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dc.contributor.authorI. M. Tangen_US
dc.contributor.authorS. Leelapruteen_US
dc.contributor.authorC. Soankwanen_US
dc.contributor.authorN. Chiengpratoomen_US
dc.contributor.otherMahidol Universityen_US
dc.date.accessioned2018-08-10T08:36:54Z-
dc.date.available2018-08-10T08:36:54Z-
dc.date.issued1991-04-15en_US
dc.identifier.citationPhysica C: Superconductivity and its applications. Vol.175, No.3-4 (1991), 250-254en_US
dc.identifier.issn09214534en_US
dc.identifier.other2-s2.0-0026136640en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=0026136640&origin=inwarden_US
dc.identifier.urihttp://repository.li.mahidol.ac.th/dspace/handle/123456789/22232-
dc.description.abstractThe effects of lanthanide rare earth (RE) substitution into two layer bismuth superconductors are studied. Quenching the RE substituted superconductors, Bi1.55Pb0.45Sr2RE0.2Ca0.8Cu2Oz, is used to lower the hole concentration to the levels where above 90 K superconductivity can be achieved. Lead substitution is used to facilitate the growth of single phase specimens. Variation in the values of Tcfor the various RE substituted superconductors is seen to be governed mainly by the value of the hole concentration in each of the superconductors. © 1991.en_US
dc.rightsMahidol Universityen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=0026136640&origin=inwarden_US
dc.subjectPhysics and Astronomyen_US
dc.titleLanthanide substitution into low hole concentration bismuth superconductorsen_US
dc.typeArticleen_US
dc.rights.holderSCOPUSen_US
dc.identifier.doi10.1016/0921-4534(91)90594-Oen_US
Appears in Collections:Scopus 1991-2000

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