| 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 |