2012
DOI: 10.1063/1.4722209
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Isotropic–nematic phase transition in the Lebwohl–Lasher model from density of states simulations

Abstract: Density of states Monte Carlo simulations have been performed to study the isotropic-nematic (IN) transition of the Lebwohl-Lasher model for liquid crystals. The IN transition temperature was calculated as a function of system size using expanded ensemble density of states simulations with histogram reweighting. The IN temperature for infinite system size was obtained by extrapolation of three independent measures. A subsequent analysis of the kinetics in the model showed that the transition occurs via spinoda… Show more

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Cited by 20 publications
(25 citation statements)
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“…Second, restricting the lateral positions reduces computational effort. Third, lattice-models to investigate liquidcrystalline phase behaviour are well established in the literature, prominent examples being the Zwanzig model (involving discretised translational motion and discretised rotations) [33][34][35][36] and the Lebwohl-Lasher model (particles fixed to lattice sites, continuous rotational motion) [37][38][39]. These models have been successfully used to study orientational ordering both in bulk [37] and in spatially confined systems [34][35][36]38].…”
Section: Introductionmentioning
confidence: 99%
“…Second, restricting the lateral positions reduces computational effort. Third, lattice-models to investigate liquidcrystalline phase behaviour are well established in the literature, prominent examples being the Zwanzig model (involving discretised translational motion and discretised rotations) [33][34][35][36] and the Lebwohl-Lasher model (particles fixed to lattice sites, continuous rotational motion) [37][38][39]. These models have been successfully used to study orientational ordering both in bulk [37] and in spatially confined systems [34][35][36]38].…”
Section: Introductionmentioning
confidence: 99%
“…From the results of previous Monte Carlo (MC) simulations performed on the discrete, nearest-neighbor LL model (see, e.g., Ref. [61]), it is known that T ni ≈ 1.11J/k B , which is distinct from the two values predicted by models I and II. The difference arises because the models are not identical with the (discrete) LL model.…”
Section: Resultsmentioning
confidence: 94%
“…The sampling, originally developed for Hamiltonian models involving random walks in discrete configurational space, continues to be applied to various problems in statistical physics [46,47], polymer and protein studies [48,49,50] and is being developed for more robust applications for continuous systems [51,52,53,54,55,56,57] and self assembly [58]. The proposed algorithm was modified [59] to suit lattice models like the Lebwohl-Lasher interaction [60], allowing for continuous variation of molecular orientations.…”
Section: Hamiltonian Modelmentioning
confidence: 99%