Cluster-cluster aggregation has been studied experimentally in two-dim
ensional colloidal systems of moderately high area fraction. In the di
ffusion limited regime the system spontaneously exhibits ordering beyo
nd the scale of the fractal aggregates, which persists into the gelled
state. This ordering arises from an effective inter-cluster repulsion
due to the mutually exclusive depletion zones surrounding each cluste
r. Various metrical and topological properties of the system indicate
that this long-range order is stationary, apart from the inherent chan
ge of scale as the clusters grow. Topological correlations show that t
he inter-cluster self-organization is compatible with maximum entropy:
the non-equilibrium system behaves as if it were in statistical equil
ibrium, and no physical forces are involved in the long-range order. F
or the reaction-limited case no such inter-cluster ordering is evident
at any stage, the system is nonstationary, and the aggregation is gov
erned by specific physical forces.