dc.contributor.author |
Nagarajan, R
|
|
dc.contributor.author |
Vijayaraghavan, R
|
|
dc.contributor.author |
Ganapathi, L
|
|
dc.contributor.author |
Ram, Ram
|
|
dc.contributor.author |
Rao, C N R
|
|
dc.date.accessioned |
2012-12-07T04:57:47Z |
|
dc.date.available |
2012-12-07T04:57:47Z |
|
dc.date.issued |
1989-05-01 |
|
dc.identifier |
0921-4534 |
en_US |
dc.identifier.citation |
Physica C 158(3), 453-457 (1989) |
en_US |
dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/1234 |
|
dc.description |
Restricted Access |
en_US |
dc.description.abstract |
Superconductivity in LnBa2Cu3O7 − δ with Ln = Nd, Eu, Gdand Dy has been investigated as a function of δ, closely following the accompanying changes in crystal structure. Orthorhombic GdBa2Cu3O7 − δ and DyBa2Cu3O7 − δ show a Tc of ≈ 90 K up to δ = 0.2 and a lower Tc plateau (40–50 K) in the δ range 02 to 0.4, similar to that found in YBa2Cu3O7 − δ. The orthorhombic structure II in the lower Tc regions is different from the structure I in the 90 K Tc (low δ) region. The unit cell parameters of the orthorhombic I structure in the high Tc region bear the relationship of a a ≠ b not, vert, similar c/3. This relationship is not seen in the low Tc plateau. The low Tc plateau region does not distinctly manifest itself in NdBa2Cu3O7 − δ just as in LaBa2Cu3O7 − δ. |
en_US |
dc.description.uri |
http://dx.doi.org/10.1016/0921-4534(89)90243-8 |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Elsevier Science BV |
en_US |
dc.rights |
© 1989 Elsevier Science Publishers BV |
en_US |
dc.subject |
oxygen stoichiometry |
en_US |
dc.subject |
Superconductivity |
en_US |
dc.subject |
Orthorhombic structure |
en_US |
dc.title |
Evidence for two distinct orthorhombic structures associated with different Tc regimes in LnBa2Cu3O7 − δ (Ln = Nd, Eu, Gd and Dy): A study of the dependence of superconductivity on oxygen stoichiometry |
en_US |
dc.type |
Article |
en_US |