scholarly journals Preparation of Bi-Pb-Sr-Ca-Cu-O High Tc Thick Films on Ag or MgO Substrate with Superconductor Paste.

1995 ◽  
Vol 42 (7) ◽  
pp. 817-820
Author(s):  
Toshiaki Ishikawa ◽  
Takashi Tsubota ◽  
Kentaro Ohhashi ◽  
Nobuyoshi Takabatake
Keyword(s):  
High Tc ◽  
Materials ◽  
2019 ◽  
Vol 12 (6) ◽  
pp. 861 ◽  
Author(s):  
J. Mejía-Salazar ◽  
José Perea ◽  
Roberto Castillo ◽  
Jesús Diosa ◽  
Eval Baca

We report here on the development of composite thick films exhibiting hybrid superconducting and ferromagnetic properties, produced through a low-cost, fast, and versatile process. These films were made of high Tc cuprate superconductor Bi2Sr2(Ca,Y)2Cu3O10 (with Y:Ca ratio of 5%) and ferromagnetic perovskite La2/3Ba1/3MnO3, synthesized by melting-quenching annealing process on a MgO substrate. Curie temperature for La2/3Ba1/3MnO3 was determined (~336 K ) by magnetic field assisted thermogravimetric analysis (TGA), while superconducting behavior of Bi2Sr2(Ca,Y)2Cu3O10/MgO films was observed through temperature-dependent resistance measurements. Superconducting features in our hybrid compound were corroborated by temperature-dependent resistivity and magnetic susceptibility.


Author(s):  
Michiharu Ichikawa ◽  
Hiroyuki Kado ◽  
Masatoyo Shibuya ◽  
Masahiro Kojima ◽  
Masakazu Kawahara ◽  
...  

1988 ◽  
Vol 27 (Part 2, No. 7) ◽  
pp. L1297-L1299 ◽  
Author(s):  
Kazutomo Hoshino ◽  
Hidefusa Takahara ◽  
Masao Fukutomi
Keyword(s):  

1992 ◽  
Vol 06 (05) ◽  
pp. 265-272 ◽  
Author(s):  
K. SUGAWARA ◽  
T. SUGIMOTO ◽  
D.J. BAAR ◽  
Y. SHIOHARA ◽  
S. TANAKA

Non-resonant microwave absorption (NRMA) studies have been done for Bi-Sr-Ca-Cu-O (BSCCO) films with thicknesses of 30 Å and 15 Å fabricated on MgO substrate by MOCVD. For the latter two kinds of samples have been fabricated: BSCCO/MgO and BiOx/BSCCO/MgO . NRMA signals have been detected up to about 70–75 K for all the samples. The lower critical magnetic field H c1 * of the 30 Å film was severely increased by the application of a magnetic field of several kGauss, whereas it is almost unaffected in the case of 15 Å films. H c1 * increases but the signal intensity decreases with increasing temperature for all the 30 Å and 15 Å samples. The temperature dependence of the intensity is quite different from that of thicker films (100 Å and 350 Å), in which the intensity vs. temperature relation has a peak (or peaks) at particular temperature(s).


1990 ◽  
Vol 37 (5) ◽  
pp. 688-691
Author(s):  
Yoshimitu Ogawa ◽  
Junichi Ishiai ◽  
Yutaka Mitsune ◽  
Yuzo Tasaki ◽  
Shuji Yoshizawa
Keyword(s):  
High Tc ◽  

1988 ◽  
Vol 96 (1112) ◽  
pp. 450-454 ◽  
Author(s):  
Junji TABUCHI ◽  
Atsushi OCHI ◽  
Kazuaki UTSUMI ◽  
Masatomo YONEZAWA
Keyword(s):  
High Tc ◽  

Cryogenics ◽  
1990 ◽  
Vol 30 (7) ◽  
pp. 593-598 ◽  
Author(s):  
A. Uusimäki ◽  
I. Kirschner ◽  
J. Levoska ◽  
J. Hagberg ◽  
G. Zsolt ◽  
...  

2004 ◽  
Vol 17 (10) ◽  
pp. 1133-1138 ◽  
Author(s):  
M Mora ◽  
F Gimeno ◽  
L A Angurel ◽  
G F de la Fuente
Keyword(s):  

1988 ◽  
Vol 153-155 ◽  
pp. 808-809 ◽  
Author(s):  
E. Beyne ◽  
C. Deneffe ◽  
J. Roggen ◽  
J. Fransaer ◽  
O. Arkens ◽  
...  

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