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SurfaceEnergyCubicCrystalBrokenBondFit_fcc_Ca__TE_402264927720_004

Title
A single sentence description.
Broken-bond fit of high-symmetry surface energies in fcc Ca v004
Description Computes the formation energy of several high-symmetry surfaces in fcc Ca and uses them to fit a broken-bond model
Species
The supported atomic species.
Ca
Disclaimer
A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.
Computer-generated
Contributor mattbierbaum
Maintainer mattbierbaum
Author Matt Bierbaum
Publication Year 2019
Item Citation

This Test is archived in OpenKIM [1-4].

[1] Bierbaum M. Broken-bond fit of high-symmetry surface energies in fcc Ca v004. OpenKIM; 2019.

[2] Bierbaum M. High-symmetry surface energies in cubic lattices and broken bond model v004. OpenKIM; 2019. doi:10.25950/6c43a4e6

[3] 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

[4] 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.
Short KIM ID
The unique KIM identifier code.
TE_402264927720_004
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.
SurfaceEnergyCubicCrystalBrokenBondFit_fcc_Ca__TE_402264927720_004
Citable Link https://openkim.org/cite/TE_402264927720_004
KIM Item TypeTest
DriverSurfaceEnergyCubicCrystalBrokenBondFit__TD_955413365818_004
Properties
Properties as defined in kimspec.edn. These properties are inhereted from the Test Driver.
KIM API Version2.0
Simulator Name
The name of the simulator as defined in kimspec.edn. This Simulator Name is inhereted from the Test Driver.
ase
Programming Language(s)
The programming languages used in the code and the percentage of the code written in each one.
100.00% Python
Previous Version SurfaceEnergyCubicCrystalBrokenBondFit_fcc_Ca__TE_402264927720_003


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Usertime muliplied 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)
EAM_IMD_BrommerGaehlerMihalkovic_2007_CaCd__MO_145183423516_003 view 19257
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Model Test Results Link to Test Results page Benchmark time
Usertime muliplied 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)
LJ_ElliottAkerson_2015_Universal__MO_959249795837_003 view 62123
Morse_Shifted__MD_552566534109_002
Model Test Results Link to Test Results page Benchmark time
Usertime muliplied 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)
Morse_Shifted_GirifalcoWeizer_1959HighCutoff_Ca__MO_159753408472_002 view 171525
Morse_Shifted_GirifalcoWeizer_1959LowCutoff_Ca__MO_887105884651_002 view 41170
Morse_Shifted__MD_552566534109_003
Model Test Results Link to Test Results page Benchmark time
Usertime muliplied 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)
Morse_Shifted_GirifalcoWeizer_1959MedCutoff_Ca__MO_562200212426_003 view 141135


Errors

  • No Errors associated with this Test




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