Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/4403
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dc.contributor.authorVasdev, Aastha and-
dc.contributor.authorYadav, C.S.-
dc.contributor.authorKumar, Ritesh-
dc.contributor.authorHooda, M.K.-
dc.contributor.authorSheet, Goutam-
dc.date.accessioned2023-08-09T04:32:48Z-
dc.date.available2023-08-09T04:32:48Z-
dc.date.issued2022-
dc.identifier.citationSolid State Communications, 357(1), 114952.en_US
dc.identifier.urihttps://doi.org/10.1016/j.ssc.2022.114952-
dc.identifier.urihttp://hdl.handle.net/123456789/4403-
dc.descriptionOnly IISER Mohali authors are available in the record.en_US
dc.description.abstractA unique superconducting phase where type I and type II superconductivity coexist was seen below 1.7 K in the Dirac semimetal PdTe. The mixed superconducting phase was attributed to the local variation of the Ginzburg–Landau parameter() in PdTe. In such a scenario, it is imperative that introduction of disorder would make the system homogeneously type II. Here, we report our study of Point contact Andreev Reflection Spectroscopy on the 4% Cu intercalated PdTe single crystals. Cu-intercalates help enhance the critical temperature by donating carriers to the system, and at the same time act as scattering centres thereby reducing the effective . Our detailed magnetic field dependent point contact spectroscopy studies show a typical type-II behaviour in Cu-PdTe. A conventional BTK analysis of the spectra revealed a BCS-like gap = 330. With , Cu-PdTe falls in the strong coupling regime.en_US
dc.language.isoen_USen_US
dc.publisherElsevieren_US
dc.subjectReflectionen_US
dc.subjectEnhanceden_US
dc.subjectSuperconductingen_US
dc.subjectCu0.04PdTe2en_US
dc.titleAndreev reflection in the enhanced superconducting phase of Cu0.04PdTe2en_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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