Linear thermal expansion coefficient of fcc Ni at 293.15 K under a pressure of 0 MPa v001

Models

EAM_CubicNaturalSpline__MD_853402641673_002

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_AngeloMoody_1995_Ni__MO_800536961967_003		view	5005524

EAM_Dynamo__MD_120291908751_005

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_005	view	3004183
EAM_Dynamo_AcklandTichyVitek_1987v2_Ni__MO_769632475533_000	view	2575978
EAM_Dynamo_AdamsFoilesWolfer_1989Universal6_Ni__MO_258836200237_000	view	6252410
EAM_Dynamo_AngeloMoodyBaskes_1995_NiAlH__MO_418978237058_005	view	9539760
EAM_Dynamo_BelandLuOsetskiy_2016_CoNi__MO_871937946490_000	view	23450014
EAM_Dynamo_BelandTammMu_2017_FeNiCr__MO_715003088863_000	view	22182207
EAM_Dynamo_BonnyCastinTerentyev_2013_FeNiCr__MO_763197941039_000	view	3612262
EAM_Dynamo_BonnyPasianotCastin_2009_FeCuNi__MO_469343973171_005	view	8055342
EAM_Dynamo_BonnyPasianotMalerba_2009_FeNi__MO_267721408934_005	view	7688748
EAM_Dynamo_BonnyTerentyevPasianot_2011_FeNiCr__MO_677715648236_000	view	19765129
EAM_Dynamo_DeluigiPasianotValencia_2021_FeNiCrCoCu__MO_657255834688_000	view	18072618
EAM_Dynamo_FarkasCaro_2018_FeNiCrCoCu__MO_803527979660_000	view	17475499
EAM_Dynamo_FarkasCaro_2020_FeNiCrCoAl__MO_820335782779_000	view	16580337
EAM_Dynamo_FischerSchmitzEich_2019_CuNi__MO_266134052596_000	view	15422685
EAM_Dynamo_Foiles_1985_Ni__MO_010059867259_000	view	5522069
EAM_Dynamo_FoilesBaskesDaw_1986Universal3_Ni__MO_580571659842_000	view	4866007
EAM_Dynamo_FoilesHoyt_2006_Ni__MO_776437554506_000	view	9086831
EAM_Dynamo_MendelevBorovikov_2020_FeNiCr__MO_922363340570_000	view	14182387
EAM_Dynamo_MendelevKramerHao_2012_Ni__MO_832600236922_005	view	12006016
EAM_Dynamo_MendelevKramerHao_2012_NiZr__MO_149104665840_005	view	24332913
EAM_Dynamo_Mishin_2004_NiAl__MO_101214310689_005	view	8338797
EAM_Dynamo_MishinFarkasMehl_1999_Ni__MO_400591584784_005	view	12735045
EAM_Dynamo_MishinMehlPapaconstantopoulos_2002_NiAl__MO_109933561507_005 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	16135252
EAM_Dynamo_OnatDurukanoglu_2014_CuNi__MO_592013496703_005	view	12997291
EAM_Dynamo_PanBorovikovMendelev_2108_AgNi__MO_222110751402_000	view	32658576
EAM_Dynamo_PunMishin_2009_NiAl__MO_751354403791_005 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	9109124
EAM_Dynamo_PunYamakovMishin_2013_NiAlCo__MO_826591359508_000	view	10083477
EAM_Dynamo_PunYamakovMishin_2015_NiCo__MO_010613863288_000	view	10119688
EAM_Dynamo_SamolyukBelandStocks_2016_NiPd__MO_532072268679_000	view	55698830
EAM_Dynamo_StollerTammBeland_2016_Ni__MO_103383163946_000	view	12938224
EAM_Dynamo_TehranchiCurtin_2010_NiH__MO_535504325462_003	view	9188136
EAM_Dynamo_WilsonMendelev_2015_NiZr__MO_306032198193_000	view	24303995
EAM_Dynamo_ZhangAshcraftMendelev_2016_NiNb__MO_047308317761_000	view	17647660
EAM_Dynamo_ZhouFosterSills_2018_FeNiCr__MO_036303866285_000	view	31228755
EAM_Dynamo_ZhouJohnsonWadley_2004_Ni__MO_110256178378_005	view	6534937
EAM_Dynamo_ZhouWadleyJohnson_2001NISTretabulation_Ni__MO_593762436933_000	view	7910784

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	25274029
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_Ni__MO_108408461881_001		view	15914272

