2012
DOI: 10.1039/c2sm26706c
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Density anomaly in a fluid of softly repulsive particles embedded in a spherical surface

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Cited by 14 publications
(11 citation statements)
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References 30 publications
(29 reference statements)
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“…Substances as well as theoretical models which also display water-like anomalies will likely share similar features in their volume gap. We refer, for instance, to isotropic onecomponent systems which undergo, upon isothermal compression, a reentrant melting over some range of temperatures and pressures; such are the systems in which particles softly repel each other through a Gaussian potential, [28][29][30][31] a modified inverse-power potential, 32,33 or a Yoshida-Kamakura (YK) potential. [34][35][36] To confirm this hypothesis, we have carried out some preliminary calculations for the latter potential at reduced pressures P = 0.3 and 1 (values in units of the energy and length parameters of the potential) which correspond to two different regions of the phase diagram: in fact, for P = 0.3 the YK model behaves "normally," while for P = 1 the fluid phase exhibits a water-like volumetric anomaly followed, at lower temperatures, by solidification at a thermodynamic state point located on a reentrant-melting line (see Fig.…”
Section: Discussionmentioning
confidence: 99%
“…Substances as well as theoretical models which also display water-like anomalies will likely share similar features in their volume gap. We refer, for instance, to isotropic onecomponent systems which undergo, upon isothermal compression, a reentrant melting over some range of temperatures and pressures; such are the systems in which particles softly repel each other through a Gaussian potential, [28][29][30][31] a modified inverse-power potential, 32,33 or a Yoshida-Kamakura (YK) potential. [34][35][36] To confirm this hypothesis, we have carried out some preliminary calculations for the latter potential at reduced pressures P = 0.3 and 1 (values in units of the energy and length parameters of the potential) which correspond to two different regions of the phase diagram: in fact, for P = 0.3 the YK model behaves "normally," while for P = 1 the fluid phase exhibits a water-like volumetric anomaly followed, at lower temperatures, by solidification at a thermodynamic state point located on a reentrant-melting line (see Fig.…”
Section: Discussionmentioning
confidence: 99%
“…Even though clearcut phase transitions (i.e., thermodynamic singularities) cannot occur in a few-particle system, a convenient choice of boundary conditions may alleviate the difference with an infinite system, making the study of a finite quantum system valuable anyway. A practical solution is to use spherical boundary conditions (SBCs), which have often been exploited in the past to discourage long-range triangular ordering at high density [ 33 , 34 , 35 , 36 , 37 , 38 ]. On the other hand, SBCs make it possible to observe novel forms of ordering, viz.…”
Section: Introductionmentioning
confidence: 99%
“…In such a case, the numerical investigation requires appropriate boundary conditions and the thermodynamic limit may be difficult to approach. "Spherical boundary conditions", which amount to considering the system on the surface of a sphere (or a hypersphere) where no boundaries need to be specified and increasing the radius of this sphere, have then been proposed as an alternative to the common procedure [20][21][22][23][24][25][26] On a general theoretical ground, studying the properties of a system in uniformly curved space provides an extra control parameter (the Gaussian curvature) in addition to the common thermodynamic parameters. This may prove interesting in several cases.…”
Section: Introductionmentioning
confidence: 99%