Title
A single sentence description.
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A spectral neighbor analysis potential for Mo developed by Chi Chen (2019) v000 |
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Citations
This panel presents the list of papers that cite the interatomic potential whose page you are on (by its primary sources given below in "How to Cite"). Articles marked by the green star have been determined to have used the potential in computations (as opposed to only citing it as background information) by a machine learning (ML) algorithm developed by the KIM Team that analyzes the full text of the papers. Articles that do not use it are marked with a null symbol, and in cases where no information is available a question mark is shown. The full text of the articles used to train the ML algorithm is provided by the Allen Institute for AI through the Semantic Scholar project. The word cloud to the right is built from the abstracts of the primary sources and using papers to give a sense of the types of physical phenomena to which this interatomic potential is applied. IMPORTANT NOTE: Usage can only be determined for articles for which Semantic Scholar can provide OpenKIM with the full text. Where this is not the case, we ask the community for help in determining usage. If you know whether an article did or did not use a potential, let us know by clicking the cloud icon by the article and completing a one question form. |
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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.
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A spectral neighbor analysis potential for Mo. The potential is trained against diverse and large materials data, including bulk bcc Mo, strained bcc Mo, ab-initio molecular dynamics (AIMD) simulated random structures, melted structures, vacancy-containing structures, surfaces, grain boundaries, strained melted structures. The potential gives accurate predictions of structural energies, forces, stresses, elasticity, lattice parameters, vacancy migration barrier, equation-of-state, phonon, free energies, melting point, surface energies, and grain boundary energies. |
Species
The supported atomic species.
| Mo |
Disclaimer
A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.
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This potential is designed for Mo bcc systems. It is not appropriate for other elements. The potential was trained using LAMMPS version 17Nov2016. Newer LAMMPS may see energy differences, but the relative values should remain to be the same. |
Content Other Locations |
https://arxiv.org/abs/1706.09122 https://journals.aps.org/prmaterials/abstract/10.1103/PhysRevMaterials.1.043603 |
Contributor |
Chi Chen |
Maintainer |
Chi Chen |
Published on KIM | 2020 |
How to Cite |
This Model originally published in [1] is archived in OpenKIM [2-5]. [1] Chen C, Deng Z, Tran R, Tang H, Chu I-H, Ong SP. Accurate Force Field for Molybdenum by Machine Learning Large Materials Data. Physical Review Materials. 2017;1(4):043603. doi:10.1103/PhysRevMaterials.1.043603 — (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] Chen C. A spectral neighbor analysis potential for Mo developed by Chi Chen (2019) v000. OpenKIM; 2020. doi:10.25950/63ad82cb [3] Chen C. Spectral neighbor analysis potential (SNAP) model driver v000. OpenKIM; 2019. doi:10.25950/f4fae493 [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 Click here to download the above citation in BibTeX format. |
Funding | Not available |
Short KIM ID
The unique KIM identifier code.
| MO_698578166685_000 |
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.
| SNAP_ChenDengTran_2017_Mo__MO_698578166685_000 |
DOI |
10.25950/63ad82cb https://doi.org/10.25950/63ad82cb https://search.datacite.org/works/10.25950/63ad82cb |
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 SNAP__MD_536750310735_000 |
Driver | SNAP__MD_536750310735_000 |
KIM API Version | 2.0 |
Potential Type | snap |
Grade | Name | Category | Brief Description | Full Results | Aux File(s) |
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P | vc-species-supported-as-stated | mandatory | The model supports all species it claims to support; see full description. |
Results | Files |
P | vc-periodicity-support | mandatory | Periodic boundary conditions are handled correctly; see full description. |
Results | Files |
P | vc-permutation-symmetry | mandatory | Total energy and forces are unchanged when swapping atoms of the same species; see full description. |
Results | Files |
A | vc-forces-numerical-derivative | consistency | Forces computed by the model agree with numerical derivatives of the energy; see full description. |
Results | Files |
P | vc-dimer-continuity-c1 | informational | The energy versus separation relation of a pair of atoms is C1 continuous (i.e. the function and its first derivative are continuous); see full description. |
Results | Files |
P | vc-objectivity | informational | Total energy is unchanged and forces transform correctly under rigid-body translation and rotation; see full description. |
Results | Files |
P | vc-inversion-symmetry | informational | Total energy is unchanged and forces change sign when inverting a configuration through the origin; see full description. |
Results | Files |
P | vc-memory-leak | informational | The model code does not have memory leaks (i.e. it releases all allocated memory at the end); see full description. |
Results | Files |
P | vc-thread-safe | mandatory | The model returns the same energy and forces when computed in serial and when using parallel threads for a set of configurations. Note that this is not a guarantee of thread safety; see full description. |
Results | Files |
N/A | vc-unit-conversion | mandatory | The model is able to correctly convert its energy and/or forces to different unit sets; see full description. |
Results | Files |
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.
