The rectification of noise into directed movement or useful energy is utilized by many different systems. The peculiar nature of the energy source and conceptual differences between such Brownian motor systems makes a characterization of the performance far from straightforward. In this work, where the Brownian motor consists of atoms interacting with dissipative optical lattices, we adopt existing theory and present experimental measurements for both the efficiency and the transport coherence. We achieve up to 0.3% for the efficiency and 0.01 for the Péclet number.PACS numbers: 05.60.Cd, 37.10.Jk Brownian motors (BMs) are devices that can rectify noise into work or directed motion in the absence of external forces. They are of interest for the understanding of fundamental principles in statistical physics and thermodynamics, and several studies have shown that they play a crucial part in transport phenomena in nature; see, for example, [1][2][3]. Since BM's utilize noise, they can work in regions where the inherent noise is large compared to other interactions. Applications of BM's, therefore, reach into the nano-scales, where they make ideal tools for powering up nano-machines [4][5][6]. Recent reviews of the subject can be found in [7][8][9][10].Of particular interest for any motor is the quantification of its efficiency, usually defined as the ratio of produced work to input energy. Due to the peculiar nature of the energy source of BMs, determination of efficiency is not straightforward. There have been several theoretical discussions on the efficiency of BM's [11][12][13][14][15], and different performance characteristics have been discussed in [16]. We present here experimental measurements of two performance characteristics of a BM realized with ultracold atoms in double optical lattices [17]: the efficiency, that is, the fraction of input power driving the directed motion, and the transport coherence, or the Péclet number, that is, the comparison between the drift and the diffusion. Usually, the efficiency is defined in terms of the amount of work obtained from the motor against a load. As no load is present in our case, we instead follow the convention [11,12] of defining "useful energy" as the energy needed to drive the directed motion of the atoms against friction. It has also been argued that including the dissipation due to friction against the directed motion provides a better definition of efficiency even when a load is present [11].For a BM to be able to function, it has to (i) present an asymmetry [18] and (ii) be out of thermal equilibrium [19]. In most cases, the symmetry breaking arises * martin.zelan@physics.umu.se either from a time-asymmetric periodic driving force with zero average (rocked ratchet), or by flashing an asymmetric potential (flashed ratchet). However, as shown in our system [17], rectification can be achieved by switching between two symmetric potentials.The model for the BM used in our experiment was introduced in [20]. Briefly, particles with mass m move in two symmet...