Mixing describes the process by which scalars, such as solute concentration
or fluid temperature, evolve from an initial heterogeneous state to uniformity
under the stirring action of a fluid flow. Mixing occurs initially through the
formation of scalar lamellae as a result of fluid stretching and later by their
coalescence due to molecular diffusion. Owing to the linearity of the
advection-diffusion equation, scalar coalescence can be envisioned as an
aggregation process. While random aggregation models have been shown to capture
scalar mixing across a range of turbulent flows, we demonstrate here that they
are not accurate for most chaotic flows. In particular, we show that the
spatial distribution of the number of lamellae in aggregates is highly
correlated with their elongation and is also influenced by the fractal geometry
that arises from the chaotic flow. The presence of correlations makes mixing
less efficient than a completely random aggregation process because lamellae
with similar elongations and scalar levels tend to remain isolated from each
other. Based on these observations, we propose a correlated aggregation
framework that captures the asymptotic mixing dynamics of chaotic flows and
predicts the evolution of the scalar pdf based on the flow stretching
statistics. We show that correlated aggregation is uniquely determined by a
single exponent which quantifies the effective number of random aggregation
events, and is dependent on the fractal dimension of the flow. These findings
expand aggregation theories to a larger class of systems, which have relevance
to various fundamental and applied mixing problems