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.
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.
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.
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.
This potential is designed for Mo bcc systems. It is not appropriate for other elements. The potential was trained using LAMMPS version 17Nov2016. Newer LAMMPS may see energy differences, but the relative values should remain to be the same.
Test | Test Results | Link to Test Results page | Benchmark time
Usertime multiplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.
Measured in Millions of Whetstone Instructions (MWI) |
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Cohesive energy versus lattice constant curve for bcc Mo v004 | view | 3839 | |
Cohesive energy versus lattice constant curve for diamond Mo v004 | view | 4286 | |
Cohesive energy versus lattice constant curve for fcc Mo v004 | view | 3163 | |
Cohesive energy versus lattice constant curve for sc Mo v004 | view | 2845 |
Test | Test Results | Link to Test Results page | Benchmark time
Usertime multiplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.
Measured in Millions of Whetstone Instructions (MWI) |
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Elastic constants for diamond Mo at zero temperature v001 | view | 17106 | |
Elastic constants for sc Mo at zero temperature v006 | view | 2976 |
Test | Test Results | Link to Test Results page | Benchmark time
Usertime multiplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.
Measured in Millions of Whetstone Instructions (MWI) |
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Relaxed energy as a function of tilt angle for a 100 symmetric tilt grain boundary in bcc Mo v001 | view | 123902601 | |
Relaxed energy as a function of tilt angle for a 110 symmetric tilt grain boundary in bcc Mo v001 | view | 376591741 | |
Relaxed energy as a function of tilt angle for a 111 symmetric tilt grain boundary in bcc Mo v001 | view | 208782313 |
Test | Test Results | Link to Test Results page | Benchmark time
Usertime multiplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.
Measured in Millions of Whetstone Instructions (MWI) |
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Equilibrium zero-temperature lattice constant for bcc Mo v007 | view | 1817 | |
Equilibrium zero-temperature lattice constant for diamond Mo v007 | view | 2099 | |
Equilibrium zero-temperature lattice constant for fcc Mo v007 | view | 1848 | |
Equilibrium zero-temperature lattice constant for sc Mo v007 | view | 2005 |
Test | Test Results | Link to Test Results page | Benchmark time
Usertime multiplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.
Measured in Millions of Whetstone Instructions (MWI) |
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Equilibrium lattice constants for hcp Mo v005 | view | 28479 |
Test | Error Categories | Link to Error page |
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Elastic constants for hcp Mo at zero temperature v004 | other | view |
Test | Error Categories | Link to Error page |
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Relaxed energy as a function of tilt angle for a 112 symmetric tilt grain boundary in bcc Mo v001 | other | view |
Test | Error Categories | Link to Error page |
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Monovacancy formation energy and relaxation volume for bcc Mo | mismatch | view |
Test | Error Categories | Link to Error page |
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Vacancy formation and migration energy for bcc Mo | mismatch | view |
Verification Check | Error Categories | Link to Error page |
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MemoryLeak__VC_561022993723_004 | other | view |
SNAP_ChenDengTran_2017_Mo__MO_698578166685_000.txz | Tar+XZ | Linux and OS X archive |
SNAP_ChenDengTran_2017_Mo__MO_698578166685_000.zip | Zip | Windows archive |
This Model requires a Model Driver. Archives for the Model Driver SNAP__MD_536750310735_000 appear below.
SNAP__MD_536750310735_000.txz | Tar+XZ | Linux and OS X archive |
SNAP__MD_536750310735_000.zip | Zip | Windows archive |