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Two-dimensional topological superconductivity in Pb/Co/Si(111)

Gerbold C. Ménard, Sébastien Guissart, Christophe Brun, Raphaël T. Leriche, Mircea Trif, François Debontridder, Dominique Demaille, Dimitri Roditchev, Pascal Simon () and Tristan Cren ()
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Gerbold C. Ménard: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588
Sébastien Guissart: Université Paris-Saclay
Christophe Brun: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588
Raphaël T. Leriche: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588
Mircea Trif: Université Paris-Saclay
François Debontridder: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588
Dominique Demaille: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588
Dimitri Roditchev: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588
Pascal Simon: Université Paris-Saclay
Tristan Cren: Université Pierre et Marie Curie (UPMC) CNRS-UMR 7588

Nature Communications, 2017, vol. 8, issue 1, 1-7

Abstract: Abstract Just like insulators can present topological phases characterized by Dirac edge states, superconductors can exhibit topological phases characterized by Majorana edge states. In particular, one-dimensional topological superconductors are predicted to host zero-energy Majorana fermions at their extremities. By contrast, two-dimensional superconductors have a one-dimensional boundary which would naturally lead to propagating Majorana edge states characterized by a Dirac-like dispersion. In this paper we present evidences of one-dimensional dispersive in-gap edge states surrounding a two-dimensional topological superconducting domain consisting of a monolayer of Pb covering magnetic Co–Si islands grown on Si(111). We interpret the measured dispersive in-gap states as a spatial topological transition with a gap closure. Our method could in principle be generalized to a large variety of heterostructures combining a Rashba superconductor with a magnetic layer in order to be used as a platform for engineering topological quantum phases.

Date: 2017
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DOI: 10.1038/s41467-017-02192-x

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