On dispersive effect of the Coriolis force for the stationary Navier–Stokes equations

The dispersive effect of the Coriolis force for the stationary and non-stationary Navier–Stokes equations is investigated. Existence of a unique solution is shown for arbitrary large external force provided the Coriolis force is large enough. In addition to the stationary case, counterparts of several classical results for the non-stationary Navier–Stokes problem have been proven. The analysis is carried out in a new framework of the Fourier–Besov spaces.