• Citation: K. Ito, T. Yokoi, K. Hyodo, and H. Mori (2024), "Machine learning interatomic potential with DFT accuracy for general grain boundaries in α-Fe", npj Computational Materials, 10(1), 255. DOI: 10.1038/s41524-024-01451-y.
    Abstract: To advance the development of high-strength polycrystalline metallic materials towards achieving carbon neutrality, it is essential to design materials in which the atomic level control of general grain boundaries (GGBs), which govern the material properties, is achieved. However, owing to the complex and diverse structures of GGBs, there have been no reports on interatomic potentials capable of reproducing them. This accuracy is essential for conducting molecular dynamics analyses to derive material design guidelines. In this study, we constructed a machine learning interatomic potential (MLIP) with density functional theory (DFT) accuracy to model the energy, atomic structure, and dynamics of arbitrary grain boundaries (GBs), including GGBs, in α-Fe. Specifically, we employed a training dataset comprising diverse atomic structures generated based on crystal space groups. The GGB accuracy was evaluated by directly comparing with DFT calculations performed on cells cut near GBs from nano-polycrystals, and extrapolation grades of the local atomic environment based on active learning methods for the entire nano-polycrystal. Furthermore, we analyzed the GB energy and atomic structure in α-Fe polycrystals through large-scale molecular dynamics analysis using the constructed MLIP. The average GB energy of α-Fe polycrystals calculated by the constructed MLIP is 1.57 J/m2, exhibiting good agreement with experimental predictions. Our findings demonstrate the methodology for constructing an MLIP capable of representing GGBs with high accuracy, thereby paving the way for materials design based on computational materials science for polycrystalline materials.

    Notes: This listing is for the level 16 MTP potential described in the articles's supplementary material. Note that the results in the main article are for the level 22 potential.

  • LAMMPS pair_style user-mlip (custom) (2024--Ito-K--Fe-16--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Kazuma Ito on November 14, 2024.
    File(s): Link(s):
  • Citation: K. Ito, T. Yokoi, K. Hyodo, and H. Mori (2024), "Machine learning interatomic potential with DFT accuracy for general grain boundaries in α-Fe", npj Computational Materials, 10(1), 255. DOI: 10.1038/s41524-024-01451-y.
    Abstract: To advance the development of high-strength polycrystalline metallic materials towards achieving carbon neutrality, it is essential to design materials in which the atomic level control of general grain boundaries (GGBs), which govern the material properties, is achieved. However, owing to the complex and diverse structures of GGBs, there have been no reports on interatomic potentials capable of reproducing them. This accuracy is essential for conducting molecular dynamics analyses to derive material design guidelines. In this study, we constructed a machine learning interatomic potential (MLIP) with density functional theory (DFT) accuracy to model the energy, atomic structure, and dynamics of arbitrary grain boundaries (GBs), including GGBs, in α-Fe. Specifically, we employed a training dataset comprising diverse atomic structures generated based on crystal space groups. The GGB accuracy was evaluated by directly comparing with DFT calculations performed on cells cut near GBs from nano-polycrystals, and extrapolation grades of the local atomic environment based on active learning methods for the entire nano-polycrystal. Furthermore, we analyzed the GB energy and atomic structure in α-Fe polycrystals through large-scale molecular dynamics analysis using the constructed MLIP. The average GB energy of α-Fe polycrystals calculated by the constructed MLIP is 1.57 J/m2, exhibiting good agreement with experimental predictions. Our findings demonstrate the methodology for constructing an MLIP capable of representing GGBs with high accuracy, thereby paving the way for materials design based on computational materials science for polycrystalline materials.

    Notes: This listing is for the level 18 MTP potential described in the articles's supplementary material. Note that the results in the main article are for the level 22 potential.

  • LAMMPS pair_style user-mlip (custom) (2024--Ito-K--Fe-18--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Kazuma Ito on November 14, 2024.
    File(s): Link(s):
  • Citation: K. Ito, T. Yokoi, K. Hyodo, and H. Mori (2024), "Machine learning interatomic potential with DFT accuracy for general grain boundaries in α-Fe", npj Computational Materials, 10(1), 255. DOI: 10.1038/s41524-024-01451-y.
    Abstract: To advance the development of high-strength polycrystalline metallic materials towards achieving carbon neutrality, it is essential to design materials in which the atomic level control of general grain boundaries (GGBs), which govern the material properties, is achieved. However, owing to the complex and diverse structures of GGBs, there have been no reports on interatomic potentials capable of reproducing them. This accuracy is essential for conducting molecular dynamics analyses to derive material design guidelines. In this study, we constructed a machine learning interatomic potential (MLIP) with density functional theory (DFT) accuracy to model the energy, atomic structure, and dynamics of arbitrary grain boundaries (GBs), including GGBs, in α-Fe. Specifically, we employed a training dataset comprising diverse atomic structures generated based on crystal space groups. The GGB accuracy was evaluated by directly comparing with DFT calculations performed on cells cut near GBs from nano-polycrystals, and extrapolation grades of the local atomic environment based on active learning methods for the entire nano-polycrystal. Furthermore, we analyzed the GB energy and atomic structure in α-Fe polycrystals through large-scale molecular dynamics analysis using the constructed MLIP. The average GB energy of α-Fe polycrystals calculated by the constructed MLIP is 1.57 J/m2, exhibiting good agreement with experimental predictions. Our findings demonstrate the methodology for constructing an MLIP capable of representing GGBs with high accuracy, thereby paving the way for materials design based on computational materials science for polycrystalline materials.

    Notes: This listing is for the level 20 MTP potential described in the articles's supplementary material. Note that the results in the main article are for the level 22 potential.

  • LAMMPS pair_style user-mlip (custom) (2024--Ito-K--Fe-20--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Kazuma Ito on November 14, 2024.
    File(s): Link(s):
  • Citation: K. Ito, T. Yokoi, K. Hyodo, and H. Mori (2024), "Machine learning interatomic potential with DFT accuracy for general grain boundaries in α-Fe", npj Computational Materials, 10(1), 255. DOI: 10.1038/s41524-024-01451-y.
    Abstract: To advance the development of high-strength polycrystalline metallic materials towards achieving carbon neutrality, it is essential to design materials in which the atomic level control of general grain boundaries (GGBs), which govern the material properties, is achieved. However, owing to the complex and diverse structures of GGBs, there have been no reports on interatomic potentials capable of reproducing them. This accuracy is essential for conducting molecular dynamics analyses to derive material design guidelines. In this study, we constructed a machine learning interatomic potential (MLIP) with density functional theory (DFT) accuracy to model the energy, atomic structure, and dynamics of arbitrary grain boundaries (GBs), including GGBs, in α-Fe. Specifically, we employed a training dataset comprising diverse atomic structures generated based on crystal space groups. The GGB accuracy was evaluated by directly comparing with DFT calculations performed on cells cut near GBs from nano-polycrystals, and extrapolation grades of the local atomic environment based on active learning methods for the entire nano-polycrystal. Furthermore, we analyzed the GB energy and atomic structure in α-Fe polycrystals through large-scale molecular dynamics analysis using the constructed MLIP. The average GB energy of α-Fe polycrystals calculated by the constructed MLIP is 1.57 J/m2, exhibiting good agreement with experimental predictions. Our findings demonstrate the methodology for constructing an MLIP capable of representing GGBs with high accuracy, thereby paving the way for materials design based on computational materials science for polycrystalline materials.
    Citation: K. Ito, T. Yokoi, K. Hyodo, and H. Mori (2024), "Grain Size Effects on the Deformation of α-Fe Nanopolycrystals: Massively Large-Scale Molecular Dynamics Simulations Using Machine Learning Interatomic Potential", . DOI: 10.2139/ssrn.5029355.
    Abstract: To improve the mechanical properties of polycrystalline metallic materials, understanding the elementary processes involved in their deformation at the atomic level is crucial. In this study, firstly, we evaluate the transferability of the recently proposed α-Fe machine-learning interatomic potential (MLIP), constructed from mechanically generated training data based on crystal space groups, to the tensile deformation process of nanopolycrystals. The transferability was evaluated by comparing the physical properties and lattice defect formation energies, which are important in the deformation behavior of nanopolycrystals, with those obtained from density functional theory (DFT) and by comprehensively calculating extrapolation grades based on active learning methods for the local atomic environment in the nanopolycrystal during tensile deformation. These evaluations demonstrate the superior transferability of the MLIP to the tensile deformation of the nanopolycrystals. Furthermore, large-scale molecular dynamics calculations were performed using the MLIP and the most commonly used embedded atom method (EAM) potential to investigate the effect of grain size on the deformation behavior of α-Fe polycrystals and the effect of interatomic potentials on them. The uniaxial tensile deformation behavior of the nanopolycrystals obtained from EAM was qualitatively consistent with that obtained from MLIP. This result supports the results of many studies conducted using EAM and is an important conclusion considering the high computational cost of the MLIP. Furthermore, the construction method for the MLIP used in this study is applicable to other metals. Therefore, this study considerably contributes to the understanding and material design of various metallic materials through the construction of highly accurate MLIPs.

    Notes: This listing is for the level 22 MTP potential, which is the version of the potential described in the journal articles. It has been tested for exploring grain boundary structures, and deformation mechanisms of polycrystals, including the generation and evolution of dislocations, twins, and cracks.

  • LAMMPS pair_style user-mlip (custom) (2024--Ito-K--Fe-22--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Kazuma Ito on November 14, 2024.
    File(s): Link(s):
  • Citation: R. Jana, and M.A. Caro (2023), "Searching for iron nanoparticles with a general-purpose Gaussian approximation potential", Physical Review B, 107(24), . DOI: 10.1103/physrevb.107.245421.
    Abstract: We present a general-purpose machine learning Gaussian approximation potential (GAP) for iron that is applicable to all bulk crystal structures found experimentally under diverse thermodynamic conditions, as well as surfaces and nanoparticles (NPs). By studying its phase diagram, we show that our GAP remains stable at extreme conditions, including those found in the Earth's core. The new GAP is particularly accurate for the description of NPs. We use it to identify new low-energy NPs, whose stability is verified by performing density functional theory calculations on the GAP structures. Many of these NPs are lower in energy than those previously available in the literature up to Natoms = 100. We further extend the convex hull of available stable structures to Natoms = 200. For these NPs, we study characteristic surface atomic motifs using data clustering and low-dimensional embedding techniques. With a few exceptions, e.g., at magic numbers Natoms = 59, 65, 76, and 78, we find that iron tends to form irregularly shaped NPs without a dominant surface character or characteristic atomic motif, and no reminiscence of crystalline features. We hypothesize that the observed disorder stems from an intricate balance and competition between the stable bulk motif formation, with bcc structure, and the stable surface motif formation, with fcc structure. We expect these results to improve our understanding of the fundamental properties and structure of low-dimensional forms of iron and to facilitate future work in the field of iron-based catalysis.

    Notes: Richard Jana notes that "This potential is suitable for a wide range of applications and structures, so we consider it general purpose. However, it is particularly intended for Fe nano particles."

  • Citation: Y. Sun, F. Zhang, M.I. Mendelev, R.M. Wentzcovitch, and K.-M. Ho (2022), "Two-step nucleation of the Earth's inner core", Proceedings of the National Academy of Sciences, 119(2), e2113059119. DOI: 10.1073/pnas.2113059119.
    Abstract: The Earth's inner core started forming when molten iron cooled below the melting point. However, the nucleation mechanism, which is a necessary step of crystallization, has not been well understood. Recent studies have found that it requires an unrealistic degree of undercooling to nucleate the stable, hexagonal, close-packed (hcp) phase of iron that is unlikely to be reached under core conditions and age. This contradiction is referred to as the inner core nucleation paradox. Using a persistent embryo method and molecular dynamics simulations, we demonstrate that the metastable, body-centered, cubic (bcc) phase of iron has a much higher nucleation rate than does the hcp phase under inner core conditions. Thus, the bcc nucleation is likely to be the first step of inner core formation, instead of direct nucleation of the hcp phase. This mechanism reduces the required undercooling of iron nucleation, which provides a key factor in solving the inner core nucleation paradox. The two-step nucleation scenario of the inner core also opens an avenue for understanding the structure and anisotropy of the present inner core.

