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Please use this identifier to cite or link to this item: https://ir.swu.ac.th/jspui/handle/123456789/14667
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dc.contributor.authorUdomsamuthirun P.
dc.contributor.authorKruaehong T.
dc.contributor.authorNilkamjon T.
dc.contributor.authorRatreng S.
dc.date.accessioned2021-04-05T03:36:20Z-
dc.date.available2021-04-05T03:36:20Z-
dc.date.issued2010
dc.identifier.issn15571939
dc.identifier.other2-s2.0-78649634709
dc.identifier.urihttps://ir.swu.ac.th/jspui/handle/123456789/14667-
dc.identifier.urihttps://www.scopus.com/inward/record.uri?eid=2-s2.0-78649634709&doi=10.1007%2fs10948-010-0786-9&partnerID=40&md5=5da534da49ca4d173fc710269f3717dd
dc.description.abstractThe new YBaCuO superconductors are synthesized by using the standard solid-state reaction method as compositions of Y5-6-11, Y7-9-16,Y358, Y5-8-13, Y7-11-18, Y156, Y3-8-11, and Y13-20-23, where the numbers indicate Y, Ba, and Cu atoms respectively; all show the Meissner effect at 77 K. The resistivity measurements used by the four-probe method have shown the highest T c onset is 94 K. The XRD spectra are shown and they have a similar crystalline structure as Y123 and Y358 materials with some impurities peaks. © 2010 Springer Science+Business Media, LLC.
dc.subjectCrystalline structure
dc.subjectCu atoms
dc.subjectFour-probe methods
dc.subjectMeissner effect
dc.subjectNew superconductor
dc.subjectResistivity measurement
dc.subjectSolid state reaction method
dc.subjectXRD spectra
dc.subjectYBaCuO superconductors
dc.subjectBarium
dc.subjectImpurities
dc.subjectSolid state reactions
dc.subjectSuperconducting materials
dc.subjectSuperconductivity
dc.titleThe new superconductors of YBaCuO materials
dc.typeArticle
dc.rights.holderScopus
dc.identifier.bibliograpycitationJournal of Superconductivity and Novel Magnetism. Vol 23, No.7 (2010), p.1377-1380
dc.identifier.doi10.1007/s10948-010-0786-9
Appears in Collections:Scopus 1983-2021

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