Equilibrium crystal structure and energy for Ni in AFLOW crystal prototype A_cF4_225_a v003

I Nikiforov; Ellad B. Tadmor; Daniel S. Karls; Moon-ki Choi

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EquilibriumCrystalStructure_A_cF4_225_a_Ni__TE_409545778110_003

Title A single sentence description.	Equilibrium crystal structure and energy for Ni in AFLOW crystal prototype A_cF4_225_a v003
Description	Computes the equilibrium crystal structure and energy for Ni in AFLOW crystal prototype A_cF4_225_a at zero temperature and applied stress by performing symmetry-constrained relaxation. The following initial guess for the parameters (representing cell and internal degrees of freedom) allowed to vary during the relaxation is used: a (angstrom): 3.5048, obtained from OpenKIM Reference Data item RD_300642565223_000
Species The supported atomic species.	Ni
Disclaimer A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.	Computer generated

Contributor	I Nikiforov
Maintainer	I Nikiforov
Developer	I Nikiforov Ellad B. Tadmor Daniel S. Karls Moon-ki Choi
Published on KIM	2025
How to Cite	This Test is archived in OpenKIM [1-4]. [1] Nikiforov I, Tadmor EB, Karls DS, Choi M-ki. Equilibrium crystal structure and energy for Ni in AFLOW crystal prototype A_cF4_225_a v003 [Internet]. OpenKIM; 2025. Available from: https://openkim.org/cite/TE_409545778110_003 [2] Nikiforov I, Tadmor EB. Equilibrium structure and energy for a crystal structure at zero temperature and pressure v003. OpenKIM; 2025. doi:10.25950/866c7cfa [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
Funding	Not available

Short KIM ID The unique KIM identifier code.	TE_409545778110_003
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.	EquilibriumCrystalStructure_A_cF4_225_a_Ni__TE_409545778110_003
Citable Link	https://openkim.org/cite/TE_409545778110_003
KIM Item Type	Test
Driver	EquilibriumCrystalStructure__TD_457028483760_003
Properties Properties as defined in kimspec.edn. These properties are inhereted from the Test Driver.	tag:staff@noreply.openkim.org,2023-02-21:property/binding-energy-crystal tag:staff@noreply.openkim.org,2023-02-21:property/crystal-structure-npt tag:staff@noreply.openkim.org,2025-04-15:property/mass-density-crystal-npt
KIM API Version	2.3
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	EquilibriumCrystalStructure_A_cF4_225_a_Ni__TE_409545778110_002

Models

EAM_CubicNaturalSpline__MD_853402641673_003

Model	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)
EAM_CubicNaturalSpline_AngeloMoodyBaskes_1995_Ni__MO_800536961967_004		view	206021

