In nanoconfined thin
films, numerous studies have revealed the
thickness dependencies of different thermophysical properties, including
the glass transition temperature (T
g)
and self-diffusion coefficient (D). While quantitative
relationships between these properties are well-known for bulk polymers,
analogous relationships for nanoconfined polymers are still not clear.
Herein, T
g−D relationships
are studied under nanoconfinement using spectroscopic ellipsometry
for measuring T
g and fluorescence recovery
after photobleaching for measuring D. Poly(isobutyl
methacrylate) (PiBMA) was selected as a model unentangled polymer,
and it was nanoconfined to 14–300 nm thick films. Multilayered
geometries incorporating PiBMA were constructed to systematically
study the influence of free surfaces (i.e., polymer surfaces exposed
directly to air, also called uncapped) and surfaces that were in contact
with a secondary polymer (also called capped). This multilayer approach
additionally allowed investigation of both relatively weak and strong
interactions between the polymer and substrate, depending on the existence
of hydrogen bonding. The T
g–D relationship observed in nanoconfined thin films deviated
from that in the bulk state (e.g., as described by Williams–Landel–Ferry
and Stokes–Einstein, or similar relationships). A model was
employed that considered the effects of molecular friction between
the different confining interfaces and PiBMA, and it successfully
described the deviation from bulk behavior.