  We investigate the magnetism in tilted fermionic Mott insulators. With a
small tilt, the fermions are still localized and form a Mott-insulating state,
where the localized spins interact via antiferromagnetic exchange coupling.
While the localized state is naively expected to be broken with a large tilt,
in fact, the fermions are still localized under a large tilt due to the
Wannier-Stark localization and it can be regarded as a localized spin system.
We find that the sign of the exchange coupling is changed and the ferromagnetic
interaction is realized under the large tilt. To show this, we employ the
perturbation theory and the real-time numerical simulation with the fermionic
Hubbard chain. Our simulation exhibits that it is possible to effectively
control the speed and time direction of the dynamics by changing the size of
tilt, which may be useful for experimentally measuring the out-of-time ordered
correlators. Finally, we address the experimental platforms, such as ultracold
atoms in an optical lattice, to observe these phenomena.

Quantum Gases;Mesoscale and Nanoscale Physics;Strongly Correlated Electrons;Quantum Physics