We study a system of bosonic dipoles that are polarized with all their dipole moments forming a certain angle with the plane containing their movement. As a first apprach, the superfluid properties of the different phases that appear in the phase diagram of this system were studied at zero temperature (T=0), showing that both for the gas and stripe phase can sustain a superfluid flow. Then, by performing Path Integral Monte Carlo simulations, we extend this study to finite temperature in order to determine the critical temperature $T_c$ at which the transition from superfluid to normal phase occurs. In two dimensional systems this transition is known to be driven by topological vortices that destroy the superfluid signal and follows the Berezinskii–Kosterlitz–Thouless (BKT) scaling. We show that, despite of the anisotropy present when dipoles are tilted, both the gas and the stripe phase follow the BKT scaling allowing us to extract the critical temperature across the phase diagram. We also evaluate the One-Body-Density-Matrix at different temperatures in the stripe phase to show the existence of a quasi-condensate below the critical temperature, which is characteristic of the BKT scenario.