We report results from a molecular dynamics (MD) simulation on the conformations of a long flexible polyelectrolyte complexed to a charged sphere, both negatively charged, in the presence of neutralizing counterions in the strong Coulomb coupling regime. The structure of this complex is very sensitive to the charge density of the polyelectrolyte. For a fully charged polyelectrolyte the polymer forms a dense two-dimensional "disk", whereas for a partially charged polyelectrolyte the monomers are spread over the colloidal surface. A mechanism involving the overcharging of the polyelectrolyte by counterions is proposed to explain the observed conformations.PACS numbers: 61.20. Qg, 82.70.Dd, 87.10.+e Polyelectrolytes in polar solvents are polymers carrying dissociated ionic groups. When a polyelectrolyte is in the vicinity of a charged colloidal particle, both may coagulate leading to charge complexation. Studying this process is motivated by many sources. The presence of polyelectrolytes has important effects on the stabilization of colloidal suspensions [1]. Besides that, for polyelectrolytes such as DNA the interaction with the interface of charged membranes or charged particles (histones) is crucial for many biophysical properties [2]. Finally long range Coulomb interactions represent a theoretical challenge, especially for the understanding of effective attractions between like charged bodies [3,4,5,6].The adsorption of polyelectrolytes onto an oppositely charged spherical particle has recently been experimentally extensively studied [2,7,8,9]. Various authors have also investigated this phenomenon theoretically [10,11,12,13,14,15,16] and by numerical simulations [17,18,19]. However, much less is known concerning the complexation of a charged sphere with a like-charged polyelectrolyte. To our knowledge there has been no study in this direction until now.In this Letter, we report the rather unexpected complexation between a charged sphere and a long flexible polyelectrolyte, both like (here negatively) charged. This article constitutes a first attempt to elucidate this striking phenomenon. We present results of MD simulation of the two macroions taking into account the counterions explicitly, but add for simplicity no salt. We propose a mechanism stemming from the polyelectrolyte overcharging to explain the complexation structure as well as the observed polyelectrolyte conformations.The MD method employed here is based on the Langevin equation and is the same as the one employed in previous studies [20]. Consider within the framework of the primitive model one spherical macroion characterized by a radius r 0 and a bare charge Q = −Z M e (where e is the elementary charge and Z M > 0) surrounded by an implicit solvent of relative dielectric permittivity ǫ r . The polymer chain is made up of N m monomers of diameter l. Both ends of the chain are always charged. The monomer charge fraction is f (i.e. every 1/f monomer is charged) so that the chain contains N cm = (N m − 1)f + 1 charged monomers. The monomer charg...