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SurfaceEnergyCubicCrystalBrokenBondFit_fcc_Ne__TE_285248425547_004

Title
A single sentence description.
Broken-bond fit of high-symmetry surface energies in fcc Ne v004
Description Computes the formation energy of several high-symmetry surfaces in fcc Ne and uses them to fit a broken-bond model
Species
The supported atomic species.
Ne
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 Ne 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_285248425547_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_Ne__TE_285248425547_004
Citable Link https://openkim.org/cite/TE_285248425547_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_Ne__TE_285248425547_003


Models

LJ_Shifted__MD_498634107543_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)
LJ_Shifted_Bernardes_1958HighCutoff_Ne__MO_966254629593_003 view 65098
LJ_Shifted_Bernardes_1958LowCutoff_Ne__MO_466741694288_003 view 18842
LJ_Shifted_Bernardes_1958MedCutoff_Ne__MO_160637895352_003 view 32309
LJ__MD_414112407348_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)
LJ_ElliottAkerson_2015_Universal__MO_959249795837_003 view 467455
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_Glyde_1970_Ne__MO_169434419764_002 view 21465
No Driver
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)
Exp6_KongChakrabarty_1973_ArNe__MO_946046425752_002 view 23096


Errors

  • No Errors associated with this Test




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