dc.contributor.author |
Vijayaraghavan, R
|
|
dc.contributor.author |
Michel, C
|
|
dc.contributor.author |
Maignan, A
|
|
dc.contributor.author |
Hervieu, M
|
|
dc.contributor.author |
Martin, C
|
|
dc.contributor.author |
Raveau, B
|
|
dc.contributor.author |
Rao, C N R
|
|
dc.date.accessioned |
2012-11-02T09:52:09Z |
|
dc.date.available |
2012-11-02T09:52:09Z |
|
dc.date.issued |
1993-02-10 |
|
dc.identifier |
0921-4534 |
en_US |
dc.identifier.citation |
Physica C 206(1-2), 81-89 (1993) |
en_US |
dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/902 |
|
dc.description |
Restricted Access |
en_US |
dc.description.abstract |
A systematic study of the Tl0.5Pb0.5Sr2Gd2−xCexCu2O9−δ system has revealed the existence of a pure phase in the compositional. range 0.0≤x≤0.6 crystalizzing in the 1222 structure. It has an intersheet distance of approximately 6 Å, a value much higher than those found in other cuprates with double CuO2 sheets interleaved by a single fluorite layer. Superconductivity has been observed in the range 0.1≤x≤0.4 with a Tc of 45 K and a superconductive volume fraction up to 20% for the optimal composition. An interesting variation of the superconducting properties of the above system with the composition, i.e. cerium content, has also been noticed. A possible dependence of superconductivity on the coupling between CuO2 sheets in the layered cuprates has been pointed out to bring out a correlation between structure and properties. |
en_US |
dc.description.uri |
http://dx.doi.org/10.1016/0921-4534(93)90704-T |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Elsevier Science BV |
en_US |
dc.rights |
© 1993 Elsevier Science BV |
en_US |
dc.subject |
Cu-O System |
en_US |
dc.subject |
Powder Diffraction |
en_US |
dc.subject |
Crystal-Structure |
en_US |
dc.subject |
Copper-Oxide |
en_US |
dc.subject |
Cuprate |
en_US |
dc.subject |
Superconductivity |
en_US |
dc.title |
Structure and properties of Tl0.5Pb0.5Sr2Gd2−xCexCu2O9−δ |
en_US |
dc.type |
Article |
en_US |