2009
DOI: 10.1063/1.3253297
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Liquid polymorphism, order-disorder transitions and anomalous behavior: A Monte Carlo study of the Bell–Lavis model for water

Abstract: Monte Carlo simulation strategies for computing the wetting properties of fluids at geometrically rough surfaces J. Chem. Phys. 135, 184702 (2011) Semi-bottom-up coarse graining of water based on microscopic simulations J. Chem. Phys. 135, 184101 (2011) Hydrophobic interactions in presence of osmolytes urea and trimethylamine-N-oxide J. Chem. Phys. 135, 174501 (2011) Potential of mean force between identical charged nanoparticles immersed in a size-asymmetric monovalent electrolyte J. Chem. Phys. 135,… Show more

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Cited by 27 publications
(25 citation statements)
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“…The spin-1 variables and mapping scheme to the BEG model were suggested by Young and Lavis 33 . This scheme was later employed by Barbosa et al 30 who used convenient lattice-gas variables to separately describe occupational and orientational ordering (see, also 31 ). In Ref.…”
Section: Model and Details Of Simulationmentioning
confidence: 99%
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“…The spin-1 variables and mapping scheme to the BEG model were suggested by Young and Lavis 33 . This scheme was later employed by Barbosa et al 30 who used convenient lattice-gas variables to separately describe occupational and orientational ordering (see, also 31 ). In Ref.…”
Section: Model and Details Of Simulationmentioning
confidence: 99%
“…30,34 the BL model was solved by the cluster variation method and a weak first-order phase transition was again obtained. Later Fiore et al 31 performed Monte Carlo (MC) calculations and attributed the transition to the Ising universality class, claiming that the first order phase transition obtained in previous papers was the artifact arising due to the Bethe-like (cluster) methods used for calculation.…”
Section: Introductionmentioning
confidence: 99%
“…AtT = 0, coexistence between a gas and a structured liquid of low density (SL) and coexistence between the structured low-density liquid and the nonstructured high-density liquid are present [32]. However, for finite temperatures, the transition between the two liquids becomes critical, as shown from detailed systematic analysis of simulational data [25]. The two liquid phases do not coexist and the density varies continuously at the phase transition as shown by susceptibility measurements on sublattice density fluctuations [27].…”
Section: The Bell-lavis Model As Solventmentioning
confidence: 99%
“…Both models present several of the anomalous features of water [14][15][16][17][18][19][20][21][22][23][24][25][26][27]. However, the second kind of model does not involve specific orientation of low-energy pairs of particles: pair energy is controlled by distance, not by orientation.…”
Section: Introductionmentioning
confidence: 99%
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