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Lead substitution in the bismuth superconductors (Bi,Pb)<inf>4</inf>Sr<inf>4</inf>Ca<inf>2</inf>Cu<inf>4</inf>O<inf>y</inf>and (Bi,Pb)<inf>4</inf>Sr<inf>3</inf>Ca<inf>3</inf>Cu<inf>4</inf>O<inf>y</inf>

dc.contributor.authorI. M. Tangen_US
dc.contributor.authorP. Jirapisasiuken_US
dc.contributor.authorN. Chiengpratoomen_US
dc.contributor.authorK. Eaiprasertsaken_US
dc.contributor.otherMahidol Universityen_US
dc.contributor.otherThammasat Universityen_US
dc.date.accessioned2018-06-14T09:27:07Z
dc.date.available2018-06-14T09:27:07Z
dc.date.issued1990-10-01en_US
dc.description.abstractX-ray diffraction patterns and resistivity measurement of the Bi 4-x Pb x Sr 3 Ca 3 Cu 4 O y (x=0.7, 1.0, 1.1 and 1. 2) superconductors and the Bi 4-x Pb x Sr 4 Ca 2 Cu 4 O y (x=0.7, 0.9, 1.1 and 1.2) superconductors show that there are differences in the way the two superconductors respond to the Pb doping. The Pb doping is seen to promote the growth of the "2223" phase more in the "4334" systems than in the "4424" systems and to affect the zero-resistivity temperatures of the superconductors in different ways. © 1990.en_US
dc.identifier.citationPhysics Letters A. Vol.149, No.5-6 (1990), 311-314en_US
dc.identifier.doi10.1016/0375-9601(90)90437-Sen_US
dc.identifier.issn03759601en_US
dc.identifier.other2-s2.0-44949291013en_US
dc.identifier.urihttps://repository.li.mahidol.ac.th/handle/20.500.14594/16172
dc.rightsMahidol Universityen_US
dc.rights.holderSCOPUSen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=44949291013&origin=inwarden_US
dc.subjectPhysics and Astronomyen_US
dc.titleLead substitution in the bismuth superconductors (Bi,Pb)<inf>4</inf>Sr<inf>4</inf>Ca<inf>2</inf>Cu<inf>4</inf>O<inf>y</inf>and (Bi,Pb)<inf>4</inf>Sr<inf>3</inf>Ca<inf>3</inf>Cu<inf>4</inf>O<inf>y</inf>en_US
dc.typeArticleen_US
dspace.entity.typePublication
mu.datasource.scopushttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=44949291013&origin=inwarden_US

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