    Notes: This potential was developed to simulate the solidification of Fe under the Earth's inner core conditions. Update Jan 12 2022: Citation information added and id updated from 2021--Mendelev-M-I--Fe.

  • LAMMPS pair_style eam/fs (2022--Sun-Y--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Mikhail Mendelev on July 15, 2021 and posted with his permission. Update Jan 14 2022: Citation information has been updated in the file's header.
    File(s):
  • Citation: S. Starikov, D. Smirnova, T. Pradhan, Y. Lysogorskiy, H. Chapman, M. Mrovec, and R. Drautz (2021), "Angular-dependent interatomic potential for large-scale atomistic simulation of iron: Development and comprehensive comparison with existing interatomic models", Physical Review Materials, 5(6), 063607. DOI: 10.1103/physrevmaterials.5.063607.
    Abstract: The development of classical interatomic potential for iron is a quite demanding task with a long history background. A new interatomic potential for simulation of iron was created with a focus on description of crystal defects properties. In contrast with previous studies, here the potential development was based on force-matching method that requires only ab initio data as reference values. To verify our model, we studied various features of body-centered-cubic iron including the properties of point defects (vacancy and self-interstitial atom), the Peierls energy barrier for dislocations (screw and mix types), and the formation energies of planar defects (surfaces, grain boundaries, and stacking fault). The verification also implies thorough comparison of a potential with 11 other interatomic potentials reported in literature. This potential correctly reproduces the largest number of iron characteristics which ensures its advantage and wider applicability range compared to the other considered classical potentials. Here application of the model is illustrated by estimation of self-diffusion coefficients and the calculation of fcc lattice properties at high temperature.

    Related Models:
  • See Computed Properties
    Notes: This file was provided by Sergei Starikov (ICAMS) on July 1, 2021 and posted with his permission. This file also contains the developed potential for simulation of non-magnetic iron (nmFe) that may be used in spin-dynamics simulation. Update Jan 10 2022: This version was identified to have issues with the non-magnetic iron model, which the version below fixes.
    File(s): superseded


  • See Computed Properties
    Notes: This file was provided by Sergei Starikov on Jan 10, 2022 and posted with his permission. In addition to Fe potential, this file also contains the modified version of the potential for simulation of non-magnetic iron (nmFe) that may be used in spin-dynamics simulation. The previous version of nmFe (above) poorly describes the crystal structures with low density. As such, the diamond lattice incorrectly had energy lower than fcc structure. This version fixes the bug by a slight change of the embedded function for nmFe in the low density region.
    File(s):
  • Citation: J. Byggmästar, and F. Granberg (2020), "Dynamical stability of radiation-induced C15 clusters in iron", Journal of Nuclear Materials, 528, 151893. DOI: 10.1016/j.jnucmat.2019.151893.
    Abstract: Density functional theory predicts clusters in the form of the C15 Laves phase to be the most stable cluster of self-interstitials in iron at small sizes. The C15 clusters can form as a result of irradiation, but their prevalence and survival in harsh irradiation conditions have not been thoroughly studied. Using a new bond-order potential optimised for molecular dynamics simulations of radiation damage, we explore the dynamical stability of the C15 clusters in iron under irradiation conditions. We find that small C15 clusters make up 5–20% of the interstitial clusters formed directly in cascades. In continuous irradiation, C15 clusters are frequently formed, after which they remain highly stable and grow by absorbing nearby single interstitial atoms. Growth of C15 clusters ultimately leads to collapse into dislocation loops, most frequently into 1/2 <111> loops and only rarely collapsing into <100> loops at low temperatures. The population, size, and collapse of C15 clusters during continuous irradiation correlates well with their formation energies relative to dislocation loops calculated at zero Kelvin.

    Notes: Jesper Byggmästar notes that "This potential was developed mainly for defect clusters and radiation damage. See also the supplementary pdf of the above paper (open access) for benchmark results."

    Related Models:
  • LAMMPS pair_style tersoff/zbl (2020--Byggmastar-J--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Jesper Byggmästar (University of Helsinki) on 11 Dec 2019.
    File(s):
  • Citation: H. Mori, and T. Ozaki (2020), "Neural network atomic potential to investigate the dislocation dynamics in bcc iron", Physical Review Materials, 4(4), 040601. DOI: 10.1103/physrevmaterials.4.040601.
    Abstract: To design the mechanical strength of body-centered-cubic (bcc) iron, clarifying the dislocation dynamics is very important. Using systematically constructed reference data based on density functional theory (DFT) calculations, we construct an atomic artificial neural network (ANN) potential to investigate the dislocation dynamics in bcc iron with the accuracy of DFT calculations. The bulk properties and defect formation energies predicted by the constructed ANN potential are in good agreement with the reference DFT calculations. The a0/2⟨111⟩110 screw dislocation core structure predicted by the ANN potential is compact and nondegenerate. The Peierls barrier predicted by the ANN potential is 35.3 meV per length of the Burgers vector. These results are consistent with the DFT results. Furthermore, not only the Peierls barrier, but also the two-dimensional energy profile of the screw dislocation core position predicted by the ANN potential are in excellent agreement with the DFT results. These results clearly demonstrate the reproducibility and transferability of the constructed ANN potential for investigating dislocation dynamics with the accuracy of the DFT. Combined with advanced atomistic techniques, the ANN potential will be highly useful for investigating the dislocation dynamics in bcc iron at finite temperatures.

    Related Models:
  • LAMMPS pair_style aenet (custom) (2020--Mori-H--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: These files were sent by Hideki Mori (College of Industrial Technology, Japan) on 13 July 2020 and posted with his permission. This package provides the parameter file of the artificial neural network (ANN) potential for BCC iron, LAMMPS module for the ANN potential and the patch of aenet for the LAMMPS library. See the included readme file for instructions on installing aenet and incorporating it with LAMMPS. The included pair style patch is also available at https://github.com/HidekiMori-CIT/aenet-lammps.
    File(s):
  • Citation: S.A. Etesami, and E. Asadi (2018), "Molecular dynamics for near melting temperatures simulations of metals using modified embedded-atom method", Journal of Physics and Chemistry of Solids, 112, 61-72. DOI: 10.1016/j.jpcs.2017.09.001.
    Abstract: Availability of a reliable interatomic potential is one of the major challenges in utilizing molecular dynamics (MD) for simulations of metals at near the melting temperatures and melting point (MP). Here, we propose a novel approach to address this challenge in the concept of modified-embedded-atom (MEAM) interatomic potential; also, we apply the approach on iron, nickel, copper, and aluminum as case studies. We propose adding experimentally available high temperature elastic constants and MP of the element to the list of typical low temperature properties used for the development of MD interatomic potential parameters. We show that the proposed approach results in a reasonable agreement between the MD calculations of melting properties such as latent heat, expansion in melting, liquid structure factor, and solid-liquid interface stiffness and their experimental/computational counterparts. Then, we present the physical properties of mentioned elements near melting temperatures using the new MEAM parameters. We observe that the behavior of elastic constants, heat capacity and thermal linear expansion coefficient at room temperature compared to MP follows an empirical linear relation (α±β × MP) for transition metals. Furthermore, a linear relation between the tetragonal shear modulus and the enthalpy change from room temperature to MP is observed for face-centered cubic materials.

    Notes: S. A. Etesami (University of Memphis) noted that "We added both melting point and high temperature elastic constants into material properties database for MEAM parameter development process."

    Related Models:
  • See Computed Properties
    Notes: These files were sent by S. A. Etesami (University of Memphis) on 23 April 2018 and posted with his permission. This version is compatible with LAMMPS.
    File(s):
  • Citation: E. Asadi, M. Asle Zaeem, S. Nouranian, and M.I. Baskes (2015), "Quantitative modeling of the equilibration of two-phase solid-liquid Fe by atomistic simulations on diffusive time scales", Physical Review B, 91(2), 024105. DOI: 10.1103/physrevb.91.024105.
    Abstract: In this paper, molecular dynamics (MD) simulations based on the modified-embedded atom method (MEAM) and a phase-field crystal (PFC) model are utilized to quantitatively investigate the solid-liquid properties of Fe. A set of second nearest-neighbor MEAM parameters for high-temperature applications are developed for Fe, and the solid-liquid coexisting approach is utilized in MD simulations to accurately calculate the melting point, expansion in melting, latent heat, and solid-liquid interface free energy, and surface anisotropy. The required input properties to determine the PFC model parameters, such as liquid structure factor and fluctuations of atoms in the solid, are also calculated from MD simulations. The PFC parameters are calculated utilizing an iterative procedure from the inputs of MD simulations. The solid-liquid interface free energy and surface anisotropy are calculated using the PFC simulations. Very good agreement is observed between the results of our calculations from MEAM-MD and PFC simulations and the available modeling and experimental results in the literature. As an application of the developed model, the grain boundary free energy of Fe is calculated using the PFC model and the results are compared against experiments.

    Notes: Prof. Mohsen Zaeem said that this potential was designed for accurately representing properties from 0K up to the melting point.

  • LAMMPS pair_style meam (2015--Asadi-E--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was sent by Prof. Mohsen Zaeem (Missouri S&T) on 12 April 2017 and posted on 5 May 2017. Update 5 Sept 2019: The 31 July 2018 update of the repository inadvertantly replaced the parameter files with those from the 2018--Etesami-S-A--Fe--LAMMPS--ipr1 potential. The links below now point to the correct files.
    File(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 Fe 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: L. Proville, D. Rodney, and M.-C. Marinica (2012), "Quantum effect on thermally activated glide of dislocations", Nature Materials, 11(10), 845-849. DOI: 10.1038/nmat3401.
    Abstract: Crystal plasticity involves the motion of dislocations under stress. So far, atomistic simulations of this process have predicted Peierls stresses, the stress needed to overcome the crystal resistance in the absence of thermal fluctuations, of more than twice the experimental values, a discrepancy best-known in body-centred cubic crystals. Here we show that a large contribution arises from the crystal zero-point vibrations, which ease dislocation motion below typically half the Debye temperature. Using Wigner’s quantum transition state theory in atomistic models of crystals, we found a large decrease of the kink-pair formation enthalpy due to the quantization of the crystal vibrational modes. Consequently, the flow stress predicted by Orowan’s law is strongly reduced when compared with its classical approximation and in much closer agreement with experiments. This work advocates that quantum mechanics should be accounted for in simulations of materials and not only at very low temperatures or in light-atom systems.

    Related Models:
  • LAMMPS pair_style eam/fs (2012--Proville-L--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was sent by M.-C. Marinica (CEA, France) on 10 January 2017 and posted with his permission.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2012--Proville-L--Fe--LAMMPS--ipr1.
    Link(s):
  • Citation: S. Chiesa, P.M. Derlet, S.L. Dudarev, and H.V. Swygenhoven (2011), "Optimization of the magnetic potential for α-Fe", Journal of Physics: Condensed Matter, 23(20), 206001. DOI: 10.1088/0953-8984/23/20/206001.
    Abstract: A second generation of empirical potentials is produced for α-Fe within the framework of the magnetic potential formalism (Dudarev and Derlet 2005 J. Phys.: Condens. Matter 17 7097). A materials database that, in addition to ab initio-derived point defect formation energies, now includes third-order elastic constant and ab initio-derived string potential data controlling, respectively, the thermal expansion properties and the core structure of the 1/2<111> screw dislocation. Three parameterizations are presented in detail, all of which exhibit positive thermal expansion and produce a non-degenerate configuration for the relaxed 1/2<111> screw dislocation easy core structure. These potentials, along with two other published potentials, are investigated in terms of defect formation volume, early stage dislocation loop clustering energetics, <110> dumbbell interstitial diffusion, and the zero-stress 1/2<111> screw dislocation Peierls barrier and its corresponding kink formation energies.

    Notes: This is for the ferromagnetic MP-CS3-33 model described in the reference.

