Calculation update! New properties have been added to the website for dislocation monopole core structures, dynamic relaxes of both crystal and liquid phases, and melting temperatures! Currently, the results for these properties predominately focus on EAM-style potentials, but the results will be updated for other potentials as the associated calculations finish. Feel free to give us feedback on the new properties so we can improve their representations as needed.
Warning! Note that elemental potentials taken from alloy descriptions may not work well for the pure species. This is particularly true if the elements were fit for compounds instead of being optimized separately. As with all interatomic potentials, please check to make sure that the performance is adequate for your problem.
Citation: H. Sharifi, and C.D. Wick (2025), "Developing interatomic potentials for complex concentrated alloys of Cu, Ti, Ni, Cr, Co, Al, Fe, and Mn", Computational Materials Science248, 113595. DOI: 10.1016/j.commatsci.2024.113595.
Abstract: Complex concentrated alloys (CCAs) are a new generation of metallic alloys composed of three or more principal elements with physical and mechanical properties that can be tuned by adjusting their compositions. The extensive compositional workspace of CCAs makes it impractical to perform a comprehensive search for a specific material property using experimental measurements. The use of computational methods can rapidly narrow down the search span, improving the efficiency of the design process. We carried out a high-throughput parameterization of modified embedded atom method (MEAM) interatomic potentials for combinations of Cu, Ti, Ni, Cr, Co, Al, Fe, and Mn using a genetic algorithm. Unary systems were parameterized based on DFT calculations and experimental results. MEAM potentials for 28 binary and 56 ternary combinations of the elements were parameterized to DFT results that were carried out with semi-automated frameworks. Specific attention was made to reproduce properties that impact compositional segregation, material strength, and mechanics.
Notes: This is a binary listing for the 2025--Sharifi-H-Wick-C-D--Fe-Mn-Ni-Ti-Cu-Cr-Co-Al potential. This potential focuses on the structural analysis of alloys including shear strength and elastic constants, dislocation dynamics and their impact on alloy strength, and the analysis of defect effects, such as voids, on material properties. However, the potential was not optimized for temperature-dependent properties and was not fit to density, thermal expansion coefficients, or thermal conductivity data.
Citation: L.K. Béland, C. Lu, Y.N. Osetskiy, G.D. Samolyuk, A. Caro, L. Wang, and R.E. Stoller (2016), "Features of primary damage by high energy displacement cascades in concentrated Ni-based alloys", Journal of Applied Physics119(8), 085901. DOI: 10.1063/1.4942533.
Abstract: Alloying of Ni with Fe or Co has been shown to reduce primary damage production under ion irradiation. Similar results have been obtained from classical molecular dynamics simulations of 1, 10, 20, and 40 keV collision cascades in Ni, NiFe, and NiCo. In all cases, a mix of imperfect stacking fault tetrahedra, faulted loops with a 1/3⟨111⟩ Burgers vector, and glissile interstitial loops with a 1/2⟨110⟩ Burgers vector were formed, along with small sessile point defect complexes and clusters. Primary damage reduction occurs by three mechanisms. First, Ni-Co, Ni-Fe, Co-Co, and Fe-Fe short-distance repulsive interactions are stiffer than Ni-Ni interactions, which lead to a decrease in damage formation during the transition from the supersonic ballistic regime to the sonic regime. This largely controls final defect production. Second, alloying decreases thermal conductivity, leading to a longer thermal spike lifetime. The associated annealing reduces final damage production. These two mechanisms are especially important at cascades energies less than 40 keV. Third, at the higher energies, the production of large defect clusters by subcascades is inhibited in the alloys. A number of challenges and limitations pertaining to predictive atomistic modeling of alloys under high-energy particle irradiation are discussed.
Notes: Prof. Beland notes that "The potential takes elemental Ni from 2004--Mishin-Y--Ni-Al and Co from 2012--Purja-Pun-G-P-Mishin-Y--Co and mixes them. We first applied the effective gauge transformation, and then fitted the cross-term as to reproduce the heat of mixing of Ni(x)-Co(1-x). The potential is very soft at short distances. In order to perform collision cascades, it should be overlaid to the ZBL potential, with an outer cutoff of 2.0 Angstroms."
See Computed Properties Notes: This file was provided by Laurent Béland on 7 Nov 2019 and posted with his permission. Note: The EAM potential by itself is very soft at short distances. In order to perform collision cascades, use the hybrid style listed below. File(s):
See Computed Properties Notes: The eam file was provided by Laurent Béland on 7 Nov 2019 and posted with his permission. It is the same eam/alloy file as the above implementation. example.lammps.in provides an example of how to call the potential with the ZBL overlay applied. File(s):
Citation: Y.-K. Kim, W.-S. Jung, and B.-J. Lee (2015), "Modified embedded-atom method interatomic potentials for the Ni-Co binary and the Ni-Al-Co ternary systems", Modelling and Simulation in Materials Science and Engineering23(5), 055004. DOI: 10.1088/0965-0393/23/5/055004.
Abstract: Interatomic potentials for the Ni-Co binary and Ni-Al-Co ternary systems have been developed on the basis of the second nearest-neighbor modified embedded-atom method (2NN MEAM) formalism. The potentials describe structural, thermodynamic, deformation and defect properties of solid solution phases or compound phases in reasonable agreements with experiments or first-principles calculations. The results demonstrate the transferability of the potentials and their applicability to large-scale atomistic simulations to investigate the effect of an alloying element, cobalt, on various microstructural factors related to mechanical properties of Ni-based superalloys on an atomic scale.
Citation: G.P. Purja Pun, V. Yamakov, and Y. Mishin (2015), "Interatomic potential for the ternary Ni–Al–Co system and application to atomistic modeling of the B2–L10 martensitic transformation", Modelling and Simulation in Materials Science and Engineering23(6), 065006. DOI: 10.1088/0965-0393/23/6/065006.
Abstract: Ni–Al–Co is a promising system for ferromagnetic shape memory applications. This paper reports on the development of a ternary embedded-atom potential for this system by fitting to experimental and first-principles data. Reasonably good agreement is achieved for physical properties between values predicted by the potential and values known from experiment and/or first-principles calculations. The potential reproduces basic features of the martensitic phase transformation from the B2-ordered high-temperature phase to a tetragonal CuAu-ordered low-temperature phase. The compositional and temperature ranges of this transformation and the martensite microstructure predicted by the potential compare well with existing experimental data. These results indicate that the proposed potential can be used for simulations of the shape memory effect in the Ni–Al–Co system.
Notes: The reference information was updated on 26 Aug. 2015.
See Computed Properties Notes: This file was sent by Y. Mishin (George Mason Univ.) on 17 Sept. 2013 and was posted on 17 Jan. 2014. This version is compatible with LAMMPS. Validation and usage information can be found in Mishin-Ni-Co-2013_lammps.pdf. File(s): superseded
See Computed Properties Notes: This file was sent by G Purja Pun (George Mason Univ.) on 12 Oct. 2015 and was posted on 15 Dec. 2015. This version corrects an issue with the cutoff distance for Co interactions that was discovered during calculations of pressure dependent elastic constants. File(s):
See Computed Properties Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2015--Purja-Pun-G-P--Ni-Co--LAMMPS--ipr2. Link(s):