  Using the time-dependent density matrix renormalization group method and
exact diagonalization, we study the non-equilibrium dynamics of the
one-dimensional Fermi-Hubbard model following a quantum quench or a ramp of the
onsite interaction strength. For quenches from the non-interacting to the
attractive regime, we investigate the dynamical emergence of
Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) correlations, which at finite spin
polarizations are the dominant two-body correlations in the ground state, and
their signatures in the pair quasi-momentum distribution function. We observe
that the post-quench double occupancy exhibits a maximum as the interaction
strength becomes of the order of the bandwidth. Finally, we study quenches and
ramps from attractive to repulsive interactions, which imprint FFLO
correlations onto repulsively bound pairs. We show that a quite short ramp time
is sufficient to wipe out the characteristic FFLO features in the post-quench
pair momentum distribution functions.