    Related Models:
  • LAMMPS pair_style eam/alloy (2011--Chiesa-S--Fe-33--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Sergei Starikov (Ruhr-Universität Bochum, Germany) on 5 May 2019 and posted with permission from him, Dr. Dudarev and Dr. Derlet.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org.
    Link(s):
  • Citation: L. Malerba, M.C. Marinica, N. Anento, C. Björkas, H. Nguyen, C. Domain, F. Djurabekova, P. Olsson, K. Nordlund, A. Serra, D. Terentyev, F. Willaime, and C.S. Becquart (2010), "Comparison of empirical interatomic potentials for iron applied to radiation damage studies", Journal of Nuclear Materials, 406(1), 19-38. DOI: 10.1016/j.jnucmat.2010.05.017.
    Abstract: The performance of four recent semi-empirical interatomic potentials for iron, developed or used within the FP6 Perfect Project, is evaluated by comparing them between themselves and with available experimental or, more often, density functional theory data. The quantities chosen for the comparison are of specific interest for radiation damage studies, i.e. they concern mainly properties of point-defects and their clusters, as well as dislocations. For completeness, an earlier, widely used (also within the Project) iron potential is included in the comparison exercise as well. This exercise allows conclusions to be drawn about the reliability of the available potentials, while providing a snapshot of the state-of-the-art concerning fundamental properties of iron, thereby being also useful as a kind of handbook and as a framework for the validation of future semi-empirical interatomic potentials for iron. It is found that Mendelev-type potentials are currently the best choice in order to "extend density functional theory" to larger scales and this justifies their widespread use, also for the development of iron alloy potentials. However, a fully reliable description of self-interstitial atom clusters and dislocations with interatomic potentials remains largely an elusive objective, that calls for further effort within the concerned scientific community.
    Citation: M.-C. Marinica, F. Willaime, and J.-P. Crocombette (2012), "Irradiation-Induced Formation of Nanocrystallites with C15 Laves Phase Structure in bcc Iron", Physical Review Letters, 108(2), 025501. DOI: 10.1103/physrevlett.108.025501.
    Abstract: A three-dimensional periodic structure is proposed for self-interstitial clusters in body-centered-cubic metals, as opposed to the conventional two-dimensional loop morphology. The underlying crystal structure corresponds to the C15 Laves phase. Using density functional theory and interatomic potential calculations, we demonstrate that in α-iron these C15 aggregates are highly stable and immobile and that they exhibit large antiferromagnetic moments. They form directly in displacement cascades, and they can grow by capturing self-interstitials. They thus constitute an important new element to account for when predicting the microstructural evolution of iron base materials under irradiation.

    Notes: Dr. Marinica noted that this iron potential was developed by M.-C. Marinca in 2007. The potential uses EAM formalism and was fitted on a database point defect oriented. The performance of the potential is tested in the above 2010 reference. Someone using this potential should cite the above two papers.

    Related Models:
  • LAMMPS pair_style eam/fs (2010--Malerba-L--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was sent by M.-C. Marinica (CEA, France) on 10 January 2017 and posted with his permission.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2010--Malerba-L--Fe--LAMMPS--ipr1.
    Link(s):
  • Citation: P.A.T. Olsson (2009), "Semi-empirical atomistic study of point defect properties in BCC transition metals", Computational Materials Science, 47(1), 135-145. DOI: 10.1016/j.commatsci.2009.06.025.
    Abstract: We have constructed a set of embedded atom method (EAM) potentials for Fe, Ta, W and V and used them in order to study point defect properties. The parametrizations of the potentials ensure that the third order elastic constants are continuous and they have been fitted to the cohesive energies, the lattice constants, the unrelaxed vacancy formation energies and the second order elastic constants. Formation energies for different self-interstitials reveal that the <1 1 0> split dumbbell is the most stable configuration for Fe while for Ta, W and V we find that the <1 1 1> split dumbbell is preferred. Self-interstitial migration energies are simulated using the nudged elastic band method and for Fe and W the migration energies are found to be in good agreement with experimental and ab initio data. Migration energies for Ta and V self-interstitials are found to be quite low. The calculated formation, activation and migration energies for monovacancies are in good agreement with experimental data. Formation energies for divacancies reveal that the second nearest neighbor divacancy is more energetically favorable than nearest neighbor divacancies and the migration energies indicate that nearest neighbor migration paths are more likely to occur than second nearest neighbor migration jumps. For Fe, we have also studied the influence of the pair potential behavior between the second and third nearest neighbor on the stability of the <1 1 0> split dumbbell, which revealed that the higher the energy level of the pair potential is in that region, the more stable the <1 1 0> split dumbbell becomes.

    Related Models:
  • EAM tabulated functions (2009--Olsson-P-A-T--Fe--table--ipr1)
    Notes: These files were provided by Pär Olsson (Malmoe University, Sweden) on 11 November 2018 and posted with his permission.
    File(s):
    F(ρ): F_fe.plt
    ρ(r): rho_fe.plt
    φ(r): phi_fe.plt

  • LAMMPS pair_style eam/alloy (2009--Olsson-P-A-T--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Pär Olsson (Malmoe University, Sweden) on 11 November 2018 and posted with his permission.
    File(s):
  • Citation: J.R. Morris, R.S. Aga, V. Levashov, and T. Egami (2008), "Many-body effects in bcc metals: An embedded atom model extension of the modified Johnson pair potential for iron", Physical Review B, 77(17), 174201. DOI: 10.1103/physrevb.77.174201.
    Abstract: In this work, we generalize a many-body extension of pairwise interatomic potentials originally proposed by Baskes [Phys. Rev. Lett. 83, 2592 (1991)], in particular, showing how a pair potential interacting with multiple near neighbor shells may be extended to an embedded atom form without changing the cohesive energy or lattice constant. This is important for parametric studies of interatomic potentials, particularly how elastic constants affect other properties. Specifically, we apply this to the modified Johnson potential, a pair potential for Fe that has been used extensively for understanding liquid and amorphous metals.

    Related Models:
  • See Computed Properties
    Notes: Listing found at https://openkim.org.
    Link(s):
  • Citation: M. Müller, P. Erhart, and K. Albe (2007), "Analytic bond-order potential for bcc and fcc iron—comparison with established embedded-atom method potentials", Journal of Physics: Condensed Matter, 19(32), 326220. DOI: 10.1088/0953-8984/19/32/326220.
    Abstract: A new analytic bond-order potential for iron is presented that has been fitted to experimental data and results from first-principles calculations. The angular-dependent functional form allows a proper description of a large variety of bulk, surface and defect properties, including the Bain path, phonon dispersions, defect diffusivities and defect formation energies. By calculating Gibbs free energies of body-centred cubic (bcc) and face-centred cubic (fcc) iron as a function of temperature, we show that this potential is able to reproduce the transitions from α-iron to γ-iron and δ-iron before the melting point. The results are compared to four widely used embedded-atom-method potentials for iron.

    Related Models:
  • Citation: H. Chamati, N.I. Papanicolaou, Y. Mishin, and D.A. Papaconstantopoulos (2006), "Embedded-atom potential for Fe and its application to self-diffusion on Fe(100)", Surface Science, 600(9), 1793-1803. DOI: 10.1016/j.susc.2006.02.010.
    Abstract: We have constructed an embedded-atom potential for Fe by fitting to both experimental and first-principles results. The potential reproduces with satisfactory accuracy the lattice properties, surface energies and point defect energies for both BCC and the high temperature FCC phases of the metal. The potential was used in tandem with molecular-dynamics simulations to calculate the thermal expansion of both BCC-Fe and FCC-Fe, the phonon dispersion curves, mean-square displacements and surface relaxations of the element. In addition, we have studied self-diffusion of single adatoms on the BCC-Fe(1 0 0) surface at several temperatures. The migration energies and pre-exponential factors for three main diffusion mechanisms were determined and compared with available experimental data. We have found that the diagonal exchange diffusion process is energetically favored over the direct hopping mechanism and that its migration energy is close to the experimental value. Furthermore, the diffusion coefficient associated with the diagonal exchange diffusion process is about an order of magnitude higher than those of the hopping and the non-diagonal exchange mechanisms.

    Related Models:
  • EAM tabulated functions (2006--Chamati-H--Fe--table--ipr1)
    Notes: These files were provided by Yuri Mishin (George Mason University) and posted on 10 Dec. 2009.
    File(s):
    F(ρ): F_fe.plt
    ρ(r): ffe.plt
    φ(r): pfe.plt

  • LAMMPS pair_style eam/alloy (2006--Chamati-H--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: Professor Mishin provided a LAMMPS-compatible version of the potential, which was posted on 23 Aug. 2017.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2006--Chamati-H--Fe--LAMMPS--ipr1.
    Link(s):
  • Citation: S.L. Dudarev, and P.M. Derlet (2005), "A 'magnetic' interatomic potential for molecular dynamics simulations", Journal of Physics: Condensed Matter, 17(44), 7097-7118. DOI: 10.1088/0953-8984/17/44/003.
    Abstract: We develop a semi-empirical many-body interatomic potential suitable for large scale molecular dynamics simulations of magnetic α-iron. The functional form of the embedding part of the potential is derived using a combination of the Stoner and the Ginzburg–Landau models. We show that it is the symmetry broken solutions of the Ginzburg–Landau model describing spontaneous magnetization of atoms that provide the link between magnetism and interatomic forces. We discuss a range of potential applications of the new method.

    Related Models:
  • MoldyPSI (2005--Dudarev-S-L--Fe--MoldyPSI--ipr1)
    Notes: These files were provided by Peter Derlet (Paul Scherrer Institute) and posted with his permission on 2 July 2010. Usage information can be found in the FAQ.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org.
    Link(s):
  • Citation: X.W. Zhou, R.A. Johnson, and H.N.G. Wadley (2004), "Misfit-energy-increasing dislocations in vapor-deposited CoFe/NiFe multilayers", Physical Review B, 69(14), 144113. DOI: 10.1103/physrevb.69.144113.
    Abstract: Recent molecular dynamics simulations of the growth of [Ni0.8Fe0.2/Au] multilayers have revealed the formation of misfit-strain-reducing dislocation structures very similar to those observed experimentally. Here we report similar simulations showing the formation of edge dislocations near the interfaces of vapor-deposited (111) [NiFe/CoFe/Cu] multilayers. Unlike misfit dislocations that accommodate lattice mismatch, the dislocation structures observed here increase the mismatch strain energy. Stop-action observations of the dynamically evolving atomic structures indicate that during deposition on the (111) surface of a fcc lattice, adatoms may occupy either fcc sites or hcp sites. This results in the random formation of fcc and hcp domains, with dislocations at the domain boundaries. These dislocations enable atoms to undergo a shift from fcc to hcp sites, or vice versa. These shifts lead to missing atoms, and therefore a later deposited layer can have missing planes compared to a previously deposited layer. This dislocation formation mechanism can create tensile stress in fcc films. The probability that such dislocations are formed was found to quickly diminish under energetic deposition conditions.

