Abstract

We consider a mesoscopic superconducting island hosting multiple pairs of Majorana zero-energy modes. The Majorana island consists of multiple p-wave wires connected together by a trivial (s-wave) superconducting backbone and is characterized by an overall charging energy $E_C$; the wires are coupled to normal-metal leads via tunnel junctions. We calculate the average charge on the island as well as non-local conductance matrix as a function of a p-wave pairing gap $\Delta_P$, charging energy $E_C$ and dimensionless junction conductances $g_i$. We find that the presence of a topological ground-state degeneracy in the island dramatically enhances charge fluctuations and leads to the suppression of Coulomb blockade effects. In contrast with conventional (s-wave) mesoscopic superconducting islands, we find that Coulomb blockade oscillations of conductance are suppressed in Majorana islands regardless of the ratio $E_C/\Delta_P$ or the magnitude of the conductances $g_i$. We also discuss our findings in relation to the so-called topological Kondo effect.

Highlights

  • The effect of quantum fluctuations in mesoscopic islands of superconducting metals has been extensively studied in the last two decades [1,2,3,4,5,6,7]

  • When such an island is coupled to normal leads, one can show that the topological ground-state degeneracy manifests itself in a number of different ways: The superconducting charge fluctuations are enhanced, suppressing Coulomb blockade effect; the conductance Gi j between leads i and j reaches a universal value Gi= j = 2e2/(Mh) at T = 0 independent of the applied gate voltage

  • We assume that L is much larger than the p-wave coherence length so we can ignore the hybridization of the Majorana states through the central segment

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Summary

INTRODUCTION

The effect of quantum fluctuations in mesoscopic islands of superconducting metals has been extensively studied in the last two decades [1,2,3,4,5,6,7]. Away from charge degeneracy points (known as the valley), tunneling of Cooper pairs across the superconducting island is suppressed at low temperatures T , i.e., G ∝ T 2 [10,11] This conclusion holds for any number of normal-metal (noninteracting) leads connected to the island. [26,27,28,29] that the remaining topological ground-state degeneracy can be used for quantum information processing When such an island is coupled to normal leads, one can show that the topological ground-state degeneracy manifests itself in a number of different ways: The superconducting charge fluctuations are enhanced, suppressing Coulomb blockade effect; the conductance Gi j between leads i and j reaches a universal value Gi= j = 2e2/(Mh) at T = 0 independent of the applied gate voltage.

QUALITATIVE DISCUSSION OF THE MAIN RESULTS
Average charge
Multiterminal conductance
THEORETICAL MODEL
STRONG SUPERCONDUCTOR LIMIT P EC
Weak tunneling limit Mg P EC
Coulomb valley
Charge degeneracy point
The strong-coupling limit
Strong tunneling limit Mg P EC
Weak tunneling limit Mg 1
Strong tunneling limit Mg 1
CHARGE AND CONDUCTANCE
Average charge in the strong superconductor limit P EC
Average charge in the weak superconductor limit P EC
Conductance in the strong superconductor limit P EC
Conductance in the weak superconductor limit P EC
ON THE RELATION TO THE MULTI-CHANNEL KONDO MODEL
VIII. CONCLUSIONS
The average
Weak tunneling limit
Strong tunneling limit
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