EAM_Dynamo__MD_120291908751_006

Model	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)
EAM_Dynamo_AcklandTichyVitek_1987_Ni__MO_977363131043_006	view	150563
EAM_Dynamo_AcklandTichyVitek_1987v2_Ni__MO_769632475533_001	view	217631
EAM_Dynamo_AdamsFoilesWolfer_1989Universal6_Ni__MO_258836200237_001	view	176100
EAM_Dynamo_AngeloMoodyBaskes_1995_NiAlH__MO_418978237058_006	view	175920
EAM_Dynamo_BelandLuOsetskiy_2016_CoNi__MO_871937946490_001	view	213227
EAM_Dynamo_BelandTammMu_2017_FeNiCr__MO_715003088863_001	view	215309
EAM_Dynamo_BonnyCastinTerentyev_2013_FeNiCr__MO_763197941039_001	view	140173
EAM_Dynamo_BonnyPasianotCastin_2009_FeCuNi__MO_469343973171_006	view	180959
EAM_Dynamo_BonnyPasianotMalerba_2009_FeNi__MO_267721408934_006	view	168660
EAM_Dynamo_BonnyTerentyevBakaev_2013_FeCuNiMn__MO_398449950394_000	view	167520
EAM_Dynamo_BonnyTerentyevPasianot_2011_FeNiCr__MO_677715648236_001	view	138594
EAM_Dynamo_DaramolaBonnyAdjanor_2022_FeNiCrMn__MO_591022523366_000	view	177600
EAM_Dynamo_DeluigiPasianotValencia_2021_FeNiCrCoCu__MO_657255834688_001	view	143211
EAM_Dynamo_FarkasCaro_2018_FeNiCrCoCu__MO_803527979660_001	view	140113
EAM_Dynamo_FarkasCaro_2020_FeNiCrCoAl__MO_820335782779_001	view	220994
EAM_Dynamo_FischerSchmitzEich_2019_CuNi__MO_266134052596_001	view	162300
EAM_Dynamo_Foiles_1985_Ni__MO_010059867259_001	view	155400
EAM_Dynamo_FoilesBaskesDaw_1986Universal3_Ni__MO_580571659842_001	view	206021
EAM_Dynamo_FoilesHoyt_2006_Ni__MO_776437554506_001	view	210505
EAM_Dynamo_MendelevBorovikov_2020_FeNiCr__MO_922363340570_001	view	139080
EAM_Dynamo_MendelevKramerHao_2012_Ni__MO_832600236922_006	view	139444
EAM_Dynamo_MendelevKramerHao_2012_NiZr__MO_149104665840_006	view	178877
EAM_Dynamo_Mishin_2004_NiAl__MO_101214310689_006	view	182880
EAM_Dynamo_MishinFarkasMehl_1999_Ni__MO_400591584784_006	view	133429
EAM_Dynamo_MishinMehlPapaconstantopoulos_2002_NiAl__MO_109933561507_006 This Model has a disclaimer This potential was developed to accurately reproduce properties of a single phase of the Ni-Al system, namely, B2-NiAl. Properties of other phases of this system are reproduced less accurately. Application of this particular potential to simulations of pure Ni or pure Al is not recommended.	view	162660
EAM_Dynamo_OnatDurukanoglu_2014_CuNi__MO_592013496703_006	view	138594
EAM_Dynamo_PanBorovikovMendelev_2108_AgNi__MO_222110751402_001	view	170979
EAM_Dynamo_PunMishin_2009_NiAl__MO_751354403791_006 This Model has a disclaimer The paper reporting on this potential (G.P. Purja Pun and Y. Mishin, "Development of an interatomic potential for the Ni-Al system," Phil. Mag. 89, 3245 (2009)) contains an error in Table 6. The generalized stacking fault energies in Ni3Al listed in this table are incorrect. The correct energies computed with the new potential are (in J/m2): APB (111) 180 CSF (111) 229 SISF (111) 21 APB (100) 20	view	210424
EAM_Dynamo_PunYamakovMishin_2013_NiAlCo__MO_826591359508_001	view	212907
EAM_Dynamo_PunYamakovMishin_2015_NiCo__MO_010613863288_001	view	161940
EAM_Dynamo_SamolyukBelandStocks_2016_NiPd__MO_532072268679_001	view	217631
EAM_Dynamo_StollerTammBeland_2016_Ni__MO_103383163946_001	view	166140
EAM_Dynamo_TehranchiCurtin_2010_NiH__MO_535504325462_004	view	216990
EAM_Dynamo_VoterChen_1993_Ni__MO_071073566434_001	view	174017
EAM_Dynamo_WilsonMendelev_2015_NiZr__MO_306032198193_001	view	158640
EAM_Dynamo_ZhangAshcraftMendelev_2016_NiNb__MO_047308317761_001	view	133247
EAM_Dynamo_ZhouFosterSills_2018_FeNiCr__MO_036303866285_001	view	179880
EAM_Dynamo_ZhouJohnsonWadley_2004_CuAgAuNiPdPtAlPbFeMoTaWMgCoTiZr__MO_870117231765_001	view	230122
EAM_Dynamo_ZhouJohnsonWadley_2004_Ni__MO_110256178378_006	view	292620
EAM_Dynamo_ZhouJohnsonWadley_2004NISTretabulation_Ni__MO_593762436933_001	view	236607