    Related Models:
  • FORTRAN (2004--Zhou-X-W--Fe--FORTRAN--ipr1)
    Notes: These are the original files sent by X.W. Zhou (Sandia National Laboratory) and posted with his permission. C.A. Becker (NIST) modified create.f to include the reference in the generated potential files and the EAM.input file for this composition. These files can be used to generate alloy potentials for Cu, Ag, Au, Ni, Pd, Pt, Al, Pb, Fe, Mo, Ta, W, Mg, Co, Ti, and Zr by editing EAM.input. However, as addressed in the reference, these potentials were not designed for use with metal compounds.
    File(s): superseded


  • LAMMPS pair_style eam/alloy (2004--Zhou-X-W--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was generated by C.A. Becker (NIST) from create.f and posted with X.W. Zhou's (Sandia National Laboratory) permission.
    File(s): superseded


  • FORTRAN (2004--Zhou-X-W--Fe--FORTRAN--ipr2)
    Notes: The file Zhou04_create_v2.f is an updated version of create.f modified by L.M. Hale (NIST) following advice from X.W. Zhou (Sandia National Laboratory). This version removes spurious fluctuations in the tabulated functions of the original potential files caused by single/double precision floating point number conflicts.
    File(s):
  • LAMMPS pair_style eam/alloy (2004--Zhou-X-W--Fe--LAMMPS--ipr2)
    See Computed Properties
    Notes: This file was generated by L.M. Hale from Zhou04_create_v2.f on 13 April 2018 and posted with X.W. Zhou's (Sandia National Laboratory) permission. This version corrects an issue with spurious fluctuations in the tabulated functions.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2004--Zhou-X-W--Fe--LAMMPS--ipr1.
    Link(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2004--Zhou-X-W--Fe--LAMMPS--ipr2.
    Link(s):
  • Citation: M.I. Mendelev, S. Han, D.J. Srolovitz, G.J. Ackland, D.Y. Sun, and M. Asta (2003), "Development of new interatomic potentials appropriate for crystalline and liquid iron", Philosophical Magazine, 83(35), 3977-3994. DOI: 10.1080/14786430310001613264.
    Abstract: Two procedures were developed to fit interatomic potentials of the embedded-atom method (EAM) form and applied to determine a potential which describes crystalline and liquid iron. While both procedures use perfect crystal and crystal defect data, the first procedure also employs the first-principles forces in a model liquid and the second procedure uses experimental liquid structure factor data. These additional types of information were incorporated to ensure more reasonable descriptions of atomic interactions at small separations than is provided using standard approaches, such as fitting to the universal binding energy relation. The new potentials (provided herein) are, on average, in better agreement with the experimental or first-principles lattice parameter, elastic constants, point-defect energies, bcc–fcc transformation energy, liquid density, liquid structure factor, melting temperature and other properties than other existing EAM iron potentials.

    Notes: This listing is for the reference's Fe #5 interaction parameters.

    Related Models:
  • See Computed Properties
    Notes: This file was provided by Mikhail Mendelev on Jun 10, 2007. Update 19 July 2021: The contact email in the file's header has been changed.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2003--Mendelev-M-I--Fe-5--LAMMPS--ipr1.
    Link(s):
  • Citation: R. Meyer, and P. Entel (1998), "Martensite-austenite transition and phonon dispersion curves of Fe1-xNix studied by molecular-dynamics simulations", Physical Review B, 57(9), 5140-5147. DOI: 10.1103/physrevb.57.5140.
    Abstract: We have done molecular-dynamics simulations of Fe1−xNix employing a semiempirical model. We present a phase diagram of the martensite-austenite transition temperatures as a function of the Ni concentration which is in good agreement with experimental observations. In addition to this we have calculated the phonon dispersion curves of Fe and Ni from the model. Results show that the vibrational properties of the metals are well reproduced by the embedded-atom-method potentials. Finally, we have derived the phonon dispersion relations of bcc Fe80Ni20. We find rather low energies of the [110]−TA1 phonons with a strong temperature dependence which we attribute to instabilities of Ni in the bcc phase. We do not find any indications of a soft mode at the martensite-austenite transition in Fe1−xNix.

    Related Models:
  • LAMMPS pair_style eam (1998--Meyer-R--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Rodrigo Freitas (Stanford) on Jan 10, 2020. It was used for the publication R. Freitas, M. Asta and M. de Koning (2016) Computational Materials Science, 112, 333-341. DOI: 10.1016/j.commatsci.2015.10.050. Update March 13, 2020: The listed LAMMPS pair style corrected from eam/alloy to eam. Update Dec 11, 2020: Lucas Hale verified that the potential's tables are consistent with the parameters in the paper, however, the elastic constants differ by roughly 10% from the published values. The id for the implementation has been updated from 1998--Meyer-R--Fe--ipr-1 to 1998--Meyer-R--Fe--LAMMPS--ipr-1 for consistency.
    File(s):
  • Citation: G.J. Ackland, D.J. Bacon, A.F. Calder, and T. Harry (1997), "Computer simulation of point defect properties in dilute Fe-Cu alloy using a many-body interatomic potential", Philosophical Magazine A, 75(3), 713-732. DOI: 10.1080/01418619708207198.
    Abstract: The behaviour of copper atoms in dilute solution in α-iron is important for the microstructural changes that occur in ferritic pressure vessel steels under fastneutron irradiation. To investigate the properties of atomic defects that control this behaviour, a set of many-body interatomic potentials has been developed for the Fe—Cu system. The procedures employed, including modifications to ensure suitability for simulating atomic collisions at high energy, are described. The effect of copper on the lattice parameter of iron in the new model is in good agreement with experiment. The phonon properties of the pure crystals and, in particular, the influence of the instability of the metastable, bcc phase of copper that precipitates during irradiation are discussed. The properties of point defects have been investigated. It is found that the vacancy has lower formation and migration energy in bcc copper than in α-iron, and the self-interstitial atom has very low formation energy in this phase of copper. The threshold displacement energy in iron has been computed as a function of recoil orientation for both iron-and copper-atom recoils. The differences between the energy for the two species are small.

    Related Models:
  • Moldy FS (1997--Ackland-G-J--Fe--MOLDY--ipr1)
    Notes: The parameters in Fe.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 (1997--Ackland-G-J--Fe--LAMMPS--ipr1)
    See Computed Properties
    Notes: This conversion was performed from G.J. Ackland's parameters by M.I. Mendelev. Conversion checks from M.I. Mendelev can be found in conversion_check.pdf. These files were posted on 30 June 2009 with the permission of G.J. Ackland and M.I. Mendelev. These potentials are not designed for simulations of radiation damage. Update 19 July 2021: The contact email in the file's header has been changed.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 1997--Ackland-G-J--Fe--LAMMPS--ipr1.
    Link(s):
 
  • Citation: X.W. Zhou, R.A. Johnson, and H.N.G. Wadley (2004), "Misfit-energy-increasing dislocations in vapor-deposited CoFe/NiFe multilayers", Physical Review B, 69(14), 144113. DOI: 10.1103/physrevb.69.144113.
    Abstract: Recent molecular dynamics simulations of the growth of [Ni0.8Fe0.2/Au] multilayers have revealed the formation of misfit-strain-reducing dislocation structures very similar to those observed experimentally. Here we report similar simulations showing the formation of edge dislocations near the interfaces of vapor-deposited (111) [NiFe/CoFe/Cu] multilayers. Unlike misfit dislocations that accommodate lattice mismatch, the dislocation structures observed here increase the mismatch strain energy. Stop-action observations of the dynamically evolving atomic structures indicate that during deposition on the (111) surface of a fcc lattice, adatoms may occupy either fcc sites or hcp sites. This results in the random formation of fcc and hcp domains, with dislocations at the domain boundaries. These dislocations enable atoms to undergo a shift from fcc to hcp sites, or vice versa. These shifts lead to missing atoms, and therefore a later deposited layer can have missing planes compared to a previously deposited layer. This dislocation formation mechanism can create tensile stress in fcc films. The probability that such dislocations are formed was found to quickly diminish under energetic deposition conditions.

    Notes: This is a combined potential that contains all 16 elements from the source reference. It is provided here due to various requests for more elemental combinations often for high entropy simulations. As a caution, note that all of the cross interactions are determined through a universal mixing function and that most elemental systems were not thoroughly explored and tested by the original authors meaning that most binary and higher-order systems may not be well optimized.

  • See Computed Properties
    Notes: This file was generated by Ilia Nikiforov using the Zhou04_create_v2.f FORTRAN code which can be found on the associated elemental listings. The code was slightly modified to increase the tabulation points to 3000 to ensure good interpolations of the embedding energy function for all elements as W has a noticeably larger delta rho than the other elements. Also, the header was fixed to include all 16 element symbol tags.
    File(s):
 
 
 
 
 
 
  • Citation: B. Jelinek, S. Groh, M.F. Horstemeyer, J. Houze, S.G. Kim, G.J. Wagner, A. Moitra, and M.I. Baskes (2012), "Modified embedded atom method potential for Al, Si, Mg, Cu, and Fe alloys", Physical Review B, 85(24), 245102. DOI: 10.1103/physrevb.85.245102.
    Abstract: A set of modified embedded-atom method (MEAM) potentials for the interactions between Al, Si, Mg, Cu, and Fe was developed from a combination of each element's MEAM potential in order to study metal alloying. Previously published MEAM parameters of single elements have been improved for better agreement to the generalized stacking fault energy (GSFE) curves when compared with ab initio generated GSFE curves. The MEAM parameters for element pairs were constructed based on the structural and elastic properties of element pairs in the NaCl reference structure garnered from ab initio calculations, with adjustment to reproduce the ab initio heat of formation of the most stable binary compounds. The new MEAM potentials were validated by comparing the formation energies of defects, equilibrium volumes, elastic moduli, and heat of formation for several binary compounds with ab initio simulations and experiments. Single elements in their ground-state crystal structure were subjected to heating to test the potentials at elevated temperatures. An Al potential was modified to avoid formation of an unphysical solid structure at high temperatures. The thermal expansion coefficient of a compound with the composition of AA 6061 alloy was evaluated and compared with experimental values. MEAM potential tests performed in this work, utilizing the universal atomistic simulation environment (ASE), are distributed to facilitate reproducibility of the results.

    Related Models:
  • See Computed Properties
    Notes: This file was sent by Bohumir Jelinek (Mississippi State University) and posted on 3 July 2012. He noted, "This is a MEAM potential for Al, Si, Mg, Cu, Fe alloys. It works with LAMMPS, version 19 Jul 2011 or later, when compiled with MEAM support. Most of the MEAM potential results presented in the accompanying paper can be reproduced with Atomistic Simulation Environment (ASE) and testing routines are provided in ase-atomistic-potential-tests-rev60.tar.gz"
    File(s):
 
  • Citation: A. Mahata, T. Mukhopadhyay, and M. Asle Zaeem (2022), "Modified embedded-atom method interatomic potentials for Al-Cu, Al-Fe and Al-Ni binary alloys: From room temperature to melting point", Computational Materials Science, 201, 110902. DOI: 10.1016/j.commatsci.2021.110902.
    Abstract: Second nearest neighbor modified embedded-atom method (2NN-MEAM) interatomic potentials are developed for binary aluminum (Al) alloys applicable from room temperature to the melting point. The binary alloys studied in this work are Al-Cu, Al-Fe and Al-Ni. Sensitivity and uncertainty analyses are performed on potential parameters based on the perturbation approach. The outcome of the sensitivity analysis shows that some of the MEAM parameters interdependently influence all MEAM model outputs, allowing for the definition of an ordered calibration procedure to target specific MEAM outputs. Using these 2NN-MEAM interatomic potentials, molecular dynamics (MD) simulations are performed to calculate low and high-temperature properties, such as the formation energies of stable phases and unstable intermetallics, lattice parameters, elastic constants, thermal expansion coefficients, enthalpy of formation of solids, liquid mixing enthalpy, and liquidus temperatures at a wide range of compositions. The computed data are compared with the available first principle calculations and experimental data, showing high accuracy of the 2NN-MEAM interatomic potentials. In addition, the liquidus temperature of the Al binary alloys is compared to the phase diagrams determined by the CALPHAD method.

  • See Computed Properties
    Notes: These files were provided by Mohsen Asle Zaeem on Oct 8, 2021 and posted with his permission.
    File(s):
 
 
 
 
 
  • Citation: F.-S. Meng, S. Shinzato, S. Zhang, K. Matsubara, J.-P. Du, P. Yu, W.-T. Geng, and S. Ogata (2024), "A highly transferable and efficient machine learning interatomic potentials study of α-Fe–C binary system", Acta Materialia, 281, 120408. DOI: 10.1016/j.actamat.2024.120408.
    Abstract: Machine learning interatomic potentials (MLIPs) for α-iron and carbon binary system have been constructed aiming for understanding the mechanical behavior of Fe–C steel and carbides. The MLIPs were trained using an extensive reference database produced by spin polarized density functional theory (DFT) calculations. The MLIPs reach the DFT accuracies in many important properties which are frequently engaged in Fe and Fe–C studies, including kinetics and thermodynamics of C in α-Fe with vacancy, grain boundary, and screw dislocation, and basic properties of cementite and cementite–ferrite interfaces. In conjunction with these MLIPs, the impact of C atoms on the mobility of screw dislocation at finite temperature, and the C-decorated core configuration of screw dislocation were investigated, and a uniaxial tensile test on a model with multiple types of defects was conducted.

