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Spin-resolved Andreev levels and parity crossings in hybrid superconductor-semiconductor nanostructures

2013/02/28 by Eduardo J. H. Lee, Xiaocheng Jiang, Manuel Houzet +3 · 1 citation
Physics and Astronomy · #cond-mat.mes-hall

paper · pdf · doi:10.1038/nnano.2013.267

published as Nature Nanotech., 9 (2014) 79-84 · 16 pages, 9 figures

arxiv created 2014/01/23 · arxiv updated 2014/01/24

Abstract

The hybrid combination of superconductors and low-dimensional semiconductors offers a versatile ground for novel device concepts, such as sources of spin-entangled electrons, nanoscale superconducting magnetometers, or recently proposed qubits based on topologically protected Majorana fermions. The underlying physics behind such hybrid devices ultimately rely on the magnetic properties of sub-gap excitations, known as Andreev levels. Here we report the Zeeman effect on the Andreev levels of a semiconductor nanowire quantum dot (QD) strongly coupled to a conventional superconductor. The combination of the large QD g-factor with the large superconductor critical magnetic field allows spin degeneracy to be lifted without suppressing superconductivity. We show that a Zeeman-split Andreev level crossing the Fermi energy signals a quantum phase transition in the ground state of the superconductivity-induced QD, denoting a change in the fermionic parity of the system. This transition manifests itself as a zero-bias conductance anomaly appearing at a finite magnetic field, with properties that resemble those expected for Majorana fermions in a topological superconductor. Although the herein reported zero-bias anomalies do not hold any relation with topological superconductivity, the observed parity transitions can be regarded as precursors of Majorana modes in the long-wire limit.

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