Hydrodynamic theory of atic liquid crystals
arXiv:2106.11957 · doi:10.1103/PhysRevE.106.024701
Abstract
We formulate a comprehensive hydrodynamic theory of two-dimensional liquid crystals with generic fold rotational symmetry, also known as atics, of which mematics and hexatics are the two best known examples. Previous hydrodynamic theories of atics are characrerized by continuous rotational symmetry, which is higher than the discrete rotational symmetry of atic phases. By contrast, here we demonstrate that the discrete rotational symmetry allows the inclusion of additional terms in the hydrodynamic equations, which, in turn, lead to novel phenomena, such as the possibility of flow alignment at high shear rates, even for . Furthermore, we show that any finite imposed shear will induce long-ranged orientational order in any atic liquid crystal, in contrast to the quasi-long-ranged order that occurs in the absence of shear. The induced order parameter scales like a non-universal power of the applied shear rate at small shear rates.
25 pages, 7 figures
References in corpus (6)
- Spontaneous motion in hierarchically assembled active matter
- Data-driven quantitative modeling of bacterial active nematics
- Hydrodynamic theory for nematic shells: the interplay among curvature, flow and alignment
- Locomotion and transport in a hexatic liquid crystal
- Driven active and passive nematics
- Long-ranged order and flow alignment in sheared atic liquid crystals
Cited by in corpus (8)
- Long-ranged order and flow alignment in sheared atic liquid crystals
- Hydrodynamic Enhancement of -atic Defect Dynamics
- Active topological defect absorption by a curvature singularity
- Supramolecular assemblies in active motor-filament systems: micelles, bilayers, and foams
- Massive Higher-Spin Fields in the Fractional Quantum Hall Effect
- Hydrodynamic stability and pattern formation in hexatic epithelial layers
- Defect Interactions Through Periodic Boundaries in Two-Dimensional -atics
- Noise-induced transitions from contractile to extensile active stress in isotropic fluids