EAM_IMD__MD_113599595631_003

Model	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)
EAM_IMD_BrommerGaehler_2006A_AlNiCo__MO_122703700223_003		view	228200
EAM_IMD_BrommerGaehler_2006B_AlNiCo__MO_128037485276_003		view	162108

EMT_Asap__MD_128315414717_004

Model	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)
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_AlAgAuCuNiPdPt__MO_115316750986_001		view	145034
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_Ni__MO_108408461881_001		view	144487

GEAM_LAMMPS__MD_810175167647_001

Model	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)
GEAM_LAMMPS_ZhaoSamanta_2024_FeNi__MO_361455675661_000		view	135191

LJ__MD_414112407348_003

Model	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)
LJ_ElliottAkerson_2015_Universal__MO_959249795837_003 This Model has a disclaimer This model was automatically fit using Lorentz-Berthelot mixing rules. It reproduces the dimer equilibrium separation (covalent radii) and the bond dissociation energies. It has not been fitted to other physical properties and its ability to model structures other than dimers is unknown.		view	241572

MEAM_LAMMPS__MD_249792265679_002

Model	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)
MEAM_LAMMPS_AsadiZaeemNouranian_2015_Ni__MO_700541006254_002	view	211305
MEAM_LAMMPS_ChoiJoSohn_2018_CoNiCrFeMn__MO_115454747503_002	view	162837
MEAM_LAMMPS_ChoiKimSeol_2017_NiMn__MO_348689608050_002	view	214988
MEAM_LAMMPS_CostaAgrenClavaguera_2007_AlNi__MO_131642768288_002	view	208823
MEAM_LAMMPS_EtesamiAsadi_2018_Ni__MO_937008984446_002	view	170857
MEAM_LAMMPS_JeongParkDo_2018_PdNi__MO_008996216289_002	view	212106
MEAM_LAMMPS_KavousiNovakBaskes_2019_NiTi__MO_050461957184_002	view	210505
MEAM_LAMMPS_KimJungLee_2015_NiAlCo__MO_876687166519_002	view	159860
MEAM_LAMMPS_KimKimJung_2017_NiAlTi__MO_478967255435_002	view	207302
MEAM_LAMMPS_KimSeolJi_2017_PtNi__MO_020840179467_002	view	219072
MEAM_LAMMPS_KoGrabowskiNeugebauer_2015_NiTi__MO_663355627503_002	view	212106
MEAM_LAMMPS_KoShimLee_2011_NiH__MO_091278480940_002	view	213467
MEAM_LAMMPS_LeeShim_2004_NiCu__MO_409065472403_002	view	211706
MEAM_LAMMPS_LeeShimBaskes_2003_Ni__MO_000553624872_001	view	205540
MEAM_LAMMPS_MahataMukhopadhyayAsleZaeem_2022_AlNi__MO_461927113651_001	view	159981
MEAM_LAMMPS_MaiselKoZhang_2017_VNiTi__MO_744610363128_002	view	160346
MEAM_LAMMPS_MurallesParkKim_NiTi__MO_182729415169_000	view	159799
MEAM_LAMMPS_SharifiWick_2025_FeMnNiTiCuCrCoAl__MO_675947402254_000 This Model has a disclaimer This potential is designed for the structural properties of High Entropy Alloys (HEA)s and Complex Concentrated Alloys (CCAs). The fitting procedure involved developing all included unary, binary and ternary systems so it can be used for any alloy subset. This potential focuses on the structural analysis of alloys including shear strength and elastic constants, dislocation dynamics and their impact on alloy strength, and the analysis of defect effects, such as voids, on material properties. However, the potential was not optimized for temperature-dependent properties and was not fit to density, thermal expansion coefficients, or thermal conductivity data.	view	227079
MEAM_LAMMPS_ShimKoKim_2013_NiVH__MO_612225165948_002	view	211305
MEAM_LAMMPS_ShimParkCho_2003_NiW__MO_500937681860_002	view	210745
MEAM_LAMMPS_Wagner_2007_Ni__MO_444394830472_002	view	161014
MEAM_LAMMPS_WuLeeSu_2017_NiCr__MO_880803040302_002	view	210424
MEAM_LAMMPS_WuLeeSu_2017_NiCrFe__MO_912636107108_002	view	215709
MEAM_LAMMPS_WuLeeSu_2017_NiFe__MO_321233176498_002	view	161318

