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 Field	Value	Language
dc.contributor.author	Nagarajan, R	-
dc.contributor.author	Vasanthacharya, N Y	-
dc.contributor.author	Gopalakrishnan, J	-
dc.contributor.author	Rao, C N R	-
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
Appears in Collections:	Research Papers (Prof. C.N.R. Rao)

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