-For the fermionic Hubbard model at strong coupling, we demonstrate that directional transport of localized doublons (repulsively bound pairs of two particles occupying the same site of the crystal lattice) can be achieved by applying an unbiased ac field of time-asymmetric (sawtooth-like) shape. The mechanism involves a transition to intermediate states of virtually zero double occupation which are reached by splitting the doublon by fields of the order of the Hubbard interaction. The process is discussed on the basis of numerically exact calculations for small clusters, and we apply it to more complex states to manipulate the charge order pattern of one-dimensional systems.To control and tune macroscopic properties by directly manipulating processes on the atomic scale is an ultimate goal in condensed matter physics. For example, one can selectively excite definite phonon modes [1] and thus create long-lived transients which exhibit interesting properties like superconductivity [2]. The design of suitable mechanisms that support such objectives requires to understand the underlying interplay of strong fields and many-particle interactions, which, nowadays, can be simulated and studied for more and more diverse situations by experiments with ultracold atoms [3][4][5]. The unprecedented control over the parameters in those systems allows one to explore the crossover between few and many-particle physics [6] and to probe or manipulate systems with single-site resolution [7]. This makes cold atoms well suited to analyze field-induced processes all the way from addressing single particles to complex many-particle states. In extended systems, the impact of an electric field on the correlated particle motion is already nontrivial at weak to moderate interactions (leading, e.g., to damping of Bloch oscillations [8,9] or nonlinear transport [10]). However, it becomes even more subtle if both the interactions and the field are comparable to or larger than the bandwidth. In this regime, fields can lead to the dielectric breakdown of a Mott insulator [11][12][13] (which is the many-body analog of the Zener breakdown in band insulators), and when the field and the interaction are resonant, the coupling of many degenerate states can lead to the emergence of phases which are described in terms of effective spin models [14][15][16].In this Letter, we investigate a controlled manipulation of few-particle states based on the interplay of the local repulsive interaction and the external field. We focus on the single-band Fermi-Hubbard model, which is the paradigm model for strongly correlated systems such as cold atoms in optical lattices or interacting electrons in a solid, and we develop a protocol by which an asymmetric alternating (ac) field is used to translate a repulsively bound "doublon" [17] along a chain in a directional motion, reminiscent of a (nondissipative) ratchet [18]. In the case of a single particle on a tight binding chain, an unbiased time-periodic driving cannot lead to a finite current or set an i...