• Citation: A. Nichol, and G.J. Ackland (2016), "Property trends in simple metals: An empirical potential approach", Physical Review B 93(18), 184101. DOI: 10.1103/physrevb.93.184101.
    Abstract: We demonstrate that the melting points and other thermodynamic quantities of the alkali metals can be calculated based on static crystalline properties. To do this we derive analytic interatomic potentials for the alkali metals fitted precisely to cohesive and vacancy energies, elastic moduli, the lattice parameter, and crystal stability. These potentials are then used to calculate melting points by simulating the equilibration of solid and liquid samples in thermal contact at ambient pressure. With the exception of lithium, remarkably good agreement is found with experimental values. The instability of the bcc structure in Li and Na at low temperatures is also reproduced and, unusually, is not due to a soft T1N phonon mode. No forces or finite-temperature properties are included in the fit, so this demonstrates a surprisingly high level of intrinsic transferability in the simple potentials. Currently, there are few potentials available for the alkali metals, so in addition to demonstrating trends in behavior, we expect that the potentials will be of broad general use.

    Notes: G.J. Ackland noted that lattice parameters, elastic constants and cohesive energies were used in the fitting process, so the values produced by this conversion should match known values. He noted that bcc crystal structure should be stable and produce a melting temperature of 370 K. Publication information was updated on 12 Oct. 2017. Prior publication listing for this potential was Han, S., Zepeda-Ruiz, L. A., Ackland, G. J., Car, R., and Srolovitz, D. J. (2003). Interatomic potential for vanadium suitable for radiation damage simulations. Journal of Applied Physics, 93(6), 3328. DOI: 10.1063/1.1555275

    Related Models:
  • Moldy FS (2016--Nichol-A--Na--MOLDY--ipr1)
    Notes: The parameters in Na.moldy were obtained from http://homepages.ed.ac.uk/graeme/moldy/moldy.html and posted with the permission of G.J. Ackland.
    File(s):
  • LAMMPS pair_style eam/fs (2016--Nichol-A--Na--LAMMPS--ipr1)
    See Computed Properties
    Notes: This conversion was performed by G.J. Ackland and submitted on 8 Dec. 2015.
    File(s): superseded


  • LAMMPS pair_style eam/fs (2016--Nichol-A--Na--LAMMPS--ipr2)
    See Computed Properties
    Notes: A new conversion to LAMMPS performed by G.J. Ackland was submitted on 10 Oct. 2017. The previous setfl version above had a spurious oscillation period in the tabulated r*phi function that influenced measurements, most notably static elastic constant evaluations.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2016--Nichol-A--Na--LAMMPS--ipr2.
    Link(s):
  • Citation: R.S. Elliott, and A. Akerson (2015), "Efficient "universal" shifted Lennard-Jones model for all KIM API supported species".

    Notes: This is the Na interaction from the "Universal" parameterization for the openKIM LennardJones612 model driver.The parameterization uses a shifted cutoff so that all interactions have a continuous energy function at the cutoff radius. This model was automatically fit using Lorentz-Berthelotmixing rules. It reproduces the dimer equilibrium separation (covalent radii) and the bond dissociation energies. It has not been fitted to other physical properties and its ability to model structures other than dimers is unknown. See the README and params files on the KIM model page for more details.

  • See Computed Properties
    Notes: Listing found at https://openkim.org.
    Link(s):
  • Citation: S.R. Wilson, K.G.S.H. Gunawardana, and M.I. Mendelev (2015), "Solid-liquid interface free energies of pure bcc metals and B2 phases", The Journal of Chemical Physics 142(13), 134705. DOI: 10.1063/1.4916741.
    Abstract: The solid-liquid interface (SLI) free energy was determined from molecular dynamics (MD) simulation for several body centered cubic (bcc) metals and B2 metallic compounds (space group: Pm-3m; prototype: CsCl). In order to include a bcc metal with a low melting temperature in our study, a semi-empirical potential was developed for Na. Two additional synthetic "Na" potentials were also developed to explore the effect of liquid structure and latent heat on the SLI free energy. The obtained MD data were compared with the empirical Turnbull, Laird, and Ewing relations. All three relations are found to predict the general trend observed in the MD data for bcc metals obtained within the present study. However, only the Laird and Ewing relations are able to predict the trend obtained within the sequence of "Na" potentials. The Laird relation provides the best prediction for our MD data and other MD data for bcc metals taken from the literature. Overall, the Laird relation also agrees well with our B2 data but requires a proportionality constant that is substantially different from the bcc case. It also fails to explain a considerable difference between the SLI free energies of some B2 phases which have nearly the same melting temperature. In contrast, this difference is satisfactorily described by the Ewing relation. Moreover, the Ewing relation obtained from the bcc dataset also provides a reasonable description of the B2 data.

    Notes: Mikhail Mendelev (Ames Laboratory) noted that his potential was designed to simulate solid-liquid interface properties in sodium. Updated 27 Apr 2015 to include publication information.

