Computing the Helmholtz energy function of solids: Difference between revisions

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*[http://dx.doi.org/10.1063/1.3483899  Tai Boon Tan, Andrew J. Schultz, and David A. Kofke "Efficient calculation of temperature dependence of solid-phase free energies by overlap sampling coupled with harmonically targeted perturbation", Journal of Chemical Physics 133, 134104 (2010)]
*[http://dx.doi.org/10.1063/1.3483899  Tai Boon Tan, Andrew J. Schultz, and David A. Kofke "Efficient calculation of temperature dependence of solid-phase free energies by overlap sampling coupled with harmonically targeted perturbation", Journal of Chemical Physics 133, 134104 (2010)]
*[http://dx.doi.org/10.1080/00268976.2015.1005704 Martin B. Sweatman "Comparison of absolute free energy calculation methods for fluids and solids", Molecular Physics '''113''' pp. 1206-1216 (2015)]
*[http://dx.doi.org/10.1080/00268976.2015.1005704 Martin B. Sweatman "Comparison of absolute free energy calculation methods for fluids and solids", Molecular Physics '''113''' pp. 1206-1216 (2015)]
*[http://dx.doi.org/10.1063/1.4944069  C. Calero1, C. Knorowski and A. Travesset "Determination of anharmonic free energy contributions: Low temperature phases of the Lennard-Jones system", Journal of Chemical Physics '''144''' 124102 (2016)]




[[Category: Monte Carlo]]
[[Category: Monte Carlo]]

Latest revision as of 15:29, 5 April 2016

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There are various methods of computing the Helmholtz energy function of solid phases. The most widely used is the procedure based on the techniques of thermodynamic integration. The usual implementations derive from the paper by Frenkel and Ladd [1] which makes use of the Einstein crystal concept. Recently, a more efficient formalism has been developed by N. G. Almarza [2].

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