  Motivated by recent experiments with ultracold magnetic atoms trapped in
optical lattices where the orientation of atomic dipoles can be fully
controlled by external fields, we study the ground state properties of dipolar
bosons trapped in a two-dimensional lattice with density-induced hopping and
where the dipoles are tilted along the $xz$ plane. We present ground state
phase diagrams of the above system at different tilt angles. We find that, as
the dipolar interaction increases, the superfluid phase at half filling factor
is destroyed in favor of either a checkerboard or stripe solid phase for tilt
angle $\theta \lesssim 35.3^{\circ}$ or $\theta \gtrsim 35.3^{\circ}$
respectively. More interesting physics happens at tilt angles $\theta \gtrsim
58^{\circ}$, where we find that, as the dipolar interaction strength increases,
solid phases first appear at filling factor lower than $0.5$. Moreover, unlike
what observed at lower tilt angles, we find that, at half filling, a stripe
supersolid intervenes between the superfluid and stripe solid phase.
