Title
A single sentence description.
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MEAM potential for BeO structure developed by Wei et al. (2019) v002 |
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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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Modified embedded atom method potential parameters of beryllium oxide (BeO) have been developed, which can reproduce the thermodynamic properties of beryllium oxide. To accurately describe the interactions between the atoms in the BeO structure, the density functional theory is used to calculate the fundamental properties such as the lattice constant, bulk modulus, and elastic constants, which are used for the potential fitting. The properties such as the enthalpy and specific heat are used to test the potential parameters' validity. The developed potential parameters' calculated results are compared with the experimental and other theoretical data as a function of temperature. The good agreement between the calculated results by the new potential and the experimental data verifies the potential parameters. The developed potential parameters have also been used to predict the thermal conductivity of BeO as a function of temperature for further applications of beryllium oxide. |
Species
The supported atomic species.
| Be, O |
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 | Files are provided by Wenzhong Zhou (Sun Yat-Sen University) on Feb 7, 2021, and posted with his permission. |
Contributor |
Yaser Afshar |
Maintainer |
Yaser Afshar |
Developer |
Jie Wei Wei Zhou Song Li Pei Shen Shuai Ren Alice Hu Wenzhong Zhou |
Published on KIM | 2023 |
How to Cite |
This Model originally published in [1] is archived in OpenKIM [2-5]. [1] Wei J, Zhou W, Li S, Shen P, Ren S, Hu A, et al. Modified Embedded Atom Method Potential for Modeling the Thermodynamic Properties of High Thermal Conductivity Beryllium Oxide. ACS Omega . 2019Apr;4(4):6339–46 . doi:10.1021/acsomega.9b00174 — (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] Wei J, Zhou W, Li S, Shen P, Ren S, Hu A, et al. MEAM potential for BeO structure developed by Wei et al. (2019) v002. OpenKIM; 2023. doi:10.25950/946e3852 [3] Afshar Y, Hütter S, Rudd RE, Stukowski A, Tipton WW, Trinkle DR, et al. The modified embedded atom method (MEAM) potential v002. OpenKIM; 2023. doi:10.25950/ee5eba52 [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_344044439515_002 |
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_WeiZhouLi_2019_BeO__MO_344044439515_002 |
DOI |
10.25950/946e3852 https://doi.org/10.25950/946e3852 https://commons.datacite.org/doi.org/10.25950/946e3852 |
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_002 |
Driver | MEAM_LAMMPS__MD_249792265679_002 |
KIM API Version | 2.2 |
Potential Type | meam |
Previous Version | MEAM_LAMMPS_WeiZhouLi_2019_BeO__MO_344044439515_001 |
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 |
N/A | 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 |
N/A | 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 Be v004 | view | 6626 | |
Cohesive energy versus lattice constant curve for diamond O v004 | view | 8464 | |
Cohesive energy versus lattice constant curve for fcc Be v004 | view | 6505 | |
Cohesive energy versus lattice constant curve for sc Be v004 | view | 6296 |
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 Be at zero temperature v006 | view | 43275 | |
Elastic constants for diamond O at zero temperature v001 | view | 130750 | |
Elastic constants for fcc Be at zero temperature v006 | view | 35338 | |
Elastic constants for sc Be at zero temperature v006 | view | 32951 |
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 Be v007 | view | 9865 | |
Equilibrium zero-temperature lattice constant for diamond O v007 | view | 14382 | |
Equilibrium zero-temperature lattice constant for fcc Be v007 | view | 13467 | |
Equilibrium zero-temperature lattice constant for sc Be v007 | view | 15681 |
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 Be v005 | view | 186702 | |
Equilibrium lattice constants for hcp O v005 | view | 174493 |
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) |
---|---|---|---|
Monovacancy formation energy and relaxation volume for hcp Be | view | 2898954 |
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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Vacancy formation and migration energy for hcp Be | view | 1760119 |
Test | Error Categories | Link to Error page |
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Elastic constants for hcp Be at zero temperature v004 | other | view |
Elastic constants for hcp O at zero temperature v004 | other | view |
Test | Error Categories | Link to Error page |
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Equilibrium crystal structure and energy for BeO in AFLOW crystal prototype AB_cF8_225_a_b v000 | other | view |
Test | Error Categories | Link to Error page |
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Equilibrium zero-temperature lattice constant for bcc O v007 | other | view |
Equilibrium zero-temperature lattice constant for diamond Be v007 | other | view |
Equilibrium zero-temperature lattice constant for fcc O v007 | other | view |
Equilibrium zero-temperature lattice constant for sc O v007 | other | view |
Verification Check | Error Categories | Link to Error page |
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DimerContinuityC1__VC_303890932454_005 | other | view |
MEAM_LAMMPS_WeiZhouLi_2019_BeO__MO_344044439515_002.txz | Tar+XZ | Linux and OS X archive |
MEAM_LAMMPS_WeiZhouLi_2019_BeO__MO_344044439515_002.zip | Zip | Windows archive |
This Model requires a Model Driver. Archives for the Model Driver MEAM_LAMMPS__MD_249792265679_002 appear below.
MEAM_LAMMPS__MD_249792265679_002.txz | Tar+XZ | Linux and OS X archive |
MEAM_LAMMPS__MD_249792265679_002.zip | Zip | Windows archive |