Internal friction in high Tc iron doped 1-2-3 yttrium ceramic superconductors

1990 ◽  
Vol 74 (7) ◽  
pp. 595-598 ◽  
Author(s):  
B. Kusz ◽  
R. Barczynski ◽  
M. Gazda ◽  
L. Murawski ◽  
O. Gzowski ◽  
...  
Author(s):  
Chalakara V. Narasimha Rao ◽  
Shyam K. Agarwal ◽  
Betanabhatla Jayaram ◽  
Sylvester Takacs ◽  
Anant V. Narlikar

1987 ◽  
Vol 01 (07n08) ◽  
pp. 275-288 ◽  
Author(s):  
S.R. OVSHINSKY ◽  
S.J. HUDGENS ◽  
R.L. LINTVEDT ◽  
D.B. RORABACHER

A structual chemical model for high Tc ceramic superconductors is proposed in which carriers pairs, coupled through a superexchange process, undergo Bose condensation. In the Y-Ba-Cu-O system, Cu atoms on “chain” sites and “sheet” sites are initially assigned formal oxidation states of +3 and +2, respectively, and “sheet”/“chain” interactions are then introduced to bring about the electrically conductive mixed oxidation state. This model explains the presence of labile oxygen in the “chain” structures, describes the structure of deoxygenated phases exhibiting ordered oxygen vacancies in the “chains”, and allows interpretation of the effects of oxygen removal on magnetic and electronic properties of the material.


1989 ◽  
pp. 281-286
Author(s):  
Shin-ichi Murasaki ◽  
Satoru Taniguchi ◽  
Uichiro Mizutani ◽  
Motohiro Suganuma ◽  
Yuh Yamada

1989 ◽  
Vol 70 (3) ◽  
pp. 333-335 ◽  
Author(s):  
W.G. Zeng ◽  
J.X. Zhang ◽  
G.M. Lin ◽  
C.L. Du ◽  
P.C.W. Fung ◽  
...  

1991 ◽  
Vol 185-189 ◽  
pp. 1373-1374 ◽  
Author(s):  
Linhai Sun ◽  
Yening Wang ◽  
Zhen Yu

1988 ◽  
Vol 37 (1) ◽  
pp. 138-140 ◽  
Author(s):  
Niels Hessel Andersen ◽  
Ib Johannsen ◽  
Mogens T Levinsen

1988 ◽  
Vol 02 (06) ◽  
pp. 1399-1405 ◽  
Author(s):  
MARK JEFFERY ◽  
CHARLES GREEN ◽  
SOMDEV TYAGI ◽  
R. GILMORE

Microwave absorption measurements of the high T c ceramic superconductors reveal reproducible features in weak magnetic fields. These features are qualitatively explained by a quantum network model of these superconducting oxides. The ceramic superconductors are modeled as a set of one-dimensional wires weakly coupled at random nodes. The magnetoconductance, magnetization and susceptibility are computed from the network S-matrix.


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