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dc.contributor.authorAbdel-Hafiez, M.-
dc.contributor.authorHarnagea, L.-
dc.contributor.authorSINGH, S.-
dc.contributor.authorStockert, U.-
dc.contributor.authorWurmehl, S.-
dc.contributor.authorLeps, N.-
dc.contributor.authorKlingeler, R.-
dc.contributor.authorWolter, A U.B.-
dc.contributor.authorBüchner, B.-
dc.coverage.spatialCambridgeen_US
dc.date.accessioned2022-06-10T12:06:57Z-
dc.date.available2022-06-10T12:06:57Z-
dc.date.issued2012-09-
dc.identifier.citationJournal of Physics: Conference Series, 391, 012120.en_US
dc.identifier.issn1742-6588-
dc.identifier.issn1742-6596-
dc.identifier.urihttps://iopscience.iop.org/article/10.1088/1742-6596/391/1/012120en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/7020-
dc.description.abstractWe present a calorimetric study on single crystals of Ca(Fe1−xCox)2As2 (x = 0, 0.032, 0.051, 0.056, 0.063, and 0.146). The combined first order spin-density wave/structural transition occurs in the parent CaFe2As2 compound at 168 K and gradually shifts to lower temperature for low doping levels (x = 0.032 and x = 0.051). It is completely suppressed upon higher doping x ≥ 0.056. Simultaneously, superconductivity appears at lower temperature with a transition temperature around Tc ~ 14.1 K for Ca(Fe0.937Co0.063)2As2. The phase diagram of Ca(Fe0.937Co0.063)2As2 has been derived and the upper critical field is found to be μ0H(c)2 = 11.5 T and μ0H(ab)c2 = 19.4 T for the c and ab directions, respectively.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectPhysicsen_US
dc.subject2012en_US
dc.titleCalorimetric study of the superconducting and normal state properties of Ca(Fe1−xCox)2As2en_US
dc.typeConference Papersen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.doihttps://doi.org/10.1088/1742-6596/391/1/012120en_US
dc.identifier.sourcetitleJournal of Physics: Conference Seriesen_US
dc.publication.originofpublisherForeignen_US
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