Some results are known for the Fermi-Hubbard model under certain assumptions. For instance, it is known that at half-filling and in the strong coupling limit, the Hubbard model reduces to a Heisenberg antiferromagnet. For reference, the Hubbard model is: \begin{equation} H = -t\sum_{\langle ij \rangle\sigma}c^\dagger_{i\sigma}c_{j\sigma}+U\sum_i n_{i\uparrow}n_{i\downarrow} \end{equation}
I'm wondering: is it possible to make general remarks on how the ground state of the system behaves by increasing the on-site interaction $U$? What I'm looking for is some basic predictions on, say, how the densities on a given lattice might evolve if $U/t$ gets higher regardless of the filling or the specific lattice.
In general, $U$ favours having a non-zero spin on each site and thus one might expect that for any lattice and any filling a sort of antiferromagnetic configuration emerges as the ground state at high $U$. Is it fair to say so? Can we say anything else? I hope the question isn't too generic.