Shear-induced melting and crystallization were investigated by confocal microscopy in concentrated colloidal suspensions of hardsphere-like particles. Both silica and polymethylmethacrylate suspensions were sheared with a constant rate in either a countertranslating parallel plate shear cell or a counterrotating cone-plate shear cell. These instruments make it possible to track particles undergoing shear for extended periods of time in a plane of zero velocity. Although on large scales, the flow profile deviated from linearity, the crystal flowed in an aligned sliding layer structure at low shear rates. Higher shear rates caused the crystal to shear melt, but, contrary to expectations, the transition was not sudden. Instead, although the overall order decreased with shear rate, this was due to an increase in the nucleation of localized domains that temporarily lost and regained their ordered structure. Even at shear rates that were considered to have melted the crystal as a whole, ordered regions kept showing up at times, giving rise to very large fluctuations in 2D bond-orientational order parameters. Low shear rates induced initially disordered suspensions to crystallize. This time, the order parameter increased gradually in time without large fluctuations, indicating that shear-induced crystallization of hard spheres does not proceed via a nucleation and growth mechanism. We conclude that the dynamics of melting and crystallization under shear differ dramatically from their counterparts in quiescent suspensions.T he majority of complex fluids are non-Newtonian liquids.That is, when subjected to a shear flow, they exhibit shear thinning or shear thickening behavior. It has long been established that the macroscopic properties of a material are coupled to its microstructure. To understand the macroscopic behavior of flowing complex fluids, much research has been done on revealing the microstructure under shear.Apart from shear thinning and shear thickening, also shear banding, which is characterized by a discontinuous jump in the flow profile, is observed for many complex fluids (1). For worm-like micellar systems this has been extensively studied (2-5). Shear banding has also been observed in rod-like colloidal suspensions (6) and in crystallizing suspensions of spherical colloids (7-10), but for the latter, the number of studies is limited. found the origin of shear banding with rheometry and small angle neutron scattering. They found that colloidal crystals shear thin discontinuously and that this is associated with a transition from a polycrystalline structure to a sliding layer structure. For not too soft potentials, these sliding layers have a hexagonal symmetry (15, 16). By using microscopy, it has been shown that this transition also leads to a shear banded flow (7).Shear has a dual influence on the order in colloidal suspensions. At high shear rates, it can disorder, or melt, a colloidal crystal (17-19), but at low shear rates or at low-amplitude oscillatory shear, it can induce order (20)(21)(22). Sh...