Abstract
We investigate theoretically non-magnetic impurity scattering in a one-dimensional atomic topological superfluid in harmonic traps, by solving self-consistently the microscopic Bogoliubov-de Gennes equation. In sharp contrast to topologically trivial Bardeen-Cooper-Schrieffer \textit{s}-wave superfluid, topological superfluid can host a mid-gap state that is bound to localized non-magnetic impurity. For strong impurity scattering, the bound state becomes universal, with nearly zero energy and a wave-function that closely follows the symmetry of that of Majorana fermions. We propose that the observation of such a universal bound state could be a useful evidence for characterizing the topolgoical nature of topological superfluids. Our prediction is applicable to an ultracold resonantly-interacting Fermi gas of K atoms with spin-orbit coupling confined in a two-dimensional optical lattice.
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