We study the effects of long range interactions on the phases observed in cohesive granular materials. At high vibration amplitudes, a gas of magnetized particles is observed with velocity distributions similar to non-magnetized particles. Below a transition temperature compact clusters are observed to form and coexist with single particles. The cluster growth rate is consistent with a classical nucleation process. However, the temperature of the particles in the clusters is significantly lower than the surrounding gas, indicating a breakdown of equipartition. If the system is quenched to low temperatures, a meta-stable network of connected chains self-assemble due to the anisotropic nature of magnetic interactions between particles.Vibro-fluidized inelastic spherical particles are an important model system which capture the essence of dissipative interactions on the statistical properties of dry non-cohesive granular materials [1]. This system has emerged as an important test bed to investigate the applicability of dissipative kinetic theory [2,3]. Experiments measuring the position and velocity of individual particles show the formation of clusters, non-Gaussian velocity distributions (to varying extent), and the violation of equipartition [4,5]. In a number of applications, additional cohesive interactions often exist due to the presence of moisture, electrostatic screening, and magnetization [6].In this Letter, we introduce a novel system consisting of magnetized particles inside a vibrated container. This enables us to study the effect of long-range attractive interactions on the formation of clusters and the velocity distributions of cohesive granular materials. Non-magnetic particles are also present in our system to define a system temperature that depends on the vibration amplitude of the container. A gas-like phase of magnetized particles is observed at high system temperature. If the system is slowly cooled below a transition temperature, compact clusters precipitate and grow in time. If the temperature is rapidly quenched, an extended mesh of particles is observed to self-assemble due to the anisotropy of the interaction. The structure and growth of the clusters is consistent with both a classical nucleation process, and recent theories of the dipolar hard sphere model [7][8][9][10]. However, the velocity distributions and the associated granular temperature of the free and clustered particles show the influence of dissipation and cohesion.The idealized interaction between two dipolar hard spheres separated by distance r is defined aswhere U HS corresponds to the hard core repulsion interaction, µ is the dipole moment, and r is the interparticle vector connecting the centers of dipoles i, j. This type of interaction has been put forth as an extremum model for ferro-fluids [11,12]. If the potential is averaged over all possible dipole arrangements, the familiar r −6 van der Waals interaction is recovered. This implies that such systems should have a well defined liquid gas transition. However, extensi...