The
flexibility of a single polymer chain, characterized by its
persistence length, is considered to be an intrinsic property of the
polymer chain, which determines its conformation and transport properties.
In this work, we find from molecular dynamics simulations for a single
ring polymer chain in thin films of linear chain melts that the relative flexibility of the ring chain (compared to the
flexibility of linear chains) determines where the ring polymer chain
is located within thin films and how fast the ring polymer chain diffuses
laterally. In this work, we tune the flexibility of ring and linear
chains by changing the bending angle potential parameter, while other
intra- and intermolecular interaction potentials are identical for
both ring and linear chains. We find that it is not the flexibility
of individual polymer chains but the relative flexibility that determines
the spatial arrangement of the ring chain in thin polymer films. When
a ring polymer chain is more flexible (more rigid) than linear polymer
chains, the ring polymer is more likely to be located at the film
surface (the film center). Such spatial arrangement should originate
from the conformational entropy of the ring polymer chain. The ring
chain at the film surface is compressed more than that at the film
center. This makes the ring chain at the surface threaded less by
linear chains. Because the relatively flexible ring chain prefers
the film surface (which is more mobile than at the film center) and
experiences less entanglement, the relatively flexible ring chain
diffuses faster than the relatively rigid ring chain.