## (a) Spectrum of Bogoliubov excitations (red dots) for a harmonically trapped system, calculated for *J*_{z} = 1.5 δ, *J* = 2 Δ^{(2)}, ω = 2π **×** 200 Hz

_{z}

#### figure

Figures are generally photos, graphs and static images that would be represented in traditional pdf publications.

**Figure 5.** (a) Spectrum of Bogoliubov excitations (red dots) for a harmonically trapped system, calculated for *J _{z}* = 1.5 δ,

*J*= 2 Δ

^{(2)}, ω = 2π

**×**200 Hz. It exhibits a bulk gap Δ

_{bulk}= 0.22

*E*and a pair of zero-energy Majorana states with a residual splitting Δ

_{r}_{s}~ 10

^{−10}

*E*. (b) Evolution of the energy splitting Δ

_{r}_{s}between Majorana states (red dots) and of the bulk gap Δ

_{bulk}(orange dots) as a function of the trapping frequency ω. While the bulk gap essentially does not depend on ω, the splitting between Majorana states strongly decreases when decreasing the ω value, i.e. increasing the separation between Majorana fermions. (c) Density distribution along

*x*of a zero-energy Majorana state, in planes

*A*(red line) and

*B*(blue line). (d) Total density distribution along

*x*calculated at zero temperature.

**Abstract**

We propose an experimental implementation of a topological superfluid with ultracold fermionic atoms. An optical superlattice is used to juxtapose a 1D gas of fermionic atoms and a 2D conventional superfluid of condensed Feshbach molecules. The latter acts as a Cooper pair reservoir and effectively induces a superfluid gap in the 1D system. Combined with a spin-dependent optical lattice along the 1D tube and laser-induced atom tunnelling, we obtain a topological superfluid phase. In the regime of weak couplings to the molecular field and for a uniform gas, the atomic system is equivalent to Kitaev's model of a p-wave superfluid. Using a numerical calculation, we show that the topological superfluidity is robust beyond the perturbative limit and in the presence of a harmonic trap. Finally, we describe how to investigate some physical properties of the Majorana fermions located at the topological superfluid boundaries. In particular, we discuss how to prepare and detect a given Majorana edge state.