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LatticeConstantHexagonalEnergy_hcp_Li__TE_343831449774_005

Title
A single sentence description.
Equilibrium lattice constants for hcp Li v005
Description Computes the equilibrium lattice constants for hcp Li at zero temperature and pressure using simplex minimization.
Species
The supported atomic species.
Li
Disclaimer
A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.
Computer generated
Contributor Junhao Li
Maintainer Junhao Li
Publication Year 2019
How to Cite

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

[1] Equilibrium lattice constants for hcp Li v005. OpenKIM; 2019.

[2] Equilibrium lattice constants for hexagonal bulk structures at zero temperature and pressure v005. OpenKIM; 2019. doi:10.25950/c339ca32

[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.
Funding Not available
Short KIM ID
The unique KIM identifier code.
TE_343831449774_005
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.
LatticeConstantHexagonalEnergy_hcp_Li__TE_343831449774_005
Citable Link https://openkim.org/cite/TE_343831449774_005
KIM Item TypeTest
DriverLatticeConstantHexagonalEnergy__TD_942334626465_005
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 LatticeConstantHexagonalEnergy_hcp_Li__TE_343831449774_004


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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 483971
MEAM_LAMMPS__MD_249792265679_000
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)
MEAM_LAMMPS_CuiGaoCui_2012_LiSi__MO_557492625287_000 view 24608
MEAM_LAMMPS_KimJungLee_2012_LiMg__MO_427397414195_000 view 27230
SNAP__MD_536750310735_000
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)
SNAP_ZuoChenLi_2019_Li__MO_732106099012_000 view 58023
SNAP_ZuoChenLi_2019quadratic_Li__MO_041269750353_000 view 40347
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)
Sim_LAMMPS_MEAM_CuiGaoCui_2012_LiSi__SM_562938628131_000 view 32755





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LatticeConstantHexagonalEnergy__TD_942334626465_005.zip Zip Windows archive

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