Induced unconventional superconductivity on the surface states of Bi<sub>2</sub>Te<sub>3</sub> topological insulator.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 29222507.
- Also identified by DOI 10.1038/s41467-017-02069-z and PMC identifier 5722924.
- Licence recorded as CC BY.
- The licence permits redistribution, so the abstract is shown in full and the full text is available from the publisher.
Abstract
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 <sub>x</sub> + ip <sub>y</sub> wave term. Here we present phase-sensitive measurements, based on the quantum interference in nanoscale Josephson junctions, realized by using Bi<sub>2</sub>Te<sub>3</sub> topological insulator. We demonstrate that the induced superconductivity is unconventional and consistent with a sign-changing order parameter, such as a chiral p <sub>x</sub> + ip <sub>y</sub> 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<sub>2</sub>Te<sub>3</sub> flakes, and the dramatic role played by thermal strain are the surprising key factors for the display of an unconventional induced order parameter.