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	53050969
MEAM_LAMMPS_ChoiJoSohn_2018_CoNiCrFeMn__MO_115454747503_002	view	145530707
MEAM_LAMMPS_ChoiKimSeol_2017_NiMn__MO_348689608050_002	view	88541093
MEAM_LAMMPS_CostaAgrenClavaguera_2007_AlNi__MO_131642768288_002	view	245571853
MEAM_LAMMPS_EtesamiAsadi_2018_Ni__MO_937008984446_002	view	75711028
MEAM_LAMMPS_JeongParkDo_2018_PdNi__MO_008996216289_002	view	148626980
MEAM_LAMMPS_KavousiNovakBaskes_2019_NiTi__MO_050461957184_002	view	90051344
MEAM_LAMMPS_KimJungLee_2015_NiAlCo__MO_876687166519_002	view	196248400
MEAM_LAMMPS_KimKimJung_2017_NiAlTi__MO_478967255435_002	view	179362876
MEAM_LAMMPS_KimSeolJi_2017_PtNi__MO_020840179467_002	view	33956599
MEAM_LAMMPS_KoGrabowskiNeugebauer_2015_NiTi__MO_663355627503_002	view	69183879
MEAM_LAMMPS_KoShimLee_2011_NiH__MO_091278480940_002	view	65868998
MEAM_LAMMPS_LeeShim_2004_NiCu__MO_409065472403_002	view	65833071
MEAM_LAMMPS_LeeShimBaskes_2003_Ni__MO_000553624872_001	view	65812163
MEAM_LAMMPS_MahataMukhopadhyayAsleZaeem_2022_AlNi__MO_461927113651_001	view	70908893
MEAM_LAMMPS_MaiselKoZhang_2017_VNiTi__MO_744610363128_002	view	127556203
MEAM_LAMMPS_ShimKoKim_2013_NiVH__MO_612225165948_002	view	206034331
MEAM_LAMMPS_ShimParkCho_2003_NiW__MO_500937681860_002	view	175281282
MEAM_LAMMPS_Wagner_2007_Ni__MO_444394830472_002	view	62303262
MEAM_LAMMPS_WuLeeSu_2017_NiCr__MO_880803040302_002	view	65789119
MEAM_LAMMPS_WuLeeSu_2017_NiCrFe__MO_912636107108_002	view	66225762
MEAM_LAMMPS_WuLeeSu_2017_NiFe__MO_321233176498_002	view	54988669

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	38492488
Morse_Shifted_GirifalcoWeizer_1959LowCutoff_Ni__MO_322509103239_004	view	11071707
Morse_Shifted_GirifalcoWeizer_1959MedCutoff_Ni__MO_758825945924_004	view	22390262

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	325896822
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	494023095
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	1007622395
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	2954898944

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	8372353
Sim_LAMMPS_ADP_XuWangQian_2022_NiPd__SM_559286646876_000	view	25858725
Sim_LAMMPS_ADP_XuWangQian_2022_NiRh__SM_306597220004_000	view	43268760
Sim_LAMMPS_HybridOverlay_BelandLuOsetskiy_2016_CoNi__SM_445377835613_001	view	19337676
Sim_LAMMPS_MEAM_AsadiZaeemNouranian_2015_Ni__SM_078420412697_000	view	37034337
Sim_LAMMPS_MEAM_KoGrabowskiNeugebauer_2015_NiTi__SM_770142935022_000	view	37889883
Sim_LAMMPS_MEAM_Wagner_2007_Ni__SM_168413969663_000	view	16598324

Title A single sentence description.	Linear thermal expansion coefficient of fcc Ni at 293.15 K under a pressure of 0 MPa v001
Description	Linear thermal expansion coefficient of a fcc lattice of Ni atoms at a temperature of 293.15 K under a pressure of 0 MPa.
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.	None

Contributor	Mingjian Wen
Maintainer	Mingjian Wen
Published on KIM	2019
How to Cite	Click here to download this citation in BibTeX format.
Funding	Not available

Short KIM ID The unique KIM identifier code.	TE_127978642829_001
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.	LinearThermalExpansionCoeffCubic_fcc_Ni__TE_127978642829_001
Citable Link	https://openkim.org/cite/TE_127978642829_001
KIM Item Type	Test
Driver	LinearThermalExpansionCoeffCubic__TD_522633393614_001
Properties Properties as defined in kimspec.edn. These properties are inhereted from the Test Driver.	tag:staff@noreply.openkim.org,2015-07-30:property/linear-thermal-expansion-coefficient-cubic-crystal-npt
KIM API Version	2.0
Simulator Name The name of the simulator as defined in kimspec.edn. This Simulator Name is inhereted from the Test Driver.	LAMMPS
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	LinearThermalExpansionCoeffCubic_fcc_Ni__TE_127978642829_000

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LinearThermalExpansionCoeffCubic_fcc_Ni__TE_127978642829_001

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EAM_IMD_BrommerGaehler_2006A_AlNiCo__MO_122703700223_003	other	view
EAM_IMD_BrommerGaehler_2006B_AlNiCo__MO_128037485276_003	other	view