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Superconductivity in Ba(Pb,Bi,Sb)O3, Ba(Pb,Bi,Te)O3 and (Ba,La) (Pb,Bi,Tl)O3 systems
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| dc.contributor.author | Nagarajan, R
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| dc.contributor.author | Vasanthacharya, N Y
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| dc.contributor.author | Gopalakrishnan, J
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| dc.contributor.author | Rao, C N R
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| dc.date.accessioned | 2012-11-06T07:05:21Z | |
| dc.date.available | 2012-11-06T07:05:21Z | |
| dc.date.issued | 1991-02 | |
| dc.identifier | 0038-1098 | en_US |
| dc.identifier.citation | Solid State Communications 77(5), 373-376 (1991) | en_US |
| dc.identifier.uri | https://libjncir.jncasr.ac.in/xmlui/10572/916 | |
| dc.description | Restricted Access | en_US |
| dc.description.abstract | It is possible to substitute Bi in the superconducting BaPb0.75Bi0.25O3 by Sb or Te without destroying the superconductivity. With Sb, a continuous series of solid solutions BaPb0.75Bi0.25−ySbyO3 (0 ≤ y ≤ 0.25) exists, while with Te, perovskite BaPb0.75Bi0.25−yTeyO3 exists only upto y = 0.15. With increasing substitution by Sb or Te, Tc decreases continously in both the systems. Superconductivity with a maximum Tc of 8K is found in Ba0.9La0.1Pb0.9−yBiyTl0.1O3 for y = 0.25. | en_US |
| dc.description.uri | http://dx.doi.org/10.1016/0038-1098(91)90753-I | en_US |
| dc.language.iso | en | en_US |
| dc.publisher | Pergamon-Elsevier Science Ltd | en_US |
| dc.rights | © 1991 Elsevier Science BV | en_US |
| dc.subject | Temperature | en_US |
| dc.title | Superconductivity in Ba(Pb,Bi,Sb)O3, Ba(Pb,Bi,Te)O3 and (Ba,La) (Pb,Bi,Tl)O3 systems | en_US |
| dc.type | Article | en_US |
