Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2514
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dc.contributor.authorAmit-
dc.contributor.authorSingh, Yogesh-
dc.date.accessioned2020-12-02T09:46:52Z-
dc.date.available2020-12-02T09:46:52Z-
dc.date.issued2016-
dc.identifier.citationJournal of Superconductivity and Novel Magnetism,29(8), pp.1975-1979.en_US
dc.identifier.other10.1007/s10948-016-3499-x-
dc.identifier.urihttps://link.springer.com/article/10.1007/s10948-016-3499-x-
dc.identifier.urihttp://hdl.handle.net/123456789/2514-
dc.description.abstractWe study the magnetic field vs. temperature (H – T) and pressure vs. temperature (P – T) phase diagrams of the T c ≈ 5.5 K superconducting phase in Pd x Bi2Te3 (x ≈ 1) using electrical resistivity versus temperature measurements at various applied magnetic fields (H) and magnetic susceptibility versus temperature measurements at various applied magnetic fields (H) and pressure (P). The H – T phase diagram has an initial upward curvature as observed in some unconventional superconductors. The critical field extrapolated to T = 0 K is H c (0) ≈ 6–10 kOe. The T c is suppressed approximately linearly with pressure at a rate d T c /d P ≈ −0.28 K/GPa.en_US
dc.language.isoenen_US
dc.publisherSpringer Linken_US
dc.subjectTopological statesen_US
dc.subjectIntense researchen_US
dc.subjectShort spanen_US
dc.titleThe H-T and P-T Phase Diagram of the Superconducting Phase in Pd:Bi2Te3en_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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