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dc.contributor.authorLaird, Brian Bostian
dc.contributor.authorMcCoy, John D.
dc.contributor.authorHaymet, A. D. J.
dc.date.accessioned2014-12-17T22:28:26Z
dc.date.available2014-12-17T22:28:26Z
dc.date.issued1987-09-01
dc.identifier.citationLaird, Brian Bostian; McCoy, John D.; Haymet, A. D. J. (1987). "Density functional theory of freezing: Analysis of crystal density." The Journal of Chemical Physics, 87(9):5449-5456. http://dx.doi.org/10.1063/1.453663
dc.identifier.issn0021-9606
dc.identifier.urihttp://hdl.handle.net/1808/16165
dc.descriptionThis is the publisher's version, also available electronically from http://scitation.aip.org/content/aip/journal/jcp/87/9/10.1063/1.453663
dc.description.abstractThe density functional theory of freezing is used to study the liquid to crystal phase transition in the hardsphere and Lennard‐Jones systems. An important step in the calculation is the parametrization of the solid phase average single particle density ρ(r). In this work two popular parametrizations are compared. The first method is a general Fourier decomposition of the periodic solid density in which the amplitude of each (non‐symmetry‐related) Fourier component is treated as an independent parameter. The second parametrization, which is more restrictive but easier to implement, approximates the solid density as a sum of Gaussian peaks centered at the sites of a periodic lattice. The two methods give essentially identical results for the phase diagrams for the two systems studied, but the crystal density predicted by the Fourier method exhibits significant anisotropies which are excluded from the Gaussian representation by construction.
dc.publisherAmerican Institute of Physics
dc.titleDensity functional theory of freezing: Analysis of crystal density
dc.typeArticle
kusw.kuauthorLaird, Brian Bostian
kusw.kudepartmentChemistry
dc.identifier.doi10.1063/1.453663
kusw.oaversionScholarly/refereed, publisher version
kusw.oapolicyThis item does not meet KU Open Access policy criteria.
dc.rights.accessrightsopenAccess


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