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Interrogating the superconductor Ca(10)(Pt(4)As(8))(Fe(2−x)Pt(x)As(2))(5) Layer-by-layer
Ever since the discovery of high-T(c) superconductivity in layered cuprates, the roles that individual layers play have been debated, due to difficulty in layer-by-layer characterization. While there is similar challenge in many Fe-based layered superconductors, the newly-discovered Ca(10)(Pt(4)As(8...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5064410/ https://www.ncbi.nlm.nih.gov/pubmed/27739517 http://dx.doi.org/10.1038/srep35365 |
Sumario: | Ever since the discovery of high-T(c) superconductivity in layered cuprates, the roles that individual layers play have been debated, due to difficulty in layer-by-layer characterization. While there is similar challenge in many Fe-based layered superconductors, the newly-discovered Ca(10)(Pt(4)As(8))(Fe(2)As(2))(5) provides opportunities to explore superconductivity layer by layer, because it contains both superconducting building blocks (Fe(2)As(2) layers) and intermediate Pt(4)As(8) layers. Cleaving a single crystal under ultra-high vacuum results in multiple terminations: an ordered Pt(4)As(8) layer, two reconstructed Ca layers on the top of a Pt(4)As(8) layer, and disordered Ca layer on the top of Fe(2)As(2) layer. The electronic properties of individual layers are studied using scanning tunneling microscopy/spectroscopy (STM/S), which reveals different spectra for each surface. Remarkably superconducting coherence peaks are seen only on the ordered Ca/Pt(4)As(8) layer. Our results indicate that an ordered structure with proper charge balance is required in order to preserve superconductivity. |
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