Soliton-induced Majorana fermions in a one-dimensional atomic topological superfluid

TL;DR

This paper predicts that dark solitons in a one-dimensional spin-orbit coupled Fermi gas can host Majorana fermions at the soliton nodes when tuned to a topological superfluid phase, offering a new way to realize and detect Majorana modes.

Contribution

It introduces the concept of soliton-induced Majorana fermions in a 1D atomic superfluid, combining soliton physics with topological quantum states.

Findings

Majorana fermions emerge at soliton nodes in the topological phase.

Zero-energy bound states localize near solitons as the system becomes topological.

Density profile minima at solitons disappear due to Majorana modes occupation.

Abstract

We theoretically investigate the behavior of dark solitons in a one-dimensional spin-orbit coupled atomic Fermi gas in harmonic traps, by solving self-consistently the Bogoliubov-de Gennes equations. The dark soliton - to be created by phase-imprinting in future experiments - is characterized by a real order parameter, which changes sign at a point node and hosts localized Andreev bound states near the node. By considering both cases of a single soliton and of multiple solitons, we find that the energy of these bound states decreases to zero, when the system is tuned to enter the topological superfluid phase by increasing an external Zeeman field. As a result, two Majorana fermions emerge in the vicinity of each soliton, in addition to the well-known Majorana fermions at the trap edges associated with the nontrivial topology of the superfluid. We propose that the soliton-induced Majorana fermions can be directly observed by using spatially-resolved radio-frequency spectroscopy or indirectly probed by measuring the density profile at the point node. For the latter, the deep minimum in the density profile will disappear due to the occupation of the soliton-induced zero-energy Majorana fermion modes. Our prediction could be tested in a resonantly-interacting spin-orbit coupled $^{40}$K Fermi gas confined in a two-dimensional optical lattice.