    Notes: This entry is for the BNNP potential in the reference that was trained using the n2p2 package. BNNP shows better overall accuracy, and DP shows advantages in the atomic stress computation. These potentials can be used to simulate 𝛼-Fe-C systems and pure 𝛼-Fe systems, but these potentials should not be used for pure C system.

  • See Computed Properties
    Notes: These files were provided by Fan-Shun Meng on October 22, 2024. Detailed instructions on using these potentials in MD simulations can be found at the link below.
    File(s): Link(s):
  • Citation: F.-S. Meng, S. Shinzato, S. Zhang, K. Matsubara, J.-P. Du, P. Yu, W.-T. Geng, and S. Ogata (2024), "A highly transferable and efficient machine learning interatomic potentials study of α-Fe–C binary system", Acta Materialia, 281, 120408. DOI: 10.1016/j.actamat.2024.120408.
    Abstract: Machine learning interatomic potentials (MLIPs) for α-iron and carbon binary system have been constructed aiming for understanding the mechanical behavior of Fe–C steel and carbides. The MLIPs were trained using an extensive reference database produced by spin polarized density functional theory (DFT) calculations. The MLIPs reach the DFT accuracies in many important properties which are frequently engaged in Fe and Fe–C studies, including kinetics and thermodynamics of C in α-Fe with vacancy, grain boundary, and screw dislocation, and basic properties of cementite and cementite–ferrite interfaces. In conjunction with these MLIPs, the impact of C atoms on the mobility of screw dislocation at finite temperature, and the C-decorated core configuration of screw dislocation were investigated, and a uniaxial tensile test on a model with multiple types of defects was conducted.

    Notes: This entry is for the DP potential in the reference that was trained using the DeepMD-kit (v2.2.3) package. BNNP shows better overall accuracy, and DP shows advantages in the atomic stress computation. These potentials can be used to simulate 𝛼-Fe-C systems and pure 𝛼-Fe systems, but these potentials should not be used for pure C system.

  • See Computed Properties
    Notes: These files were provided by Fan-Shun Meng on October 22, 2024. The authors suggest users compress the DP-FeC.dp model (see the DeepMD-kit documentation) before using it for MD simulation, as this will make the calculation significantly faster with limited influence on accuracy. Detailed instructions on using these potentials in MD simulations can be found at the link below.
    File(s): Link(s):
  • Citation: A. Allera, F. Ribeiro, M. Perez, and D. Rodney (2022), "Carbon-induced strengthening of bcc iron at the atomic scale", Physical Review Materials, 6(1), 013608. DOI: 10.1103/physrevmaterials.6.013608.
    Abstract: In steels, the interaction between screw dislocations and carbon solutes has a great influence on the yield strength. Fe-C potentials used in molecular dynamics (MD) simulations yield a poor description of screw dislocation properties-their core structure and Peierls barrier-compared to ab initio calculations. Here we combine two EAM potentials from the literature, which greatly improves dislocation property accuracy in FeC alloys. Using this hybrid potential, MD simulations of dislocation glide in random solid solutions confirm a powerful solute strengthening, caused by complex interaction processes. We analyze these processes in a model geometry, where a row of carbon atoms is inserted in the dislocation core with varying separations. We use a combination of MD simulations, minimum-energy path calculations, and a statistical model based on the harmonic transition state theory to explain the strengthening induced by carbon. We unveil that carbon disrupts the glide process, as unpinning requires the successive nucleation of two kink pairs. When solute separation is below about 100 Burgers vectors, the activation enthalpy of both kink pairs are markedly increased compared to pure iron, resulting in a strong dependence of the unpinning stress on solute spacing. Our simulations also suggest an effect of carbon spacing on the kink-pair activation entropy. This work provides elementary processes and parameters that will be useful for larger-scale models and, in particular, kinetic Monte Carlo simulations.

    Notes: This interatomic potential is a combination of the Fe-Fe interaction from 2012--Proville-L-Rodney-D-Marinica-M-C--Fe and the Fe-C interaction from 10.1016/j.commatsci.2013.09.048. It was adjusted for screw dislocation-carbon interaction, in the dilute limit (details in the paper). Authors recommend using it in reasonably similar settings.

    Related Models:
  • LAMMPS pair_style eam/alloy (2022--Allera-A--Fe-C--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was taken from the github repository listed below at the request of Arnaud Allera on 16 May 2023
    File(s): Link(s):
    Companion repository for the paper https://github.com/arn-all/FeC-EAM-potential

  • Citation: L.S.I. Liyanage, S.-G. Kim, J. Houze, S. Kim, M.A. Tschopp, M.I. Baskes, and M.F. Horstemeyer (2014), "Structural, elastic, and thermal properties of cementite (Fe3C) calculated using a modified embedded atom method", Physical Review B, 89(9), 094102. DOI: 10.1103/physrevb.89.094102.
    Abstract: Structural, elastic, and thermal properties of cementite (Fe3C) were studied using a modified embedded atom method (MEAM) potential for iron-carbon (Fe-C) alloys. Previously developed Fe and C single-element potentials were used to develop a Fe-C alloy MEAM potential, using a statistics-based optimization scheme to reproduce structural and elastic properties of cementite, the interstitial energies of C in bcc Fe, and heat of formation of Fe-C alloys in L12 and B1 structures. The stability of cementite was investigated by molecular dynamics simulations at high temperatures. The nine single-crystal elastic constants for cementite were obtained by computing total energies for strained cells. Polycrystalline elastic moduli for cementite were calculated from the single-crystal elastic constants of cementite. The formation energies of (001), (010), and (100) surfaces of cementite were also calculated. The melting temperature and the variation of specific heat and volume with respect to temperature were investigated by performing a two-phase (solid/liquid) molecular dynamics simulation of cementite. The predictions of the potential are in good agreement with first-principles calculations and experiments.

    Related Models:
  • See Computed Properties
    Notes: These files were contributed by Laalitha Liyanage (Central Michigan Univ., Univ. of North Texas) on 14 Apr. 2014.
    File(s):
  • Citation: K.O.E. Henriksson, C. Björkas, and K. Nordlund (2013), "Atomistic simulations of stainless steels: a many-body potential for the Fe-Cr-C system", Journal of Physics: Condensed Matter, 25(44), 445401. DOI: 10.1088/0953-8984/25/44/445401.
    Abstract: Stainless steels found in real-world applications usually have some C content in the base Fe–Cr alloy, resulting in hard and dislocation-pinning carbides—Fe3C (cementite) and Cr23C6—being present in the finished steel product. The higher complexity of the steel microstructure has implications, for example, for the elastic properties and the evolution of defects such as Frenkel pairs and dislocations. This makes it necessary to re-evaluate the effects of basic radiation phenomena and not simply to rely on results obtained from purely metallic Fe–Cr alloys. In this report, an analytical interatomic potential parameterization in the Abell–Brenner–Tersoff form for the entire Fe–Cr–C system is presented to enable such calculations. The potential reproduces, for example, the lattice parameter(s), formation energies and elastic properties of the principal Fe and Cr carbides (Fe3C, Fe5C2, Fe7C3, Cr3C2, Cr7C3, Cr23C6), the Fe–Cr mixing energy curve, formation energies of simple C point defects in Fe and Cr, and the martensite lattice anisotropy, with fair to excellent agreement with empirical results. Tests of the predictive power of the potential show, for example, that Fe–Cr nanowires and bulk samples become elastically stiffer with increasing Cr and C concentrations. High-concentration nanowires also fracture at shorter relative elongations than wires made of pure Fe. Also, tests with Fe3C inclusions show that these act as obstacles for edge dislocations moving through otherwise pure Fe.

    Notes: Note that this entry only represents the Fe-C subset of interatomic potentials developed and used in this reference.

    Related Models:
  • LAMMPS pair_style tersoff/zbl (2013--Henriksson-K-O-E--Fe-C--LAMMPS--ipr1)
    See Computed Properties
    Notes: The Tersoff/ZBL file was contributed by Astrid Gubbels-Elzas and Peter Klaver (Delft University of Technology, Netherlands) and posted with their approval and that of Krister Henriksson (Univ. of Helsinki, Finland) on 9 Jul. 2014. Note that this file only represents the Fe-C subset of interatomic potentials developed and used in this reference.
    File(s):
  • EAM tabulated functions (2013--Henriksson-K-O-E--Fe-C--table--ipr1)
    Notes: The following files were contributed by Dr. Henriksson and modified by C. Becker to include the reference and format in the header information. They represent the potential in Equation 7 of the reference, and the columns are r, VZBL, and d/dr (VZBL). They were approved by Dr. Henriksson for posting on 25 Jul. 2014.
    File(s):
 
  • Citation: I. Aslam, M.I. Baskes, D.E. Dickel, S. Adibi, B. Li, H. Rhee, M. Asle Zaeem, and M.F. Horstemeyer (2019), "Thermodynamic and kinetic behavior of low-alloy steels: An atomic level study using an Fe-Mn-Si-C modified embedded atom method (MEAM) potential", Materialia, 8, 100473. DOI: 10.1016/j.mtla.2019.100473.
    Abstract: A quaternary element Modified Embedded Atom Method (MEAM) potential comprising Fe, Mn, Si, and C is developed by employing a hierarchical multiscale modeling paradigm to simulate low-alloy steels. Experimental information alongside first-principles calculations based on Density Functional Theory served as calibration data to upscale and develop the MEAM potential. For calibrating the single element potentials, the cohesive energy, lattice parameters, elastic constants, and vacancy and interstitial formation energies are used as target data. The heat of formation and elastic constants of binary compounds along with substitutional and interstitial formation energies serve as binary potential calibration data, while substitutional and interstitial pair binding energies aid in developing the ternary potential. Molecular dynamics simulations employing the developed potentials predict the thermal expansion coefficient, heat capacity, self-diffusion coefficients, and stacking fault energy for steel alloys comparable to those reported in the literature.

    Related Models:
  • See Computed Properties
    Notes: This file was provided by Imran Aslam (Mississippi State) on Feb 28, 2020 and posted with his permission.
    File(s):
 
 
 
  • Citation: O.R. Deluigi, R.C. Pasianot, F.J. Valencia, A. Caro, D. Farkas, and E.M. Bringa (2021), "Simulations of primary damage in a High Entropy Alloy: Probing enhanced radiation resistance", Acta Materialia, 213, 116951. DOI: 10.1016/j.actamat.2021.116951.
    Abstract: High Entropy Alloys (HEA) attract attention as possible radiation resistant materials, a feature observed in some experiments that has been attributed to several unique properties of HEA, in particular to the disorder-induced reduced thermal conductivity and to the peculiar defect properties originating from the chemical complexity. To explore the origin of such behavior we study the early stages (less than 0.1 ns), of radiation damage response of a HEA using molecular dynamics simulations of collision cascades induced by primary knock-on atoms (PKA) with 10, 20 and 40 keV, at room temperature, on an idealized model equiatomic quinary fcc FeNiCrCoCu alloy, the corresponding "Average Atom" (AA) material, and on pure Ni. We include accurate corrections to describe short-range atomic interactions during the cascade. In all cases the average number of defects in the HEA is lower than for pure Ni, which has been previously used to help claiming that HEA is radiation resistant. However, simulated defect evolution during primary damage, including the number of surviving Frenkel Pairs, and the defect cluster size distributions are nearly the same in all cases, within our statistical uncertainty. The number of surviving FP in the alloy is predicted fairly well by analytical models of defect production in pure materials. All of this indicates that the origin of radiation resistance in HEAs as observed in experiments may not be related to a reduction in primary damage due to chemical disorder, but is probably caused by longer-time defect evolution.

    Notes: This is a modified version of 2018--Farkas-D-Caro-A--Fe-Ni-Cr-Co-Cu that adds the ZBL correction at shorter interatomic distances making it suitable for radiation studies.