Morse_Shifted__MD_552566534109_004

Model	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)
Morse_Shifted_GirifalcoWeizer_1959HighCutoff_Ni__MO_381861218831_004	view	218512
Morse_Shifted_GirifalcoWeizer_1959LowCutoff_Ni__MO_322509103239_004	view	227880
Morse_Shifted_GirifalcoWeizer_1959MedCutoff_Ni__MO_758825945924_004	view	180078

SNAP__MD_536750310735_000

Model	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)
SNAP_LiHuChen_2018_Ni__MO_913991514986_000 This Model has a disclaimer This potential is designed for Ni fcc systems. It is not appropriate for other elements. The potential was trained using LAMMPS version 17Nov2016. Newer LAMMPS may see energy differences, but the relative values should remain to be the same.	view	174953
SNAP_LiHuChen_2018_NiMo__MO_468686727341_000 This Model has a disclaimer This potential is designed for Ni-Mo chemistries, including both the elementary and binary systems. The potential was trained using LAMMPS version 17Nov2016. Newer LAMMPS may see energy differences, but the relative values should remain to be the same.	view	184402
SNAP_ZuoChenLi_2019_Ni__MO_365106510449_000 This Model has a disclaimer This potential is designed for Ni fcc systems. It is not appropriate for other elements. The potential was trained using LAMMPS version 12Dec2018. Newer LAMMPS may see energy differences, but the relative values should remain to be the same.	view	177298
SNAP_ZuoChenLi_2019quadratic_Ni__MO_263593395744_000 This Model has a disclaimer This potential is designed for Ni fcc systems. It is not appropriate for other elements. The potential was trained using LAMMPS version 12Dec2018. Newer LAMMPS may see energy differences, but the relative values should remain to be the same.	view	178088

No Driver

Model	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)
Sim_LAMMPS_ADP_MishinMehlPapaconstantopoulos_2005_Ni__SM_477692857359_000	view	156275
Sim_LAMMPS_ADP_XuWangQian_2022_NiPd__SM_559286646876_000	view	202337
Sim_LAMMPS_ADP_XuWangQian_2022_NiRh__SM_306597220004_000	view	161257
Sim_LAMMPS_Buckingham_FisherMatsubara_2005_NiO__SM_337243826931_000	view	161500
Sim_LAMMPS_HybridOverlay_BelandLuOsetskiy_2016_CoNi__SM_445377835613_001	view	153054
Sim_LAMMPS_MEAM_AsadiZaeemNouranian_2015_Ni__SM_078420412697_001	view	188325
Sim_LAMMPS_MEAM_EtesamiAsadi_2018_Ni__SM_333792531460_001	view	191528
Sim_LAMMPS_MEAM_KoGrabowskiNeugebauer_2015_NiTi__SM_770142935022_000	view	138958
Sim_LAMMPS_MEAM_MaiselKoZhang_2017_VNiTi__SM_971529344487_000	view	137075
Sim_LAMMPS_MEAM_Wagner_2007_Ni__SM_168413969663_000	view	156000
Sim_LAMMPS_Table_GrogerVitekDlouhy_2020_CoCrFeMnNi__SM_786004631953_001	view	167090

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