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Artículo

dc.creatorVega, Carloses
dc.creatorRull Fernández, Luis Felipees
dc.creatorLago, S.es
dc.date.accessioned2018-02-02T17:02:03Z
dc.date.available2018-02-02T17:02:03Z
dc.date.issued1995
dc.identifier.citationVega, C., Rull Fernández, L.F. y Lago, S. (1995). Location of the Fisher-Widom line for systems interacting through short-ranged potentials. Physical Review E, 51 (4), 1-10.
dc.identifier.issn1539-3755 (impreso)es
dc.identifier.urihttps://hdl.handle.net/11441/69944
dc.description.abstractFor finite-ranged potentials the behavior of the total correlation function h (r) at large distances can be of two different types. In three-dimensional systems at low densities the function r h (r) presents exponential decay whereas at high densities it presents exponentially damped oscillatory decay. The locus of points on the phase diagram where a transition from exponential to oscillatory decay occurs is denoted as the Fisher-Widom line after the work of these authors [M. E. Fisher and B. Widom, J. Chem. Phys. 50, 3756 {1969)]. These authors exactly computed the Fisher-Widom line for several one-dimensional systems and conjectured that the same behavior could occur in three dimensions. In this work the Fisher-VA'dom line is computed for a three-dimensional finite-range potential by using the structural information obtained from the reference hypernetted chain theory which is probably the most successful theory of liquid structure available now. By combining these results with computer simulations of the vapor-liquid equilibria of the considered model the Fisher-Widom line is located within the phase diagram of the model. For the considered model the Fisher-VA'dom line cuts the liquid branch of the vapor liquid equilibria at a reduced temperature of T/T, =0.88 and a reduced density of p/p, =2.07. The effect of the range of the potential on the location of the Fisher-%'idom line is also considered. Increasing the range of the potential reduces the region of the phase diagram where oscillatory behavior of the function r h (r ) occurs. The long-range decay of a Lennard Jones Quid is also considered. Decay of h (r) to zero at large distances is difFerent for a Lennard-Jones potential and for a finite-ranged potential. Although the Lennard Jones potential does not present a true Fisher-Widom line when the ultimate decay of h (r} is considered it is shown that it exhibits a Fisher-Widom —like transition when an intermediate range of distances is considered.es
dc.formatapplication/pdfes
dc.language.isoenges
dc.publisherPhysical Review Ees
dc.relation.ispartofPhysical Review E, 51 (4), 1-10.
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.titleLocation of the Fisher-Widom line for systems interacting through short-ranged potentialses
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Física Atómica, Molecular y Nucleares
idus.format.extent10 P.es
dc.journaltitlePhysical Review Ees
dc.publication.volumen51es
dc.publication.issue4es
dc.publication.initialPage1es
dc.publication.endPage10es
dc.identifier.sisius6607671es

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