Title
A single sentence description.
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MEAM potential for Li-Si alloys developed by Cui et al. (2012) v001 |
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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 second nearest-neighbor modified embedded atom method (2NN MEAM) interatomic potential for lithium-silicon (Li-Si) alloys developed by using the particle swarm optimization (PSO) method in conjunction with ab initio calculations. This interatomic potential is capable of simulating the transition from disordered to ordered states of Li-Si crystalline structures, an indication of the stability and robustness of the interatomic potential at finite temperature. In the paper (Cui et al., J. Power Sources, 207:150-159, 2012), examples are given demonstrating that the new interatomic potential is also capable of predicting the material properties of both crystalline and amorphous Li-Si alloys, including the elastic modulus, compositional expansion, the diffusivity of Li in Li-Si alloys, and plastic yield strength. |
Species
The supported atomic species.
| Li, Si |
Disclaimer
A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.
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None |
Content Origin | https://doi.org/10.1016/j.jpowsour.2012.01.145\nhttps://doi.org/10.1088/0965-0393/20/1/015014 |
Content Other Locations | https://openkim.org/id/MEAM_2NN_LiSi__MO_596436139350_001 (retired)\nhttps://openkim.org/id/Sim_LAMMPS_MEAM_CuiGaoCui_2012_LiSi__SM_562938628131_000 |
Contributor |
Yaser Afshar |
Maintainer |
Yaser Afshar |
Developer |
Zhiwei Cui Feng Gao Zhihua Cui Jianmin Qu |
Published on KIM | 2021 |
How to Cite | Click here to download this citation in BibTeX format. |
Funding | Not available |
Short KIM ID
The unique KIM identifier code.
| MO_557492625287_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.
| MEAM_LAMMPS_CuiGaoCui_2012_LiSi__MO_557492625287_001 |
DOI |
10.25950/8b4eca6b https://doi.org/10.25950/8b4eca6b https://commons.datacite.org/doi.org/10.25950/8b4eca6b |
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 MEAM_LAMMPS__MD_249792265679_001 |
Driver | MEAM_LAMMPS__MD_249792265679_001 |
KIM API Version | 2.2 |
Potential Type | meam |
Previous Version | MEAM_LAMMPS_CuiGaoCui_2012_LiSi__MO_557492625287_000 |
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 |
F | 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 |
P | 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 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.
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.
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 Li v004 | view | 7549 | |
Cohesive energy versus lattice constant curve for bcc Si v004 | view | 7519 | |
Cohesive energy versus lattice constant curve for diamond Li v004 | view | 7450 | |
Cohesive energy versus lattice constant curve for diamond Si v004 | view | 9865 | |
Cohesive energy versus lattice constant curve for fcc Li v004 | view | 7768 | |
Cohesive energy versus lattice constant curve for fcc Si v004 | view | 9718 | |
Cohesive energy versus lattice constant curve for sc Li v004 | view | 9939 | |
Cohesive energy versus lattice constant curve for sc Si v004 | view | 9644 |
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 bcc Li at zero temperature v006 | view | 39048 | |
Elastic constants for bcc Si at zero temperature v006 | view | 17518 | |
Elastic constants for diamond Li at zero temperature v001 | view | 34328 | |
Elastic constants for diamond Si at zero temperature v001 | view | 98734 | |
Elastic constants for fcc Li at zero temperature v006 | view | 18711 | |
Elastic constants for fcc Si at zero temperature v006 | view | 39605 | |
Elastic constants for sc Li at zero temperature v006 | view | 29937 | |
Elastic constants for sc Si at zero temperature v006 | view | 29201 |
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) |
---|---|---|---|
Equilibrium zero-temperature lattice constant for bcc Li v007 | view | 34961 | |
Equilibrium zero-temperature lattice constant for bcc Si v007 | view | 20127 | |
Equilibrium zero-temperature lattice constant for diamond Li v007 | view | 19232 | |
Equilibrium zero-temperature lattice constant for diamond Si v007 | view | 25681 | |
Equilibrium zero-temperature lattice constant for fcc Li v007 | view | 23444 | |
Equilibrium zero-temperature lattice constant for fcc Si v007 | view | 24338 | |
Equilibrium zero-temperature lattice constant for sc Li v007 | view | 16251 | |
Equilibrium zero-temperature lattice constant for sc Si v007 | view | 17294 |
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) |
---|---|---|---|
Equilibrium lattice constants for hcp Li v005 | view | 439255 | |
Equilibrium lattice constants for hcp Si v005 | view | 584239 |
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) |
---|---|---|---|
Linear thermal expansion coefficient of bcc Li at 293.15 K under a pressure of 0 MPa v001 | view | 14317545 |
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) |
---|---|---|---|
Broken-bond fit of high-symmetry surface energies in bcc Li v004 | view | 116848 |
Test | Error Categories | Link to Error page |
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Conjugate gradient relaxation of random finite cluster of Si atoms v003 | other | view |
Test | Error Categories | Link to Error page |
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Elastic constants for hcp Li at zero temperature v004 | other | view |
Elastic constants for hcp Si at zero temperature v004 | other | view |
Test | Error Categories | Link to Error page |
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Linear thermal expansion coefficient of diamond Si at 293.15 K under a pressure of 0 MPa v001 | other | view |
Verification Check | Error Categories | Link to Error page |
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MemoryLeak__VC_561022993723_004 | other | view |
PeriodicitySupport__VC_895061507745_004 | other | view |
MEAM_LAMMPS_CuiGaoCui_2012_LiSi__MO_557492625287_001.txz | Tar+XZ | Linux and OS X archive |
MEAM_LAMMPS_CuiGaoCui_2012_LiSi__MO_557492625287_001.zip | Zip | Windows archive |
This Model requires a Model Driver. Archives for the Model Driver MEAM_LAMMPS__MD_249792265679_001 appear below.
MEAM_LAMMPS__MD_249792265679_001.txz | Tar+XZ | Linux and OS X archive |
MEAM_LAMMPS__MD_249792265679_001.zip | Zip | Windows archive |