  We propose a method to control the particle current of a one-dimensional
quantum system by resonating two many-body states through an external driving
field. We consider the Bose-Hubbard and spinless Fermi-Hubbard models with the
Peierls phase which induces net particle currents in the many-body eigenstates.
A driving field couples the ground state with one of the excited states having
large net currents, enabling us to control the system's current via Rabi
oscillation. Employing the Floquet analysis, we find that the resonate excited
states are determined by the symmetry of the driving field, which allows us to
selectively excite only certain states among the dense spectrum of a many-body
quantum system.
