Dipolar interactions, molecular flexibility, and flexoelectricity in bent-core liquid crystals

TL;DR

This study uses Monte Carlo simulations to explore how dipolar interactions and molecular flexibility influence the phase behavior and flexoelectric properties of bent-core liquid crystals, revealing phase transitions and structural fluctuations.

Contribution

It introduces a detailed simulation analysis of dipolar effects, molecular flexibility, and flexoelectricity in bent-core liquid crystals, highlighting their impact on phase stability and properties.

Findings

Dipolar interactions destabilize certain liquid crystal phases.

Molecular flexibility induces smectic fluctuations and reduces tilt.

Flexoelectric coefficients vary with phase and interactions.

Abstract

The effects of dipolar interactions and molecular flexibility on the structure and phase behavior of bent-core molecular fluids are studied using Monte Carlo computer simulations. Some calculations of flexoelectric coefficients are also reported. The rigid cores of the model molecules consist of either five or seven soft spheres arranged in a `V' shape with external bend angle $\gamma$. With purely repulsive sphere-sphere interactions and $\gamma=0^\circ$ (linear molecules) the seven-sphere model exhibits isotropic, uniaxial nematic, smectic-A, and tilted phases. With $\gamma \geq 20^\circ$ the smectic-A phase disappears, while the system with $\gamma \geq 40^\circ$ shows a direct tilted smectic--isotropic fluid transition. The addition of electrostatic interactions between transverse dipole moments on the apical spheres is generally seen to reduce the degree of tilt in the smectic and solid phases, destabilize the nematic and smectic-A phases of linear molecules, and destabilize the tilted smectic-B phase of bent-core molecules. The effects of adding three-segment flexible tails to the ends of five-sphere bent-core molecules are examined using configurational-bias Monte Carlo simulations. Only isotropic and smectic phases are observed. On the one hand, molecular flexibility gives rise to pronounced fluctuations in the smectic-layer structure, bringing the simulated system in better correspondence with real materials; on the other hand, the smectic phase shows almost no tilt. Lastly, the flexoelectric coefficients of various nematic phases -- with and without attractive sphere-sphere interactions -- are presented. The results are encouraging, but the computational effort required is a drawback associated with the use of fluctuation relations.