| Abstract: | Main chain liquid crystalline polymers (LCPs) at solid-nematic interfaces exhibit a variety of phase transition between distorted and undistorted states. In one case the transition results from the confinement of grafted chains immersed in a nematic solvent and subject to homeotropic anchoring. The general features of the transition are similar for long and for short chains. The detailed physics is different since long chains exhibit Gaussian, entropic elasticity while the elasticity of the short chain is due to their rigidity. As a result it is possible to weakly confine long chains without triggering a distortion while for short chains the nematic distortion occurs simultaneously with the buckling of the rod like LCPs. Related effects are found for uniformly adsorbed LCPs and for free, confined chains. Different scenarios are expected when homogeneous anchoring is imposed. |
