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Superconducting (1:1:2:2)-type layered cuprates of the formula TlCA1-xLxSr2Cu2Oy (L=Y or rare-earth element)
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| dc.contributor.author | Rao, C N R
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| dc.contributor.author | Ganguli, A K
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| dc.contributor.author | Vijayaraghavan, R
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| dc.date.accessioned | 2012-08-30T11:15:26Z | |
| dc.date.available | 2012-08-30T11:15:26Z | |
| dc.date.issued | 1989-08-01 | |
| dc.identifier | 0163-1829 | en_US |
| dc.identifier.citation | Physical Review B 40(4), 2565-2567 (1989) | en_US |
| dc.identifier.uri | https://libjncir.jncasr.ac.in/xmlui/10572/786 | |
| dc.description | Restricted Access | en_US |
| dc.description.abstract | The TlCa1-xLxSr2Cu2Oy (L=Y or a rare earth element) series of cuprates possessing a (1:1:2:2)-type layered structure exhibit superconductivity in the 60–90-K region. The TlCa1-xLxSr2Cu2Oy (x=1) series of cuprates also possess the (1:1:2:2)-type structure, but are not superconducting. A change in the conduction mechanism seems to occur in the TlCa1-xLxSr2Cu2Oy system with a change in x. Partial substitution of Tl by Pb does not favor superconductivity in this series of cuprates. | en_US |
| dc.description.uri | http://dx.doi.org/10.1103/PhysRevB.40.2565 | en_US |
| dc.language.iso | en | en_US |
| dc.publisher | American Physical Society | en_US |
| dc.rights | © 1989 The American Physical Society | en_US |
| dc.subject | Superconducting (1:1:2:2)-type layered cuprates | en_US |
| dc.subject | TlCA1-xLxSr2Cu2Oy | en_US |
| dc.subject | L=Y or rare-earth element | en_US |
| dc.title | Superconducting (1:1:2:2)-type layered cuprates of the formula TlCA1-xLxSr2Cu2Oy (L=Y or rare-earth element) | en_US |
| dc.type | Article | en_US |
