dc.contributor.author |
Naik, M.S. |
|
dc.contributor.author |
Sarode, P.R. |
|
dc.contributor.author |
Prabhu, R.B. |
|
dc.contributor.author |
Priolkar, K.R. |
|
dc.contributor.author |
Vasanthacharya, N.Y. |
|
dc.date.accessioned |
2015-06-03T10:18:33Z |
|
dc.date.available |
2015-06-03T10:18:33Z |
|
dc.date.issued |
2009 |
|
dc.identifier.citation |
Acta Physica Polonica A. 115(3); 2009; 742-744. |
en_US |
dc.identifier.uri |
http://przyrbwn.icm.edu.pl/APP/PDF/115/a115z326.pdf |
|
dc.identifier.uri |
http://irgu.unigoa.ac.in/drs/handle/unigoa/2363 |
|
dc.description.abstract |
In this paper we present the resistivity data for Pr and Zn codoped compound Y(1-x)Pr(x)Ba(2) [Cu(1-y)Zn(y)](3)O(7-delta) with 0 less than y less than 0:1 and x = 0.0, 0.1 and 0.2. The data is analysed in terms of the superconducting critical temperature T(c), residual resistivity po. and the resistivity slope dp/dT corresponding to the linear p-T region. It is found that for x = 0:1 Pr has a minimal influence on the in-plane processes for Zn impurity alone affecting slightly Tc and p0. The slope dp/dT becomes larger for 0.03 less than y less than 0.06 leading to larger depining effect and hence slower fall of T(c) as a function of y. For x = 0.2 there is a drastic change, p0 becomes abnormally large, dp/dT becomes negative implying absence of depinning and a totally pinned charge stripes. Superconductivity vanishes at y = 0.03. It is concluded that for x = 0.2 Pr converts the system from overdoped to underdoped region leading to the universal superconductor-insulator transition. |
en_US |
dc.publisher |
Polish Academy of Sciences |
en_US |
dc.subject |
Physics |
en_US |
dc.title |
Codoping effect of Zn and Pr in YBa(2)Cu(3)O(7-delta) |
en_US |
dc.type |
Journal article |
en_US |
dc.identifier.impf |
y |
|