Phase-locked magnetoconductance oscillations as a probe of Majorana edge states
arXiv:1301.4400 · doi:10.1103/PhysRevB.87.125406
Abstract
We calculate the Andreev conductance of a superconducting ring interrupted by a flux-biased Josephson junction, searching for electrical signatures of circulating edge states. Two-dimensional pair potentials of spin-singlet d-wave and spin-triplet p-wave symmetry support, respectively, (chiral) Dirac modes and (chiral or helical) Majorana modes. These produce h/e-periodic magnetoconductance oscillations of amplitude \simeq (e^{2}/h)N^{-1/2}, measured via an N-mode point contact at the inner or outer perimeter of the grounded ring. For Dirac modes the oscillations in the two contacts are independent, while for an unpaired Majorana mode they are phase locked by a topological phase transition at the Josephson junction.
arXiv comment10 pages, 6 figures. New appendix on the gauge invariant discretization of the Bogoliubov-De Gennes equation. Accepted for publication in PRB
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- Signatures of Majorana Fermions in Topological Insulator Josephson Junction Devices
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- Magnetic Flux Control of Chiral Majorana Edge Modes in Topological Superconductor
- Degeneracy of Majorana bound states and fractional Josephson effect in a dirty SNS junction
- Absence of Aharonov-Bohm effect of chiral Majorana fermion edge states
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- Protected gap closing in Josephson junctions constructed on BiTe surface
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