We report an optical and atomic force microscopic study of interactions between charged polystyrene spheres at a water-air interface. Optical observations of bonded particle clusters and formation of circular chainlike structures at the interface demonstrate that the interaction potential is of dipole origin. Atomic force microscope phase images show patchy domains on the colloidal surface, indicating that the surface charge distribution is not uniform as is commonly believed. Such surface heterogeneity introduces inplane dipoles, leading to an attraction at short interparticle distances. DOI: 10.1103/PhysRevLett.95.218301 PACS numbers: 82.70.Dd, 61.20.ÿp, 68.05.Gh Coulomb repulsion between molecules of the same charge is a fundamental force necessary for the stability and structure formation of various macromolecules in aqueous solutions [1]. However, in some special circumstances, attractions are observed between like-charged species ranging from simple colloidal particles [2] to complex cytoskeletal filamentous actin [3] and DNA [4]. Because of its fundamental interest and important implications in colloid science and biology, the paradox of likecharge attractions has been under intensive theoretical scrutiny for many years [5]. Understanding of such attractions is needed for computer modeling, process control, and various engineering applications of colloids from soft materials to biotechnology. A careful examination of the experimental conditions reveals that the attractions occur when the charged particles (or macromolecules) and the screening counterions are in confined geometries such that the usual spherical symmetry of the counterion distribution is broken. For example, attractions between like-charged particles were found only when they are dispersed near a solid wall [2] or at a liquid interface [6,7].Charged colloidal particles dispersed at an aqueous interface are stabilized by the Coulomb repulsion between the induced out-of-plane dipoles due to the asymmetric distribution of counterions in the aqueous phase [8,9]. The inset in Fig. 1 shows the surface charge on the particle and the asymmetric counterion clouds in water at an average separation of the Debye screening length D from the sphere's surface. If the charge distribution on the particle surface is uniform, a dipole moment pointing downward perpendicular to the interface forms with a magnitude [9] P z ' q 0 D = p , where q 0 is the effective charge carried by the particle and ('80) is the dielectric constant of water. A crucial assumption made for charged latex spheres is that the surface charge distribution of the particles is uniform. All such spheres have charge-stabilizing chemical functionality on their surfaces, but the actual distribution of the surface charge groups has not been examined systematically.Recent experiments [6,7] indicated that the interfacial particles also experience attractions, but the origin of such attractions remains illusive [7,10]. While these experiments revealed interesting mesostructure formation of par...