Extended Data Fig. 3: Vortex nucleation in a dipolar BEC and supersolid for different parameters.

Vortex nucleation in a dipolar BEC (a) and in a supersolid (b) for different atom number and different scattering length as. c, Vortex nucleation for initial noise with different temperatures. All of the results are obtained from eGPE calculations with (ω⊥, ωz) = 2π × [50, 103] Hz, magnetic-field angle from the z axis θ = 30° and three-body recombination losses are included.