Abstract

Majorana zero-modes bound to vortices in a topological superconductor have a non-Abelian exchange statistics expressed by a non-deterministic fusion rule: When two vortices merge they may or they may not produce an unpaired fermion with equal probability. Building on a recent proposal to inject edge vortices in a chiral mode by means of a Josephson junction, we show how the fusion rule manifests itself in an electrical measurement. A \bm {2\pi}2𝛑 phase shift at a pair of Josephson junctions creates a topological qubit in a state of even-even fermion parity, which is transformed by the chiral motion of the edge vortices into an equal-weight superposition of even-even and odd-odd fermion parity. Fusion of the edge vortices at a second pair of Josephson junctions results in a correlated charge transfer of zero or one electron per cycle, such that the current at each junction exhibits shot noise, but the difference of the currents is nearly noiseless.

Highlights

  • Vortices in a two-dimensional topological superconductor contain a midgap state, or zeromode, that can be used to store quantum mechanical information in a nonlocal way, protected from local sources of decoherence [1,2,3,4,5]

  • The Majorana fermion modes in the topological superconductor are not self-conjugate, instead creation and annihilation operators a†, a are related by the particle-hole symmetry relation (3.8)

  • We have shown how the method of time-resolved and “on-demand” injection of edge vortices proposed in Ref. 15 can be used to demonstrate the non-Abelian fusion rule of Majorana zeromodes

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Summary

Introduction

Vortices in a two-dimensional topological superconductor contain a midgap state, or zeromode, that can be used to store quantum mechanical information in a nonlocal way, protected from local sources of decoherence [1,2,3,4,5]. The fusion of two vortices σ produces a quantum superposition of states ψ and with and without a quasiparticle excitation This is the Majorana fusion rule of nonAbelian anyons, symbolically written as σ ⊗ σ = ψ ⊕. Neither the braiding nor the fusion of vortices has been realized in the laboratory This has motivated a variety of theoretical proposals for methods to demonstrate the appearance of nonAbelian anyons in a topological superconductor [10,11,12,13,14]. The obstacle that these proposals seek to remove, is the need to physically move the zero-modes around.

Edge vortex injection and fusion in a four-terminal Josephson junction
Construction of the fermion parity operator
Klich formula for particle-hole conjugate Majorana operators
Fermion parity as the determinant of a scattering matrix product
Simplification in the adiabatic regime
Vanishing of the average fermion parity
Frozen scattering matrix of the Josephson junction
Reduction of the fermion parity to a Toeplitz determinant
Fisher-Hartwig asymptotics
Average charge
Charge correlations
Conclusion
A Calculation of the frozen scattering matrix
B Derivation of the Klich formula
General expressions for first and second moments
Adiabatic approximation
Full Text
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