{"data":{"id":"10.6084/m9.figshare.c.2555520.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.c.2555520.v1","prefix":"10.6084","suffix":"m9.figshare.c.2555520.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Ó. Vázquez-Rodríguez","affiliation":[],"nameIdentifiers":[]},{"name":"H. Ruiz-Estrada","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"An explicit expression for the static structure factor for a multi-Yukawa fluid: the one-component case"}],"publisher":"Figshare","container":{},"publicationYear":2016,"subjects":[{"subject":"Space Science"},{"subject":"29999 Physical Sciences not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Physical sciences","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Medicine"},{"subject":"Hematology"},{"subject":"Computational Biology"}],"contributors":[],"dates":[{"date":"2016-02-23","dateType":"Created"},{"date":"2016-05-18","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"GEN","bibtex":"misc","citeproc":"article","schemaOrg":"Collection","resourceType":"Collection","resourceTypeGeneral":"Collection"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1080/00319104.2016.1139708","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.c.2555520","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"CC-BY","rightsUri":"http://creativecommons.org/licenses/by/3.0/us"}],"descriptions":[{"description":"By using the mean spherical approximation, we obtain an analytical expression for the static structure factor (SSF) for a monodisperse system of particles interacting through a potential given by a hard-sphere contribution and \u003ci\u003eM\u003c/i\u003e Yukawa terms. This expression depends on scaling matrix \u003cb\u003eΓ\u003c/b\u003e, which is determined by solving a set of nonlinear equations. Our theoretical results show that using three Yukawa terms in the closure relation greatly improves the accuracy when compared with hypernetted-chain closure and Monte Carlo simulation data, which display a secondary low-\u003ci\u003ek\u003c/i\u003e peak in the SSF, due to the formation of an intermediate range order structure governed by a short-range attraction and a long-range repulsion. We discuss the appearance of such a peak in terms of the microstructure order given by the radial distribution function. Following the original proposal made by Waisman (Mol Phys. 1973; 25:45–48), we give an explicit expression that improves the structural properties of a hard-sphere system.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/collections/An_explicit_expression_for_the_static_structure_factor_for_a_multi_Yukawa_fluid_the_one_component_case/2555520/1","contentUrl":null,"metadataVersion":3,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"api","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":0,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2016-02-23T02:56:00.000Z","registered":"2016-02-23T02:56:01.000Z","published":"2016","updated":"2024-12-14T20:15:03.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients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