Quantum charge fluctuations of a proximitized nanowire
arXiv:1606.06756 · doi:10.1103/PhysRevB.94.125407
Abstract
Motivated by recent experiment, we consider charging of a nanowire which is proximitized by a superconductor and connected to a normal-state lead by a single-channel junction. The charge of the nanowire is controlled by gate voltage . A finite conductance of the contact allows for quantum charge fluctuations, making the function continuous. It depends on the relation between the superconducting gap and the effective charging energy . The latter is determined by the junction conductance, in addition to the geometrical capacitance of the proximitized nanowire. We investigate at zero magnetic field , and at fields exceeding the critical value corresponding to the topological phase transition. Unlike the case of , the function is analytic even in the limit of negligible level spacing in the nanowire. At and , the maxima of are smeared by -fluctuations described by a single-channel "charge Kondo" physics, while the , case is described by a crossover between the Kondo and mixed-valence regimes of the Anderson impurity model. In the topological phase, is analytic function of the gate voltage with -periodic steps. In the weak tunneling limit, has peaks corresponding to Breit-Wigner resonances, whereas in the strong tunneling limit (i.e., small reflection amplitude ) these resonances are broadened, and .
11 pages, 5 figures
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- Suppressing quasiparticle poisoning with a voltage-controlled filter
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- Transport through a Majorana island: strong tunneling regime
- Coulomb Blockade in Fractional Topological Superconductors
- Signatures of topological ground state degeneracy in Majorana islands
- Strongly correlated electrons in superconducting islands with fluctuating Cooper pairs
- Majorana Conductances in Three-Terminal Transports
- Cross-correlation mediated by Majorana island with finite charging energy