Majorana modes in multiband superconducting quantum wires
arXiv:2001.08123 · doi:10.1103/PhysRevB.101.094502
Abstract
We calculate analytically the spectrum of the Andreev bound states in a half-infinite superconducting wire with an arbitrary number of bands crossing the chemical potential. The normal state of the wire is assumed to have an antiunitary symmetry A (time reversal or its combination with a crystallographic point group operation), with A^2=-1 or +1. This symmetry may be broken by the superconducting order parameter and/or the boundary scattering. We present a model-independent proof of the existence of one Majorana mode near the end of the wire with an odd number of bands.
9 pages, 2 figures
References in corpus (8)
- Signatures of Majorana fermions in hybrid superconductor-semiconductor nanowire devices
- Majorana Fermions and a Topological Phase Transition in Semiconductor-Superconductor Heterostructures
- Introduction to topological superconductivity and Majorana fermions
- Topology of crystalline insulators and superconductors
- Multichannel Generalization of Kitaev's Majorana End States and a Practical Route to Realize Them in Thin Films
- Search for Majorana fermions in multiband semiconducting nanowires
- Noncentrosymmetric superconductors in one dimension
- Superconductivity in quantum wires: A symmetry analysis
Cited by in corpus (5)
- Topology of critical chiral phases: multiband insulators and superconductors
- Edge states, Majorana fermions and topological order in superconducting wires with generalized boundary conditions
- Resilience of topological superconductivity under particle current
- A topological flux trap: Majorana bound states at screw dislocations
- Ever-present Majorana bound state in a generic one-dimensional superconductor with odd number of Fermi surfaces