We observe the myosin V stepping mechanism by traveling wave tracking. This technique, associated with optical tweezers, allows one to follow a scattering particle in a two-dimensional plane, with nanometer accuracy and a temporal resolution in the microsecond range. We have observed that, at the millisecond time scale, the myosin V combines longitudinal and vertical motions during the step. Because at this time scale the steps appear heterogeneous, we deduce their general features by aligning and averaging a large number of them. Our data show that the 36-nm step occurs in three main stages. First, the myosin center of mass moves forward 5 nm; the duration of this short prestep depends on the ATP concentration. Second, the motor performs a fast motion over 23 nm; this motion is associated to a vertical movement of the myosin center of mass, whose distance from the actin filament increases by 6 nm. Third, the myosin head freely diffuses toward the next binding site and the vertical position is recovered. We propose a simple model to describe the step mechanism of the dimeric myosin V. molecular motor ͉ single molecule ͉ traveling wave tracking ͉ total internal reflection ͉ interference M olecular motors convert the chemical energy, obtained from ATP hydrolysis, into mechanical work in a very efficient way. Understanding this active system, which is constantly driven away from the thermodynamics equilibrium, has been a challenge for physicists, biologists, and chemists. Nowadays, the genetic approach, together with an increasing amount of structural information (1, 2) and single-molecule studies (3-10), has supplied a detailed description of molecular motor dynamics. To describe how those machines move and develop force, several hypothesis have been proposed. They range from purely mechanical models, in which a conformational change takes place during the chemical cycle and drives the motor to the final state (11-13), to stochastic descriptions based on thermal ratchets. In the latter models, the molecular motor thermally explores the energy landscape and the arrival to the final state triggers the chemical cycle and prevents the motor from stepping back (14-21).A detailed description of the mechanical cycle (existence of internal subcycles and their dynamics) is essential to discriminate among the various theoretical models. The myosin V-actin complex is naturally a good candidate for this study: at each chemical cycle the myosin V center of mass moves toward the plus-end of the actin filaments, by steps of 36 nm (5). This movement is among the widest steps observed in molecular motors, and it facilitates the observation and characterization of the mechanical substeps. In addition, myosin V, like many dimeric machines, moves along the filament in a hand-over-hand manner (9), which seems to be a very general feature of processive motors (22,23).The single-molecule approach has been indispensable to understand the myosin V dynamics: this motor steps back only occasionally at zero load, whereas the backward/forward...