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Induced unconventional superconductivity on the surface states of Bi(2)Te(3) topological insulator

Topological superconductivity is central to a variety of novel phenomena involving the interplay between topologically ordered phases and broken-symmetry states. The key ingredient is an unconventional order parameter, with an orbital component containing a chiral p (x) + ip (y) wave term. Here we p...

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Detalles Bibliográficos
Autores principales: Charpentier, Sophie, Galletti, Luca, Kunakova, Gunta, Arpaia, Riccardo, Song, Yuxin, Baghdadi, Reza, Wang, Shu Min, Kalaboukhov, Alexei, Olsson, Eva, Tafuri, Francesco, Golubev, Dmitry, Linder, Jacob, Bauch, Thilo, Lombardi, Floriana
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5722924/
https://www.ncbi.nlm.nih.gov/pubmed/29222507
http://dx.doi.org/10.1038/s41467-017-02069-z
Descripción
Sumario:Topological superconductivity is central to a variety of novel phenomena involving the interplay between topologically ordered phases and broken-symmetry states. The key ingredient is an unconventional order parameter, with an orbital component containing a chiral p (x) + ip (y) wave term. Here we present phase-sensitive measurements, based on the quantum interference in nanoscale Josephson junctions, realized by using Bi(2)Te(3) topological insulator. We demonstrate that the induced superconductivity is unconventional and consistent with a sign-changing order parameter, such as a chiral p (x) + ip (y) component. The magnetic field pattern of the junctions shows a dip at zero externally applied magnetic field, which is an incontrovertible signature of the simultaneous existence of 0 and π coupling within the junction, inherent to a non trivial order parameter phase. The nano-textured morphology of the Bi(2)Te(3) flakes, and the dramatic role played by thermal strain are the surprising key factors for the display of an unconventional induced order parameter.