    Related Models:
  • LAMMPS pair_style eam/fs (2015--Wilson-S-R--Na--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Mikhail Mendelev (Ames Laboratory) and posted with his permission on 14 Nov. 2014. He noted that his potential was designed to simulate solid-liquid interface properties in sodium.
    Updated 27 Apr 2015 to include publication information. Update 19 July 2021: The contact email in the file's header has been changed. Update Jan 14 2022: Citation information has been updated in the file's header.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2015--Wilson-S-R--Na--LAMMPS--ipr1.
    Link(s):
 
  • Citation: X.W. Zhou, F.P. Doty, and P. Yang (2011), "Atomistic simulation study of atomic size effects on B1 (NaCl), B2 (CsCl), and B3 (zinc-blende) crystal stability of binary ionic compounds", Computational Materials Science 50(8), 2470-2481. DOI: 10.1016/j.commatsci.2011.03.028.
    Abstract: Ionic compounds exhibit a variety of crystal structures that can critically affect their applications. Traditionally, relative sizes of cations and anions have been used to explain coordination of ions within the crystals. Such approaches assume atoms to be hard spheres and they cannot explain the observed structures of some crystals. Here we develop an atomistic method and use it to explore the structure-determining factors beyond the limitations of the hard sphere approach. Our approach is based upon a calibrated interatomic potential database that uses independent intrinsic bond lengths to measure atomic sizes. By carrying out extensive atomistic simulations, striking relationships among intrinsic bond lengths are discovered to determine the B1 (NaCl), B2 (CsCl), and B3 (zinc-blende) structure of binary ionic compounds.

    Related Models:
  • See Computed Properties
    Notes: This file was taken from the August 22, 2018 LAMMPS distribution. It is listed as being contributed by Xiaowang Zhou (Sandia)
    File(s):
 
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl-MgCl2 model referred to as "Pot_1" in the paper that used PBE_D3 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl-MgCl2 model referred to as "Pot_2" in the paper that used PBE_D3 data. Pot_2 was the potential used to calculate the thermophysical properties and was also named ACE or PBE_D3 in different sections of the paper.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl-MgCl2 model referred to as "Pot_3" in the paper that used PBE_D3 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl-MgCl2 model referred to as "Pot_4" in the paper that used PBE_D3 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
 
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl potential fit using PBED4 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the "Pot_N" model described in the citation, which was fit using PBE_D3 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl potential fit using R2SCAND4 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
  • Citation: S. Attarian, C. Shen, D. Morgan, and I. Szlufarska (2025), "Best practices for fitting machine learning interatomic potentials for molten salts: A case study using NaCl-MgCl2", Computational Materials Science 246, 113409. DOI: 10.1016/j.commatsci.2024.113409.
    Abstract: In this work, we developed a compositionally transferable machine learning interatomic potential using atomic cluster expansion potential and PBE-D3 method for (NaCl)1-x(MgCl2)x molten salt and we showed that it is possible to fit a robust potential for this pseudo-binary system by only including data from x={0, 1/3, 2/3, 1}. We also assessed the performance of several DFT methods including PBE-D3, PBE-D4, R2SCAN-D4, and R2SCANrVV10 on unary NaCl and MgCl2 salts. Our results show that the R2SCAN-D4 method calculates the thermophysical properties of NaCl and MgCl2 with an overall modestly better accuracy compared to the other three methods.

    Notes: This listing is for the NaCl potential fit using R2SCANrVV10 data.

  • See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The link was pulled from the paper and contains all associated potentials and training and testing data.
    File(s): Link(s):
 
  • Citation: Z. Fan, M.L. Whittaker, and M. Asta (2025), "Efficient machine learning interatomic potentials robust for liquid and multiple solid polymorphs of NaF and KF", Physical Review Materials 9(10). DOI: 10.1103/xbfm-clgd.
    Abstract: Achieving atomic-level understanding of crystallization of molten salts is of importance to a wide range of technological applications. Recent work [Fan et al., Proc. Natl. Acad. Sci. USA 122, e2425702122 (2025)] revealed that crystal nucleation in molten LiF salt is a multistage process according to the molecular-dynamics (MD) simulations based on an atomic cluster expansion (ACE) machine-learning interatomic potential (MLIP). In order to understand the influence of increasing cation size on nucleation pathways and nucleation rates of molten fluoride salts, here we develop two new ACE MLIPs for NaF and KF. The two ACE MLIPs feature DFT-SCAN-level accuracy for liquid and multiple solid polymorphs over a wide temperature (0–2000 K) and pressure (0-100 GPa) range, and also reproduce well a number of experimental data for solid and liquid equilibrium properties. The efficiency of the two ACE MLIPs enable million-atom-scale or microsecond-scale MD simulations. The two general-purpose ACE MLIPs are expected to be useful for atomistic simulations for different purposes, in addition to studying crystallization of molten NaF and KF salts.

