Liquid-crystal patterns of rectangular particles in a square nanocavity

Abstract

Using density-functional theory in the restricted-orientation approximation, we analyze the liquid-crystal patterns and phase behavior of a fluid of hard rectangular particles confined in a two-dimensional square nanocavity of side length H composed of hard inner walls. Patterning in the cavity is governed by surface-induced order as well as capillary and frustration effects and depends on the relative values of the particle aspect ratio κ ≡ L/σ, with L the length and σ the width of the rectangles (L ≥σ), and cavity size H. Ordering may be very different from bulk (H → ∞) behavior when H is a few times the particle length L (nanocavity). Bulk and confinement properties are obtained for the cases κ = 1, 3, and 6. In bulk the isotropic phase is always stable at low packing fractions η = Lσρ0 (with ρ0 the average density) and nematic, smectic, columnar, and crystal phases can be stabilized at higher η depending on κ: For increasing η the sequence of isotropic to columnar is obtained for κ = 1 and 3, whereas for κ = 6 we obtain isotropic to nematic to smectic (the crystal being unstable in all three cases for the density range explored). In the confined fluid surface-induced frustration leads to fourfold symmetry breaking in all phases (which become twofold symmetric). Since no director distortion can arise in our model by construction, frustration in the director orientation is relaxed by the creation of domain walls (where the director changes by 90º); this configuration is necessary to stabilize periodic phases. For κ = 1 the crystal becomes stable with commensurate transitions taking place as H is varied. These transitions involve structures with different number of peaks in the local density. In the case κ = 3 the commensurate transitions involve columnar phases with different number of columns. In the case κ = 6 the high-density region of the phase diagram is dominated by commensurate transitions between smectic structures; at lower densities there is a symmetry-breaking isotropic to nematic transition exhibiting nonmonotonic behavior with cavity size. Apart from the present application in a confinement setup, our model could be used to explore the bulk region near close packing in order to elucidate the possible existence of disordered phases at close packing