  • See Computed Properties
    Notes: This file was provided by Diana Farkas (Virginia Tech) on May 16, 2021 and posted with her permission.
    File(s):
 
 
  • Citation: R. Gröger, V. Vitek, and A. Dlouhý (2020), "Effective pair potential for random fcc CoCrFeMnNi alloys", Modelling and Simulation in Materials Science and Engineering, 28(7), 075006. DOI: 10.1088/1361-651x/ab7f8b.
    Abstract: The single-phase equiatomic CoCrFeMnNi alloy is a random solid solution of five elements on the face-centered cubic lattice, whose pure constituents crystallize in very different structures and exhibit diverse magnetic properties. Due to the randomness of the alloy, 80% of nearest neighbor bonds are between unlike elements and thus the details of bonding in pure structures are less important. The elastic moduli of this alloy give rise to small Cauchy pressure C12 − C44, which suggests that the dominant part of bonding may be described by a simple pair potential. We test this hypothesis by developing a long-range Lennard-Jones potential in which the equilibrium crystal structures of pure constituents are taken as reference. The standard mixing rules for regular solutions are then adopted to obtain parameters for bonds between unlike elements in the quinary system. The transferability of this potential to quaternary CoCrFeNi, ternary CoCrNi, and binary FeNi alloys is investigated and the predictions compared with experiments and density functional theory calculations. By sampling over a large number of random configurations, we investigate the effect of compositional randomness on misfit volumes, energies of point defects and stacking faults, and the dislocation friction stresses experienced by moving edge and screw dislocations.

    Notes: R. Gröger notes that "This is the Mie n-2n potential, where n=6 was found to give the best results - it is the same as the Lennard-Jones 6-12 potential. These potential files contain parameterizations of the Co-Cr-Fe-Mn-Ni system intended for studies of compositionally complex alloys with spatially random distributions of individual elements. Although it was developed primarily for studies of the quinary fcc CoCrFeMnNi system, the paper above demonstrates that it can be used equally well for quaternaries and ternaries. We emphasize that the model ceases to be applicable for binary and unary systems, where most or all first neighbor bonds are between the same elements."

  • See Computed Properties
    Notes: These files were provided by Roman Gröger on Oct 23, 2021 and posted with his permission. The file mie.mod shows how to include these potentials in LAMMPS simulations via "include mie.mod".
    File(s):
 
  • Citation: A. Liang, D.C. Goodelman, A.M. Hodge, D. Farkas, and P.S. Branicio (2023), "CoFeNiTix and CrFeNiTix high entropy alloy thin films microstructure formation", Acta Materialia, 257, 119163. DOI: 10.1016/j.actamat.2023.119163.
    Abstract: High entropy alloys (HEA) composition-structure relationships are crucial for guiding their design and applications. Here, we use a combined experimental and molecular dynamics (MD) approach to investigate phase formation during physical vapor deposition (PVD) of CoFeNiTix and CrFeNiTix HEA thin films. We vary titanium molar ratio from 0 to 1 to understand the role of a larger element in the alloy mixture. The experiments show that a high titanium content favors amorphous phase formation in the samples produced by magnetron co-sputtering. In contrast, a low titanium content results in the formation of a face-centered cubic (FCC) structure in both HEA families. This effect of titanium content on the stability of the amorphous and FCC phases is reproduced in PVD MD simulations. The threshold titanium molar ratio is identified to be ~0.53 and ~0.16 for the CoFeNiTix and CrFeNiTix films in the experiments, and ~0.53 and ~0.53 in the MD simulations. In addition, the atomistic modeling allows for energy versus volume calculations with increasing titanium content, which demonstrate the stabilization of the amorphous phase with respect to crystalline structures. To isolate the effect of atomic sizes, additional simulations are performed using an average-atom model, which disregards differences in atomic radii while preserving the average properties of the alloy. In these simulations, the energetic stability of the amorphous phase disappears. The combined experimental and simulation results demonstrate that the formation of the amorphous phase in HEA thin films generated by PVD is directly caused by the atomic size difference.

  • See Computed Properties
    Notes: This file was provided by Diana Farkas on January 12, 2024.
    File(s):
 
 
 
 
 
 
 
  • Citation: P. Olsson, J. Wallenius, C. Domain, K. Nordlund, and L. Malerba (2005), "Two-band modeling of α-prime phase formation in Fe-Cr", Physical Review B, 72(21), 214119. DOI: 10.1103/physrevb.72.214119.
    Abstract: We have developed a two-band model of Fe-Cr, fitted to properties of the ferromagnetic alloy. Fitting many-body functionals to the calculated mixing enthalpy of the alloy and the mixed interstitial binding energy in iron, our potential reproduces changes in sign of the formation energy as a function of Cr concentration. When applied in kinetic Monte Carlo simulations, the potential correctly predicts decomposition of initially random Fe-Cr alloys into the α-prime phase as function of Cr concentration.
    Citation: P. Olsson, J. Wallenius, C. Domain, K. Nordlund, and L. Malerba (2006), "Erratum: Two-band modeling of α-prime phase formation in Fe-Cr [Phys. Rev. B 72, 214119 (2005)]", Physical Review B, 74(22), 229906. DOI: 10.1103/physrevb.74.229906.

    Related Models:
  • Citation: J. Wallenius, P. Olsson, and C. Lagerstedt (2005), "Relation between thermal expansion and interstitial formation energy in pure Fe and Cr", Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 228(1-4), 122-125. DOI: 10.1016/j.nimb.2004.10.032.
    Abstract: By fitting a potential of modified Finnis–Sinclair type to the thermal expansion of ferromagnetic Fe and paramagnetic Cr, stability of the <110> self-interstitial atom is obtained. The resulting potentials are relatively hard, yielding high SIA formation energies. Less hard potentials give lower interstitial formation energy, but predict too small thermal expansion. We also show that the formation energy of the <111> SIA depends on distances in-between the 2nd and 3rd neighbour. By raising the value of the pair potential in this region, the energy difference with respect to the <110> configuration calculated with VASP in the PAW approximation can be reproduced.

    Related Models:
 
  • Citation: S. Starikov, D. Smirnova, T. Pradhan, I. Gordeev, R. Drautz, and M. Mrovec (2022), "Angular-dependent interatomic potential for large-scale atomistic simulation of the Fe-Cr-H ternary system", Physical Review Materials, 6(4), 043604. DOI: 10.1103/physrevmaterials.6.043604.
    Abstract: The recently developed angular-dependent potential for pure iron was advanced to the interatomic potential of the Fe-Cr-H ternary system. The new potential allows to simulate Fe-Cr alloys for a wide range of compositions and different concentrations of hydrogen. The angular-dependent format of the model and the development procedure based on the machine learning approach allow to achieve a favorable balance between the computation cost and the reliability of the created parametrization. As part of potential validation, we performed a large number of tests of both the binary metallic alloys and hydrogen interactions. The applicability of the potential is demonstrated by large-scale simulations of hydrogen diffusion in the vicinity of crystal defects.

    Related Models:
  • See Computed Properties
    Notes: This file was provided by Sergei Starikov on April 26, 2022 and posted with his permission.
    File(s):
 
 
  • Citation: A. Daramola, G. Bonny, G. Adjanor, C. Domain, G. Monnet, and A. Fraczkiewicz (2022), "Development of a plasticity-oriented interatomic potential for CrFeMnNi high entropy alloys", Computational Materials Science, 203, 111165. DOI: 10.1016/j.commatsci.2021.111165.
    Abstract: An interatomic potential (termed EAM-21) has been developed with the embedded atomic method (EAM) for CrFeMnNi quaternary HEAs. This potential is based on a previously developed potential for CrFeNi ternary alloys. The parameters to develop the potential were determined by fitting to experimental values, density functional theory (DFT) and thermodynamic calculations, to reproduce the main crystal characteristics, namely: the stability of the fcc phase, elastic constants, and stacking fault energy. Its applicability for the study of plastic deformation mechanisms was checked by calculations of behaviour of a ½<1 1 0>1 1 1 edge dislocation in equiatomic quaternary CrFeMnNi alloy, as well as its less-complex subsystems (ternaries, binaries, and pure metals). The calculations were performed in the domain of temperatures between 0 and 900 K; smooth and stable glide of an edge dislocation and fcc phase stability in this temperature range was confirmed. This study demonstrates the suitability of the EAM-21 potential for the analysis of plasticity mechanisms and mechanical properties of CrFeMnNi HEAs.

    Notes: This potential is mostly suitable for microplasticity studies. This version of the potential is not stiffened for irradiation damage and displacement cascades studies.

  • See Computed Properties
    Notes: This file was provided by Giovanni Bonny on April 3, 2024 with the agreement of all the authors.
    File(s):
 
  • Citation: X.W. Zhou, M.E. Foster, and R.B. Sills (2018), "An Fe-Ni-Cr embedded atom method potential for austenitic and ferritic systems", Journal of Computational Chemistry, 39(29), 2420-2431. DOI: 10.1002/jcc.25573.
    Abstract: Fe‐Ni‐Cr stainless‐steels are important structural materials because of their superior strength and corrosion resistance. Atomistic studies of mechanical properties of stainless‐steels, however, have been limited by the lack of high‐fidelity interatomic potentials. Here using density functional theory as a guide, we have developed a new Fe‐Ni‐Cr embedded atom method potential. We demonstrate that our potential enables stable molecular dynamics simulations of stainless‐steel alloys at high temperatures, accurately reproduces the stacking fault energy-known to strongly influence the mode of plastic deformation (e.g., twinning vs. dislocation glide vs. cross‐slip)-of these alloys over a range of compositions, and gives reasonable elastic constants, energies, and volumes for various compositions. The latter are pertinent for determining short‐range order and solute strengthening effects. Our results suggest that our potential is suitable for studying mechanical properties of austenitic and ferritic stainless‐steels which have vast implementation in the scientific and industrial communities. Published 2018. This article is a U.S. Government work and is in the public domain in the USA.

    Related Models:
  • LAMMPS pair_style eam/alloy (2018--Zhou-X-W--Fe-Ni-Cr--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Xiaowang Zhou (Sandia National Laboratories) on 1 January 2019 and posted with his permission. The function tabulations are identical to 2018--Zhou-X-W--Fe-Ni-Cr--LAMMPS--ipr2 below, only the file format is different.
    File(s):
  • See Computed Properties
    Notes: This file was provided by Xiaowang Zhou (Sandia National Laboratories) on 1 January 2019 and posted with his permission. The function tabulations are identical to 2018--Zhou-X-W--Fe-Ni-Cr--LAMMPS--ipr1 above, only the file format is different.
    File(s):
  • Citation: L.K. Béland, A. Tamm, S. Mu, G.D. Samolyuk, Y.N. Osetsky, A. Aabloo, M. Klintenberg, A. Caro, and R.E. Stoller (2017), "Accurate classical short-range forces for the study of collision cascades in Fe–Ni–Cr", Computer Physics Communications, 219, 11-19. DOI: 10.1016/j.cpc.2017.05.001.
    Abstract: The predictive power of a classical molecular dynamics simulation is largely determined by the physical validity of its underlying empirical potential. In the case of high-energy collision cascades, it was recently shown that correctly modeling interactions at short distances is necessary to accurately predict primary damage production. An ab initio based framework is introduced for modifying an existing embedded-atom method FeNiCr potential to handle these short-range interactions. Density functional theory is used to calculate the energetics of two atoms approaching each other, embedded in the alloy, and to calculate the equation of state of the alloy as it is compressed. The pairwise terms and the embedding terms of the potential are modified in accordance with the ab initio results. Using this reparametrized potential, collision cascades are performed in Ni50Fe50, Ni80Cr20 and Ni33Fe33Cr33. The simulations reveal that alloying Ni and NiCr to Fe reduces primary damage production, in agreement with some previous calculations. Alloying Ni and NiFe to Cr does not reduce primary damage production, in contradiction with previous calculations.

    Notes: Prof. Béland notes that "The potential takes the 2011--Bonny-G-Terentyev-D-Pasianot-R-C-et-al--Fe-Ni-Cr potential and re-parameterizes the short-distance interactions based on DFT calculations, as explained in the paper and https://doi.org/10.1021/acs.jctc.5b01194. We recommend using this potential for simulating collision cascades."