  • LAMMPS pair_style pace (2025--Fan-Z--Na-F--LAMMPS--ipr1)
    See Computed Properties
    Notes: These files were provided by Sergei Starikov on July 15, 2026. The .yaml file is the fitted potential in the original format, while the .yace file is in the LAMMPS-compatible format. The .asi file can be used with pace/extrapolation to perform additional active learning. The link was pulled from the paper and contains training and testing data.
    File(s): Link(s):
 
  • Citation: S.R. Wilson, K.G.S.H. Gunawardana, and M.I. Mendelev (2015), "Solid-liquid interface free energies of pure bcc metals and B2 phases", The Journal of Chemical Physics 142(13), 134705. DOI: 10.1063/1.4916741.
    Abstract: The solid-liquid interface (SLI) free energy was determined from molecular dynamics (MD) simulation for several body centered cubic (bcc) metals and B2 metallic compounds (space group: Pm-3m; prototype: CsCl). In order to include a bcc metal with a low melting temperature in our study, a semi-empirical potential was developed for Na. Two additional synthetic "Na" potentials were also developed to explore the effect of liquid structure and latent heat on the SLI free energy. The obtained MD data were compared with the empirical Turnbull, Laird, and Ewing relations. All three relations are found to predict the general trend observed in the MD data for bcc metals obtained within the present study. However, only the Laird and Ewing relations are able to predict the trend obtained within the sequence of "Na" potentials. The Laird relation provides the best prediction for our MD data and other MD data for bcc metals taken from the literature. Overall, the Laird relation also agrees well with our B2 data but requires a proportionality constant that is substantially different from the bcc case. It also fails to explain a considerable difference between the SLI free energies of some B2 phases which have nearly the same melting temperature. In contrast, this difference is satisfactorily described by the Ewing relation. Moreover, the Ewing relation obtained from the bcc dataset also provides a reasonable description of the B2 data.

    Notes: This listing is for the Na2 parameterization listed in the reference. M.I. Mendelev (Ames Laboratory) noted that "these 'Na' potentials were developed using the same fitting procedure as for the realistic Na potential 2015--Wilson-S-R-Gunawardana-K-G-S-H-Mendelev-M-I--Na except the fact that the latent heat of melting was purposely increased and the liquid was purposely made less ordered. The potentials were developed to study the effect of the latent heat and liquid structure on the SLI properties of bcc metals." Update 27 Apr. 2015: Changed the reference to update publication status.

    Related Models:
  • See Computed Properties
    Notes: This file was sent by M.I. Mendelev (Ames Laboratory) on 13 Jan. 2015 and posted with his permission. Update 19 July 2021: The contact email in the file's header has been changed. Update Jan 14 2022: Citation information has been updated in the file's header.
    File(s):
  • Citation: S.R. Wilson, K.G.S.H. Gunawardana, and M.I. Mendelev (2015), "Solid-liquid interface free energies of pure bcc metals and B2 phases", The Journal of Chemical Physics 142(13), 134705. DOI: 10.1063/1.4916741.
    Abstract: The solid-liquid interface (SLI) free energy was determined from molecular dynamics (MD) simulation for several body centered cubic (bcc) metals and B2 metallic compounds (space group: Pm-3m; prototype: CsCl). In order to include a bcc metal with a low melting temperature in our study, a semi-empirical potential was developed for Na. Two additional synthetic "Na" potentials were also developed to explore the effect of liquid structure and latent heat on the SLI free energy. The obtained MD data were compared with the empirical Turnbull, Laird, and Ewing relations. All three relations are found to predict the general trend observed in the MD data for bcc metals obtained within the present study. However, only the Laird and Ewing relations are able to predict the trend obtained within the sequence of "Na" potentials. The Laird relation provides the best prediction for our MD data and other MD data for bcc metals taken from the literature. Overall, the Laird relation also agrees well with our B2 data but requires a proportionality constant that is substantially different from the bcc case. It also fails to explain a considerable difference between the SLI free energies of some B2 phases which have nearly the same melting temperature. In contrast, this difference is satisfactorily described by the Ewing relation. Moreover, the Ewing relation obtained from the bcc dataset also provides a reasonable description of the B2 data.

    Notes: This listing is for the Na3 parameterization listed in the reference. M.I. Mendelev (Ames Laboratory) noted that "these 'Na' potentials were developed using the same fitting procedure as for the realistic Na potential 2015--Wilson-S-R-Gunawardana-K-G-S-H-Mendelev-M-I--Na except the fact that the latent heat of melting was purposely increased and the liquid was purposely made less ordered. The potentials were developed to study the effect of the latent heat and liquid structure on the SLI properties of bcc metals." Update 27 Apr. 2015: Changed the reference to update publication status.

    Related Models:
  • See Computed Properties
    Notes: This file was sent by M.I. Mendelev (Ames Laboratory) on 13 Jan. 2015 and posted with his permission. Update 19 July 2021: The contact email in the file's header has been changed. Update Jan 14 2022: Citation information has been updated in the file's header.
    File(s):
Date Created: October 5, 2010 | Last updated: August 12, 2026