2010
DOI: 10.1063/1.3463424
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Softness dependence of the anomalies for the continuous shouldered well potential

Abstract: By molecular dynamic simulations we study a system of particles interacting through a continuous isotropic pairwise core-softened potential consisting of a repulsive shoulder and an attractive well. The model displays a phase diagram with three fluid phases, a gas-liquid critical point, a liquid-liquid critical point, and anomalies in density, diffusion and structure. The hierarchy of the anomalies is the same as for water. Here we study in a systematic way the effect on the anomalies of varying the softness o… Show more

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Cited by 76 publications
(88 citation statements)
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References 57 publications
(68 reference statements)
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“…Also in confined water clustering, due to hydrogen-bond correlation, has been considered as the cause for increased mobility [67]. In our case layering [31] and long-range correlations and structural changes [30] can be the origin of correlated aggregates and collective modes responsible for the moderate increase of mobility.…”
Section: B Confinement Effects On Dynamicsmentioning
confidence: 97%
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“…Also in confined water clustering, due to hydrogen-bond correlation, has been considered as the cause for increased mobility [67]. In our case layering [31] and long-range correlations and structural changes [30] can be the origin of correlated aggregates and collective modes responsible for the moderate increase of mobility.…”
Section: B Confinement Effects On Dynamicsmentioning
confidence: 97%
“…The distance is large enough to have homogeneous fluid inside the pore [31] for a range of T and ρ comparable to that investigated for the bulk case in previous works [28][29][30]. The attractive wall is made of CSW particles quenched in a triangular lattice with constant d = a and centered at z attr = 0.…”
mentioning
confidence: 95%
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“…Recently it has been proposed that a CS potential exhibits density anomaly if the two length scales identified with the softened region would be accessible 22,24,48 what can be understood as follows. The radial distribution, g(r) of a CS potential has peaks at g(r 1 ) and g(r 2 ) where r 1 and r 2 > r 1 are the two length scales of the CS potential 1,20 .…”
Section: Introductionmentioning
confidence: 99%
“…12 CSW consists of five adjustable parameters that allow it to assume several quite distinct forms, ranging from deep double walls to repulsive ramp-like potentials. In our work we used original parameters as proposed by Franzese et al [13][14][15] Due to the presence of strongly repulsive wall, mildly repulsive shoulder and attractive well, CSW is rather difficult to treat with IE. As we show later, some standard procedures and closures fail or yield erroneous results.…”
Section: Introductionmentioning
confidence: 99%