    Related Models:
  • LAMMPS pair_style eam/alloy (2017--Beland-L-K--Fe-Ni-Cr--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Laurent Béland on 7 Nov 2019 and posted with his permission.
    File(s):
  • Citation: G. Bonny, N. Castin, and D. Terentyev (2013), "Interatomic potential for studying ageing under irradiation in stainless steels: the FeNiCr model alloy", Modelling and Simulation in Materials Science and Engineering, 21(8), 085004. DOI: 10.1088/0965-0393/21/8/085004.
    Abstract: The degradation of austenitic stainless steels in a radiation environment is a known problem for the in-core components of nuclear light water reactors. For a better understanding of the prevailing mechanisms responsible for the materials' degradation, large-scale atomistic simulations are desirable. In this framework and as a follow-up on Bonny et al (2011 Modelling Simul. Mater. Sci. Eng. 19 085008), we developed an embedded atom method type interatomic potential for the ternary FeNiCr system to model the production and evolution of radiation defects. Special attention has been drawn to the Fe10Ni20Cr alloy, whose properties were ensured to be close to those of 316L austenitic stainless steels. The potential is extensively benchmarked against density functional theory calculations and the potential developed in our earlier work. As a first validation, the potential is used in AKMC simulations to simulate thermal annealing experiments in order to determine the self-diffusion coefficients of the components in FeNiCr alloys around the Fe10Ni20Cr composition. The results from these simulations are consistent with experiments, i.e., DCr > DNi > DFe.

    Notes: Notes from Giovanni Bonny: "The present potential was developed to model POINT DEFECTS near the Fe-10Ni-20Cr composition.

    Related Models:
  • LAMMPS pair_style eam/alloy (2013--Bonny-G--Fe-Ni-Cr--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Giovanni Bonny (Nuclear Materials Science Institute of SCK-CEN, Belgium) on 13 Jan. 2014.
    File(s):
  • EAM tabulated functions (2013--Bonny-G--Fe-Ni-Cr--table--ipr1)
    Notes: These files were provided by Giovanni Bonny on 13 Jan. 2014.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2013--Bonny-G--Fe-Ni-Cr--LAMMPS--ipr1.
    Link(s):
  • Citation: G. Bonny, D. Terentyev, R.C. Pasianot, S. Poncé, and A. Bakaev (2011), "Interatomic potential to study plasticity in stainless steels: the FeNiCr model alloy", Modelling and Simulation in Materials Science and Engineering, 19(8), 085008. DOI: 10.1088/0965-0393/19/8/085008.
    Abstract: Austenitic stainless steels are commonly used materials for in-core components of nuclear light water reactors. In service, such components are exposed to harsh conditions: intense neutron irradiation, mechanical and thermal stresses, and aggressive corrosion environment which all contribute to the components' degradation. For a better understanding of the prevailing mechanisms responsible for the materials degradation, large-scale atomistic simulations are desirable. In this framework we developed an embedded atom method type interatomic potential for the ternary FeNiCr system to model movement of dislocations and their interaction with radiation defects. Special attention has been drawn to the Fe-10Ni-20Cr alloy, whose properties were ensured to be close to those of 316L austenitic stainless steel. In particular, the stacking fault energy and elastic constants are well reproduced. The fcc phase for the Fe–10Ni-20Cr random alloy was proven to be stable in the temperature range 0–900 K and under shear strain up to 5%. For the same alloy the stable glide of screw dislocations and stability of Frank loops was confirmed.

    Notes: Notes from Giovanni Bonny: "The present potential was developed to model dislocations around the Fe-10Ni-20Cr composition."

    Related Models:
  • LAMMPS pair_style eam/alloy (2011--Bonny-G--Fe-Ni-Cr--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Giovanni Bonny (Nuclear Materials Science Institute of SCK-CEN, Belgium) on 2 Sept. 2013. Update May 26 2021: This version is not compatible for LAMMPS versions starting with 29 Oct 2020 due to Infinify and NaN values no longer allowed.
    File(s): superseded


  • EAM tabulated functions (2011--Bonny-G--Fe-Ni-Cr--table--ipr1)
    Notes: These files were provided by Giovanni Bonny on 2 Sept. 2013.
    File(s):
    Fe F(ρ): F_Fe.spt
    Ni F(ρ): F_Ni.spt
    Cr F(ρ): F_Cr.spt
    Fe ρ(r): rhoFe.spt
    Ni ρ(r): rhoNi.spt
    Cr ρ(r): rhoCr.spt
    Fe φ(r): pFeFe.spt
    Ni φ(r): pNiNi.spt
    Cr φ(r): pCrCr.spt
    Fe-Ni φ(r): pFeNi.spt
    Fe-Cr φ(r): pFeCr.spt
    Ni-Cr φ(r): pNiCr.spt

  • LAMMPS pair_style eam/alloy (2011--Bonny-G--Fe-Ni-Cr--LAMMPS--ipr2)
    See Computed Properties
    Notes: This is a modification to the previous LAMMPS version and was posted by Lucas Hale on May 26, 2021. To make the file compatible with LAMMPS versions after 29 Oct 2020, INF values at r=0 for the elemental r*phi tables were replaced by values computed using the parameters listed in the paper.
    File(s):
 
  • Citation: G. Arora, G. Bonny, N. Castin, and D.S. Aidhy (2021), "Effect of different point-defect energetics in Ni80X20 (X=Fe, Pd) on contrasting vacancy cluster formation from atomistic simulations", Materialia, 15, 100974. DOI: 10.1016/j.mtla.2020.100974.
    Abstract: Recent irradiation experiments have shown that smaller vacancy clusters are observed in Ni80Pd20 compared to Ni80Fe20. Using atomistic calculations, we find that the vacancy energetics are significantly different between the two alloys. Ni80Pd20 has lower vacancy migration barriers and lower vacancy-vacancy binding energies than Ni80Fe20. The consequence of these energetic differences is observed in molecular dynamics (MD) simulations, where despite higher vacancy diffusivity that would help in cluster formation, significantly reduced vacancy clusters are observed in Ni80Pd20 than Ni80Fe20. Calculations show that binding energy decreases and formation energy increases with increasing Ni-Ni bond lengths, and larger Ni-Ni bond lengths are observed in Ni80Pd20 than Ni80Fe20. Thus, the reduced vacancy-vacancy binding and higher formation energy due to longer Ni-Ni bonds in Ni80Pd20 are possibly the underlying reasons for smaller vacancy clusters in Ni80-Pd20 than Ni80Fe20. This study illustrates the unique effects of alloying elements on defect energetics and microstructural evolution in random alloys.

    Notes: Gaurav Arora notes that "This is one of the first types of potentials used to study radiation defects in alloys containing Pd and is a modified version of 2018--Bonny-G-Chakraborty-D-Pandey-S-et-al--Ni-Fe-Cr-Pd. This potential was specifically developed to study defect energetics, such as vacancy formation energies, binding energies, voids, stacking fault tetrahedra (SFTs) formation, and other radiation defects in high entropy alloys."

  • LAMMPS pair_style eam/alloy (2021--Arora-G--Fe-Ni-Cr-Pd--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Gaurav Arora on July 17, 2024.
    File(s):
  • Citation: G. Bonny, D. Chakraborty, S. Pandey, A. Manzoor, N. Castin, S.R. Phillpot, and D.S. Aidhy (2018), "Classical interatomic potential for quaternary Ni-Fe-Cr-Pd solid solution alloys", Modelling and Simulation in Materials Science and Engineering, 26(6), 065014. DOI: 10.1088/1361-651x/aad2e7.
    Abstract: In this paper, we present a new quaternary interatomic potential for the NiFeCrPd system, which is an extension on the previous NiFeCr potential. Density functional theory is used to calculate the quantities to be fitted, with particular focus on the energetics of point defects with solutes, for the potential to be used towards understanding radiation damage properties. The potential thus will enable the modeling of multi-elemental solid solution alloys consisting of up to four elements. To test the potential, we have performed atomistic kinetic Monte Carlo simulations to investigate the effect of configurational entropy on the self-diffusion coefficients. The self-diffusion coefficients are found to increase with chemical complexity, contrary to the common postulation of sluggish diffusion in high entropy alloys (HEAs). In addition, we have performed molecular dynamics simulations to elucidate the effect of Pd on vacancy diffusion and clustering in pure Ni and binary alloys. In agreement with recent irradiation experiments, our simulations show that while large vacancy clusters, such as stacking fault tetrahedra, are formed in pure Ni, Ni-Fe and Ni-Cr systems, negligible vacancy clustering is observed in Ni-Pd systems, indicating a possible effect of Pd in reducing cluster sizes. We suggest that this potential will be useful for studying the defect evolution in multi-component HEAs.

 
 
 
 
 
 
 
 
  • Citation: P. Kumar, M.M. Ludhwani, S. Das, V. Gavini, A. Kanjarla, and I. Adlakha (2023), "Effect of hydrogen on plasticity of α-Fe: A multi-scale assessment", International Journal of Plasticity, 165, 103613. DOI: 10.1016/j.ijplas.2023.103613.
    Abstract: A multi-scale study was carried out to quantify the effect of interstitial hydrogen concentration on plasticity in α-Fe. In this work, the influence of hydrogen on the screw dislocation glide behavior was examined across several length-scales. The insights obtained were integrated to provide an accurate continuum description for the effect of hydrogen on the dislocation based plasticity in polycrystalline α-Fe. At the outset of this work, a new Fe-H interatomic potential was formulated that enhanced the atomistic estimation of the variation in dislocation glide behavior in presence of hydrogen. Next, the dislocation core reconstruction observed due to the addition of hydrogen using atomistic simulations was validated with the help of large-scale DFT calculations based on the DFT-FE framework. Several atomistic simulations were carried out to comprehensively quantify the effect of hydrogen on the non-Schmid behavior exhibited during the dislocation glide in α-Fe. Finally, crystal plasticity simulations were carried out to understand the effect of hydrogen on the meso-scale deformation behavior of polycrystalline α-Fe.

    Notes: Professor Adlakha notes that this potential is able to "accurately predict the correct (non-degenerate) screw dislocation core in BCC-Fe. Furthermore, the potential correctly predicts a single-hump profile for the Peierls potential. The effect of hydrogen on the screw dislocation was found to be in good agreement with large scale DFT calculations discussed in the manuscript. The potential correctly predicts hydrogen binding at various defects and surfaces in BCC-Fe. However, the potential has not been validated for finite temperature hydrogen diffusion."

  • LAMMPS pair_style eam/fs (2023--Kumar-P--Fe-H--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Ilaksh Adlakha on 28 April 2023.
    File(s):
  • Citation: F.-S. Meng, J.-P. Du, S. Shinzato, H. Mori, P. Yu, K. Matsubara, N. Ishikawa, and S. Ogata (2021), "General-purpose neural network interatomic potential for the 𝛼-iron and hydrogen binary system: Toward atomic-scale understanding of hydrogen embrittlement", Physical Review Materials, 5(11), 113606. DOI: 10.1103/physrevmaterials.5.113606.
    Abstract: To understand the physics of hydrogen embrittlement at the atomic scale, a general-purpose neural network interatomic potential (NNIP) for the 𝛼-iron and hydrogen binary system is presented. It is trained using an extensive reference database produced by density functional theory (DFT) calculations. The NNIP can properly describe the interactions of hydrogen with various defects in 𝛼-iron, such as vacancies, surfaces, grain boundaries, and dislocations; in addition to the basic properties of 𝛼-iron itself, the NNIP also handles the defect properties in 𝛼-iron, hydrogen behavior in 𝛼-iron, and hydrogen-hydrogen interactions in 𝛼-iron and in vacuum, including the hydrogen molecule formation and dissociation at the 𝛼-iron surface. These are superb challenges for the existing empirical interatomic potentials, like the embedded-atom method based potentials, for the 𝛼-iron and hydrogen binary system. In this study, the NNIP was applied to several key phenomena necessary for understanding hydrogen embrittlement, such as hydrogen charging and discharging to 𝛼-iron, hydrogen transportation in defective 𝛼-iron, hydrogen trapping and desorption at the defects, and hydrogen-assisted cracking at the grain boundary. Unlike the existing interatomic potentials, the NNIP simulations quantitatively described the atomistic details of hydrogen behavior in the defective 𝛼-iron system with DFT accuracy.

