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LatticeConstantHexagonalEnergy_hcp_Y__TE_541022626225_005

Title
A single sentence description.
Equilibrium lattice constants for hcp Y v005
Description Computes the equilibrium lattice constants for hcp Y at zero temperature and pressure using simplex minimization.
Species
The supported atomic species.
Y
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
Published on KIM 2019
How to Cite

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

[1] Equilibrium lattice constants for hcp Y 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_541022626225_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_Y__TE_541022626225_005
Citable Link https://openkim.org/cite/TE_541022626225_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_Y__TE_541022626225_004


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 210309
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_KimJeonLee_2015_MgY__MO_018428823000_000 view 33295
MEAM_LAMMPS_KoLee_2013_VPdY__MO_046547823135_000 view 38096
MEAM_LAMMPS__MD_249792265679_001
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_AhmadGrohGhazisaeidi_2018_MgY__MO_135739722270_001 view 389045


No Driver
Model Error Categories Link to Error page
Dipole_Umeno_YSZ__MO_394669891912_001 mismatch view




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LatticeConstantHexagonalEnergy__TD_942334626465_005.txz Tar+XZ Linux and OS X archive
LatticeConstantHexagonalEnergy__TD_942334626465_005.zip Zip Windows archive
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