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Pseudogap and proximity effect in the Bi(2)Te(3)/Fe(1+y)Te interfacial superconductor
In the interfacial superconductor Bi(2)Te(3)/Fe(1+y)Te, two dimensional superconductivity occurs in direct vicinity to the surface state of a topological insulator. If this state were to become involved in superconductivity, under certain conditions a topological superconducting state could be forme...
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/PMC5009436/ https://www.ncbi.nlm.nih.gov/pubmed/27587000 http://dx.doi.org/10.1038/srep32508 |
Sumario: | In the interfacial superconductor Bi(2)Te(3)/Fe(1+y)Te, two dimensional superconductivity occurs in direct vicinity to the surface state of a topological insulator. If this state were to become involved in superconductivity, under certain conditions a topological superconducting state could be formed, which is of high interest due to the possibility of creating Majorana fermionic states. We report directional point-contact spectroscopy data on the novel Bi(2)Te(3)/Fe(1+y)Te interfacial superconductor for a Bi(2)Te(3) thickness of 9 quintuple layers, bonded by van der Waals epitaxy to a Fe(1+y)Te film at an atomically sharp interface. Our data show highly unconventional superconductivity, which appears as complex as in the cuprate high temperature superconductors. A very large superconducting twin-gap structure is replaced by a pseudogap above ~12 K which persists up to 40 K. While the larger gap shows unconventional order parameter symmetry and is attributed to a thin FeTe layer in proximity to the interface, the smaller gap is associated with superconductivity induced via the proximity effect in the topological insulator Bi(2)Te(3). |
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