    Notes: Fan-Shun Meng notes that "This potential was designed for the general purpose usage of the 𝛼-Fe-H binary system. Additionally, the potential also can be used for pure 𝛼-Fe. To use the potential in LAMMPS, the pair_style of hdnnp should be adopted, and the package of ML-HDNNP should be compiled(see ML-HDNNP documentation)."

  • LAMMPS pair_style hdnnp (2021--Meng-F-S--Fe-H--LAMMPS--ipr1)
    See Computed Properties
    Notes: These files were provided by Fan-Shun Meng on August 30, 2024.
    File(s): Link(s):
  • Citation: M. Wen (2021), "A new interatomic potential describing Fe-H and H-H interactions in bcc iron", Computational Materials Science, 197, 110640. DOI: 10.1016/j.commatsci.2021.110640.
    Abstract: We present a new many-body interatomic potential for H in body-centered cubic (bcc) Fe. The potential is developed based on extensive energetics and atomic configurations of an H atom and H-H interactions in Fe from density functional theory calculations. In detail, the potential is parameterized by fitting not only to a single H atom in the perfect bcc Fe lattice and to the properties of H trap binding to a vacancy and surfaces as being done by previous studies, but also to multiple H trapping to a vacancy and H-H interaction in Fe lattice. With such a fitting strategy, the developed potential outperforms existing potentials in its ability not only describing the behaviors of a single H atom in Fe, but also capturing the features of H-H interaction reliably, which is of key importance in revealing H behaviors in local H accumulation around dislocation cores, grain boundaries and crack tips.

  • LAMMPS pair_style eam/fs (2021--Wen-M--Fe-H--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Ping Yu (Shanghai Jiao Tong University) on June 24, 2021 and posted with his permission.
    File(s):
 
 
 
 
 
 
  • Citation: Y. Sun, M.I. Mendelev, F. Zhang, X. Liu, B. Da, C.-Z. Wang, R.M. Wentzcovitch, and K.-M. Ho (2024), "Unveiling the effect of Ni on the formation and structure of Earth’s inner core", Proceedings of the National Academy of Sciences, 121(4), e2316477121. DOI: 10.1073/pnas.2316477121.
    Abstract: Ni is the second most abundant element in the Earth’s core. Yet, its effects on the inner core’s structure and formation process are usually disregarded because of its electronic and size similarity with Fe. Using ab initio molecular dynamics simulations, we find that the bcc phase can spontaneously crystallize in liquid Ni at temperatures above Fe’s melting point at inner core pressures. The melting temperature of Ni is shown to be 700 to 800 K higher than that of Fe at 323 to 360 GPa. hcp, bcc, and liquid phase relations differ for Fe and Ni. Ni can be a bcc stabilizer for Fe at high temperatures and inner core pressures. A small amount of Ni can accelerate Fe’s crystallization at core pressures. These results suggest that Ni may substantially impact the structure and formation process of the solid inner core.

    Notes: The potential was employed in the TI calculations in the above reference. It can be used as an initial approximation for MD simulations under the Earth’s inner core conditions.

  • LAMMPS pair_style eam/fs (2024--Sun-Y--Fe-Ni--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Mikhail Mendelev on February 16, 2024.
    File(s):
  • Citation: Y. Mishin, M.J. Mehl, and D.A. Papaconstantopoulos (2005), "Phase stability in the Fe-Ni system: Investigation by first-principles calculations and atomistic simulations", Acta Materialia, 53(15), 4029-4041. DOI: 10.1016/j.actamat.2005.05.001.
    Abstract: First-principles calculations of the energy of various crystal structures of Fe, Ni and ordered Fe–Ni compounds with different stoichiometries have been performed by the linearized augmented plane wave (LAPW) method in the generalized gradient approximation. The most stable compounds are L12–Ni3Fe, L10–FeNi, C11f–Ni2Fe and C11f–Fe2Ni. The L12-Ni3Fe compound has the largest negative formation energy, which is consistent with the experimental Fe–Ni phase diagram. The L10–FeNi compound has also been observed experimentally in meteorite samples as a metastable phase. It is suggested here that the C11f compounds could also form in Fe–Ni alloys at low temperatures. A new semi-empirical interatomic potential has been developed for the Fe–Ni system by fitting to experimental data and the results of the LAPW calculations. Recognizing the significance of the covalent component of bonding in this system, the potential is based on the embedded-atom method (EAM) but additionally includes a bond-angle dependence. In comparison with the existing modified EAM method, our potential form is simpler, extends interactions to several (3–5) coordination shells and replaces the screening procedure by a smooth cutoff of the potential functions. The potential reproduces a variety of properties of Fe and Ni with a reasonable accuracy. It also reproduces all stability trends across the Fe–Ni system established by the LAPW calculations. The potential can be useful in atomistic simulations of the phases of the Fe–Ni system.

  • ADP tabulated functions (2005--Mishin-Y--Fe-Ni--table--ipr1)
    Notes: These files were provided by Yuri Mishin (George Mason University) and posted on 22 Dec. 2009. Prof. Mishin requested the following note be included: "The equation appearing in the Appendix on page 4040 contains a typing error: the sign before 1/3 in the last line must be negative." He provided the corrected equation for the angular-dependent force contributions in ADP_Forces.jpg or ADP_Forces.pdf.
    File(s):
    Fe F(ρ): F_Fe.plt
    Ni F(ρ): F_Ni.plt
    Fe ρ(r): fFe.plt
    Ni ρ(r): fNi.plt
    Fe φ(r): pFe.plt
    Ni φ(r): pNi.plt
    Fe-Ni φ(r): pFeNi.plt
    Fe u(r): dFe.plt
    Ni u(r): dNi.plt
    Fe-Ni u(r): dFeNi.plt
    Fe w(r): qFe.plt
    Ni w(r): qNi.plt
    Fe-Ni w(r): qFeNi.plt
    ADP_Forces.jpg
    ADP_Forces.pdf

 
 
  • Citation: J. Byggmästar, M. Nagel, K. Albe, K. Henriksson, and K. Nordlund (2019), "Analytical interatomic bond-order potential for simulations of oxygen defects in iron", Journal of Physics: Condensed Matter, 31, 215401. DOI: 10.1088/1361-648x/ab0931.
    Abstract: We present an analytical bond-order potential for the Fe–O system, capable of reproducing the basic properties of wüstite as well as the energetics of oxygen impurities in α-iron. The potential predicts binding energies of various small oxygen-vacancy clusters in α-iron in good agreement with density functional theory results, and is therefore suitable for simulations of oxygen-based defects in iron. We apply the potential in simulations of the stability and structure of Fe/FeO interfaces and FeO precipitates in iron, and observe that the shape of FeO precipitates can change due to formation of well-defined Fe/FeO interfaces. The interface with crystalline Fe also ensures that the precipitates never become fully amorphous, no matter how small they are.

    Notes: The potential is not suitable for simulations of the Fe2O3 and Fe3O4 phases.

    Related Models:
  • LAMMPS pair_style tersoff/zbl (2019--Byggmastar-J--Fe-O--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was provided by Jesper Byggmästar (University of Helsinki) on 20 March 2019 and posted with his permission.
    File(s):
 
 
 
 
 
  • Citation: M.I. Mendelev, S. Han, W.- Son, G.J. Ackland, and D.J. Srolovitz (2007), "Simulation of the interaction between Fe impurities and point defects in V", Physical Review B, 76(21), 214105. DOI: 10.1103/physrevb.76.214105.
    Abstract: We report improved results of atomistic modeling of V-Fe alloys. We introduced an electronic structure embedding approach to improve the description of the point defects in first-principles calculations, by including the semicore electrons in some V atoms (those near the interstitial where the semicore levels are broadened) but not those further from the point defect. This enables us to combine good accuracy for the defect within large supercells and to expand the data set of first-principles point defect calculations in vanadium with and without small amounts of iron. Based on these data, previous first-principles work, and new calculations on the alloy liquid, we fitted an interatomic potential for the V-Fe system which describes the important configurations likely to arise when such alloys are exposed to radiation. This potential is in a form suitable for molecular dynamics (MD) simulations of large systems. Using the potential, we have calculated the migration barriers of vacancies in the presence of iron, showing that these are broadly similar. On the other hand, MD simulations show that V self-diffusion at high temperatures and Fe diffusion are greatly enhanced by the presence of interstitials.

    Related Models:
  • See Computed Properties
    Notes: This file was provided by Mikhail Mendelev. Except for comments, this file is equivalent to "VFe_mm.eam.fs" in the August 22, 2018 LAMMPS distribution. Update 19 July 2021: The contact email in the file's header has been changed.
    File(s):
  • See Computed Properties
    Notes: Listing found at https://openkim.org. This KIM potential is based on the files from 2007--Mendelev-M-I--V-Fe--LAMMPS--ipr1.
    Link(s):
 
 
  • Citation: P. Wang, S. Xu, J. Liu, X. Li, Y. Wei, H. Wang, H. Gao, and W. Yang (2017), "Atomistic simulation for deforming complex alloys with application toward TWIP steel and associated physical insights", Journal of the Mechanics and Physics of Solids, 98, 290-308. DOI: 10.1016/j.jmps.2016.09.008.
    Abstract: The interest in promoting deformation twinning for plasticity is mounting for advanced materials. In contrast to disordered grain boundaries, highly organized twin boundaries are beneficial to promoting strength-ductility combination. Twinning deformation typically involves the kinetics of stacking faults, its interplay with dislocations, as well as the interactions between dislocations and twin boundaries. While the latter has been intensively studied, the dynamics of stacking faults has been rarely touched upon. In this work, we report new physical insights on the stacking fault dynamics in twin induced plasticity (TWIP) steels. The atomistic simulation is made possible by a newly introduced approach: meta-atom molecular dynamics simulation. The simulation suggests that the stacking fault interactions are dominated by dislocation reactions that take place spontaneously, different from the existing mechanisms. Whether to generate a single stacking fault, or a twinning partial and a trailing partial dislocation, depends upon a unique parameter, namely the stacking fault energy. The latter in turn determines the deformation twinning characteristics. The complex twin-slip and twin-dislocation interactions demonstrate the dual role of deformation twins as both the dislocation barrier and dislocation storage. This duality contributes to the high strength and high ductility of TWIP steels.

    Notes: Dr. Peng Wang noted that this potential for TWIP steel was developed based on the concept "meta-atom method". The meta-atom method is developed based on the basic assumption that the mechanical properties of an alloy system are primarily governed by a finite set of material constants instead of specific atomic configurations. Once the completeness of this set of material constants is established, two systems with the same material constants should exhibit identical mechanical behaviors in experimental observations. In this way, a detailed distinction among various atomic species is discarded and an alloy system is represented by a set of meta-atoms with a single interatomic potential to fit all related material constants. This method is firstly published in Journal of the Mechanics and Physics of Solids (2017), 98, 290-308. It is not possible to model individual elements of Fe or Mn with this potential.

  • LAMMPS pair_style eam/fs (2017--Wang-P--TWIP--LAMMPS--ipr1)
    See Computed Properties
    Notes: This file was sent by P. Wang (Zhejiang University) on 24 Feb. 2017 and posted with the permission of Dr. Peng Wang and Prof. Hongtao Wang.
    File(s): superseded


  • LAMMPS pair_style eam/fs (2017--Wang-P--TWIP--LAMMPS--ipr2)
    See Computed Properties
    Notes: Dr. P. Wang (Zhejiang University) sent a revised file on 25 Sept. 2017 to address significant confusion regarding the appropriate use of the potential. The file name was changed and the element label Fe was replaced with meta_TWIP. It is not possible to model individual elements of Fe or Mn with this potential.
    File(s):
Date Created: October 5, 2010 | Last updated: March 05, 2025