N. Bharadwaja ◽  
C. Venkatasubramanian ◽  
N. Fieldhouse ◽  
S. Ashok ◽  
M. W. Horn ◽  
...  

2012 ◽  
Vol 12 (12) ◽  
pp. 9234-9237 ◽  
Author(s):  
M. A. Vasquez-A. ◽  
Goiz O. ◽  
R. Baca-Arroyo ◽  
J. A. Andraca-Adame ◽  
G. Romero-Paredes ◽  
...  
Keyword(s):  

2012 ◽  
Vol 152 (6) ◽  
pp. 478-482 ◽  
Author(s):  
J. Li ◽  
W. Peng ◽  
Ke Chen ◽  
Y. Zhang ◽  
L.M. Cui ◽  
...  

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