Self-assembly of block copolymers into interesting and
useful nanostructures,
in both solution and bulk, is a vibrant research arena. While much
attention has been paid to characterization and prediction of equilibrium
phases, the associated dynamic processes are far from fully understood.
Here, we explore what is known and not known about the equilibration
of particle phases in the bulk, and spherical micelles in solution.
The presumed primary equilibration mechanisms are chain exchange,
fusion, and fragmentation. These processes have been extensively studied
in surfactants and lipids, where they occur on subsecond time scales.
In contrast, increased chain lengths in block copolymers create much
larger barriers, and time scales can become prohibitively slow. In
practice, equilibration of block copolymers is achievable only in
proximity to the critical micelle temperature (in solution) or the
order–disorder transition (in the bulk). Detailed theories
for these processes in block copolymers are few. In the bulk, the
rate of chain exchange can be quantified by tracer diffusion measurements.
Often the rate of equilibration, in terms of number density and aggregation
number of particles, is much slower than chain exchange, and consequently
observed particle phases are often metastable. This is particularly
true in regions of the phase diagram where Frank–Kasper phases
occur. Chain exchange in solution has been explored quantitatively
by time-resolved SANS, but the results are not well captured by theory.
Computer simulations, particularly via dissipative particle dynamics,
are beginning to shed light on the chain escape mechanism at the molecular
level. The rate of fragmentation has been quantified in a few experimental
systems, and TEM images support a mechanism akin to the anaphase stage
of mitosis in cells, via a thin neck that pinches off to produce two
smaller micelles. Direct measurements of micelle fusion are quite
rare. Suggestions for future theoretical, computational, and experimental
efforts are offered.