Quantum Brownian motion in ratchet potentials is investigated by means of an approach based on a duality relation. This relation links the long-time dynamics in a tilted ratchet potential in the presence of dissipation with the one in a driven dissipative tight-binding model. The application to quantum ratchets yields a simple expression for the ratchet current in terms of the transition rates in the tight-binding system.Keywords: Quantum dissipative systems; Quantum ratchets; Path inegrals methods Brownian motion in ratchet potentials [1] has attracted a lot of interest. One reason is the fact that ratchet systems, i.e. periodic structures with broken spatial symmetry, present the property of allowing transport under the influence of unbiased forces. The interest has recently grown with the transfer of the problem in the quantum regime. There, the description of dissipative tunneling [2] presents a theoretical challenge which was tackled in relatively few works [3,4,5,6,7,8], while first experimental realizations were reported [9,10]. After the semiclassical work [3], further progress towards the theoretical description of quantum ratchets involved modeling in terms of tight-binding systems [4,5] or in terms of a molecular wire [6]. Other available methods include perturbation theory [7] or a quantum Smoluchowski equation [8]. Most of these methods [3,4,5,8] are restricted to the regime of moderate-tostrong friction.The approach discussed in this article originates from works [11,12,13,14,15] on quantum Brownian motion in a tilted sinusoidal potential, which led to a duality relation for the mobility of the system considered with the one of a driven dissipative tight-binding model. This idea emerged first in Ref. [11], where the linear dc mobility at zero temperature was considered. In that work the interest was focused on the occurrence of a diffusion-to-localization transition in the system with increasing dissipation. These results were corroborated by means of renormalizationgroup methods [12]. The duality relation was extended to the nonlinear dc mobility at finite temperatures in Ref. [13], where an extensive physical discussion as well as important milestones of the proof were given. It was subsequently applied to the investigation of the current-voltage characteristic of small Josephson junctions [14]. Later, an identical duality relation for the linear ac mobility was obtained by a different approach in the frame of linear response [15]. In particular, that work went beyond the case of a strictly Ohmic dissipative bath considered in Ref. [13], and included the case of an Ohmic bath with finite cutoff frequency as well as sub and super-Ohmic baths. In Ref.[16], the formalism of Ref.[13] was generalized to arbitrary ratchet potentials, i.e., periodic potentials of arbitrary shape. Moreover, the duality relation was extended to the average position of the quantum particle at long time. In the present article, we give detailed proofs and discussion of these last results. The duality relation is obtained i...