EAM_Dynamo_StollerTammBeland_2016_Ni__MO_103383163946_001
| Title
A single sentence description.
|
EAM potential (LAMMPS cubic hermite tabulation) for Ni developed by Stoller et al. (2016) v001 |
|---|---|
| Description
A short description of the Model describing its key features including for example: type of model (pair potential, 3-body potential, EAM, etc.), modeled species (Ac, Ag, ..., Zr), intended purpose, origin, and so on.
|
This is an EAM potential for high-energy collisions in nickel. It is fitted using a procedure that involves the use of ab initio calculations to determine the magnitude and spatial dependence of the pair interactions at intermediate distances, along with systematic criteria for choosing the joining parameters. |
| Species
The supported atomic species.
| Ni |
| Disclaimer
A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.
|
None |
| Content Origin | https://www.ctcms.nist.gov/potentials/entry/2016--Stoller-R-E-Tamm-A-Beland-L-K-et-al--Ni/ |
| Contributor |
I Nikiforov |
| Maintainer |
I Nikiforov |
| Developer |
Roger E. Stoller Artur Tamm Laurent K. Béland German D. Samolyuk G. Malcolm Stocks A. Caro Lyudmila V. Slipchenko Yuri N. Osetskiy Alvo Aabloo Mattias Klintenberg Yang Wang |
| Published on KIM | 2025 |
| How to Cite |
This Model originally published in [1] is archived in OpenKIM [2-5]. [1] Stoller RE, Tamm A, Béland LK, Samolyuk GD, Stocks GM, Caro A, et al. Impact of Short-Range Forces on Defect Production from High-Energy Collisions. Journal of Chemical Theory and Computation [Internet]. 2016;12(6):2871–9. Available from: https://doi.org/10.1021/acs.jctc.5b01194 doi:10.1021/acs.jctc.5b01194 — (Primary Source) A primary source is a reference directly related to the item documenting its development, as opposed to other sources that are provided as background information. [2] Stoller RE, Tamm A, Béland LK, Samolyuk GD, Stocks GM, Caro A, et al. EAM potential (LAMMPS cubic hermite tabulation) for Ni developed by Stoller et al. (2016) v001. OpenKIM; 2025. doi:10.25950/4522e4b5 [3] Foiles SM, Baskes MI, Daw MS, Plimpton SJ. EAM Model Driver for tabulated potentials with cubic Hermite spline interpolation as used in LAMMPS v006. OpenKIM; 2025. doi:10.25950/233cb735 [4] Tadmor EB, Elliott RS, Sethna JP, Miller RE, Becker CA. The potential of atomistic simulations and the Knowledgebase of Interatomic Models. JOM. 2011;63(7):17. doi:10.1007/s11837-011-0102-6 [5] Elliott RS, Tadmor EB. Knowledgebase of Interatomic Models (KIM) Application Programming Interface (API). OpenKIM; 2011. doi:10.25950/ff8f563a |
| Funding |
Funder: Basic Energy Sciences Funder: Fonds Québécois de la Recherche sur la Nature et les Technologies Funder: Purdue University |
| Short KIM ID
The unique KIM identifier code.
| MO_103383163946_001 |
| Extended KIM ID
The long form of the KIM ID including a human readable prefix (100 characters max), two underscores, and the Short KIM ID. Extended KIM IDs can only contain alpha-numeric characters (letters and digits) and underscores and must begin with a letter.
| EAM_Dynamo_StollerTammBeland_2016_Ni__MO_103383163946_001 |
| DOI |
10.25950/4522e4b5 https://doi.org/10.25950/4522e4b5 https://commons.datacite.org/doi.org/10.25950/4522e4b5 |
| KIM Item Type
Specifies whether this is a Portable Model (software implementation of an interatomic model); Portable Model with parameter file (parameter file to be read in by a Model Driver); Model Driver (software implementation of an interatomic model that reads in parameters).
| Portable Model using Model Driver EAM_Dynamo__MD_120291908751_006 |
| Driver | EAM_Dynamo__MD_120291908751_006 |
| KIM API Version | 2.2 |
| Potential Type | eam |
| Previous Version | EAM_Dynamo_StollerTammBeland_2016_Ni__MO_103383163946_000 |
This bar chart plot shows the mono-atomic body-centered cubic (bcc) lattice constant predicted by the current model (shown in the unique color) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This graph shows the cohesive energy versus volume-per-atom for the current mode for four mono-atomic cubic phases (body-centered cubic (bcc), face-centered cubic (fcc), simple cubic (sc), and diamond). The curve with the lowest minimum is the ground state of the crystal if stable. (The crystal structure is enforced in these calculations, so the phase may not be stable.) Graphs are generated for each species supported by the model.
(No matching species)This bar chart plot shows the mono-atomic face-centered diamond lattice constant predicted by the current model (shown in the unique color) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This graph shows the dislocation core energy of a cubic crystal at zero temperature and pressure for a specific set of dislocation core cutoff radii. After obtaining the total energy of the system from conjugate gradient minimizations, non-singular, isotropic and anisotropic elasticity are applied to obtain the dislocation core energy for each of these supercells with different dipole distances. Graphs are generated for each species supported by the model.
(No matching species)This bar chart plot shows the mono-atomic face-centered cubic (fcc) elastic constants predicted by the current model (shown in blue) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This bar chart plot shows the mono-atomic face-centered cubic (fcc) lattice constant predicted by the current model (shown in red) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This bar chart plot shows the intrinsic and extrinsic stacking fault energies as well as the unstable stacking and unstable twinning energies for face-centered cubic (fcc) predicted by the current model (shown in blue) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This bar chart plot shows the mono-atomic face-centered cubic (fcc) relaxed surface energies predicted by the current model (shown in blue) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This bar chart plot shows the mono-atomic simple cubic (sc) lattice constant predicted by the current model (shown in the unique color) compared with the predictions for all other models in the OpenKIM Repository that support the species. The vertical bars show the average and standard deviation (one sigma) bounds for all model predictions. Graphs are generated for each species supported by the model.
(No matching species)This Model requires a Model Driver. Click below for the Model Driver EAM_Dynamo__MD_120291908751_006 archive.