Nematic liquid crystals at rough and fluctuating interfaces are analyzed within
the Frank elastic theory and the Landau–de Gennes theory. We study specifically
interfaces that locally favor planar anchoring. In the first part we reconsider the
phenomenon of Berreman anchoring on fixed rough surfaces, and derive new simple
expressions for the corresponding azimuthal anchoring energy. Surprisingly, we find
that for strongly aligning surfaces, it depends only on the geometrical surface
anisotropy and the bulk elastic constants, and not on the precise values
of the chemical surface parameters.
In the second part, we calculate the capillary waves at nematic-isotropic
interfaces. If one neglects elastic interactions, the capillary wave spectrum
is characterized by an anisotropic interfacial tension. With elastic interactions,
the interfacial tension, i.e., the coefficient of the leading q2 term of
the capillary wave spectrum, becomes isotropic. However, the elastic interactions
introduce a strongly anisotropic cubic q3 term. The amplitudes of
capillary waves are largest in the direction perpendicular to the director.
These results are in agreement with previous molecular dynamics simulations.