material_id stringlengths 13 15 | formula stringlengths 3 13 | reduced_formula stringlengths 3 13 | doi stringlengths 15 62 | n_atoms int64 4 20 | elements stringlengths 3 13 | n_frames int64 2 74 | first_ionic_step int64 0 3 | last_ionic_step int64 1 76 | energy_eV float64 -172 -22.68 | energy_per_atom_eV float64 -9.48 -3.29 | total_magmom_muB float64 0 0 | n_magnetic_sites int64 0 12 | max_abs_site_magmom_muB float64 0 4.69 | endpoint_fmax_eV_per_A float64 0 0.09 | occupancy_policy stringclasses 2
values | collinear_axis stringclasses 35
values |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
MAGNDATA_0_15 | MnF2 | F2Mn | 10.1139/p10-081 | 6 | F Mn | 3 | 0 | 2 | -38.584044 | -6.430674 | 0 | 2 | 4.689 | 0.029487 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_18 | BaMn2As2 | As2BaMn2 | 10.1103/physrevb.80.100403 | 10 | As Ba Mn | 7 | 0 | 6 | -65.820999 | -6.5821 | 0 | 4 | 3.463 | 0.015007 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_25 | NaOsO3 | NaO3Os | 10.1103/physrevlett.108.257209 | 20 | Na O Os | 5 | 0 | 4 | -134.408244 | -6.720412 | 0 | 4 | 1.176 | 0.045308 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_72 | CaMnBi2 | Bi2CaMn | 10.1103/PhysRevB.90.075120 | 8 | Bi Ca Mn | 10 | 0 | 9 | -40.098896 | -5.012362 | 0 | 2 | 3.755 | 0.042555 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_73 | SrMnBi2 | Bi2MnSr | 10.1103/PhysRevB.90.075120 | 16 | Bi Mn Sr | 6 | 0 | 5 | -79.763922 | -4.985245 | 0 | 4 | 3.837 | 0.043691 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_75 | Cr2WO6 | Cr2O6W | 10.1103/PhysRevLett.113.076406 | 18 | Cr O W | 7 | 0 | 6 | -140.255725 | -7.791985 | 0 | 4 | 2.928 | 0.01834 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_76 | Cr2TeO6 | Cr2O6Te | 10.1103/PhysRevLett.113.076406 | 18 | Cr O Te | 11 | 0 | 10 | -124.414551 | -6.911919 | 0 | 4 | 2.904 | 0.046257 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_79 | CaIrO3 | CaIrO3 | 10.1103/PhysRevLett.110.217212 | 20 | Ca Ir O | 8 | 0 | 7 | -136.550776 | -6.827539 | 0 | 0 | 0.404 | 0.021986 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_89 | BaMn2Bi2 | BaBi2Mn2 | 10.1103/PhysRevB.89.064417 | 10 | Ba Bi Mn | 6 | 0 | 5 | -57.984241 | -5.798424 | 0 | 4 | 3.793 | 0.021421 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_92 | CaMn2Sb2 | CaMn2Sb2 | 10.1016/j.jmmm.2009.03.054 | 5 | Ca Mn Sb | 8 | 0 | 7 | -30.091291 | -6.018258 | 0 | 2 | 3.814 | 0.024092 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_142 | Fe2TeO6 | Fe2O6Te | 10.1016/0022-3697(68)90187-X | 18 | Fe O Te | 7 | 0 | 6 | -111.759515 | -6.208862 | 0 | 4 | 4.332 | 0.003192 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_143 | Cr2TeO6 | Cr2O6Te | 10.1016/0022-3697(68)90187-X | 18 | Cr O Te | 11 | 0 | 10 | -124.41455 | -6.911919 | 0 | 4 | 2.904 | 0.04641 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_144 | Cr2WO6 | Cr2O6W | 10.1016/0022-3697(68)90187-X | 18 | Cr O W | 7 | 0 | 6 | -140.255726 | -7.791985 | 0 | 4 | 2.928 | 0.018232 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_163 | MnPS3 | MnPS3 | 10.1103/PhysRevB.82.100408 | 20 | Mn P S | 15 | 0 | 14 | -116.033654 | -5.801683 | 0 | 4 | 4.211 | 0.035858 | none | 0.42838283 0.00000000 0.90359734 |
MAGNDATA_0_178 | CoF2 | CoF2 | 10.1107/S0108767303022803 | 6 | Co F | 8 | 0 | 7 | -30.841112 | -5.140185 | 0 | 2 | 2.781 | 0.029727 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_201 | Ca2PrCr2NbO9 | CaCrO3 | 10.1016/j.jssc.2018.09.012 | 20 | Ca Cr O | 6 | 0 | 5 | -142.110301 | -7.105515 | 0 | 4 | 2.064 | 0.029294 | max_occupancy_site | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_202 | Ca2PrCr2TaO9 | CaCrO3 | 10.1016/j.jssc.2018.09.012 | 20 | Ca Cr O | 6 | 0 | 5 | -142.110889 | -7.105544 | 0 | 4 | 2.064 | 0.03427 | max_occupancy_site | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_212 | Sr2Mn3As2O2 | As2Mn3O2Sr2 | 10.1016/0925-8388(95)02066-7 | 18 | As Mn O Sr | 4 | 0 | 3 | -106.169723 | -5.898318 | 0 | 4 | 4.344 | 0.032366 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_213 | Sr2Mn2CuAs2O2 | As2Cu2MnO2Sr2 | 10.1103/PhysRevB.81.224513 | 18 | As Cu Mn O Sr | 10 | 0 | 9 | -99.439322 | -5.524407 | 0 | 2 | 4.328 | 0.045632 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_222 | CuMnAs | AsCuMn | 10.1038/srep17079 | 6 | As Cu Mn | 7 | 0 | 6 | -36.322529 | -6.053755 | 0 | 2 | 3.374 | 0.049853 | none | 0.00000000 -1.00000000 0.00000000 |
MAGNDATA_0_266 | Na2BaCo(VO4)2 | BaCoNa2O14V2 | 10.1021/acs.inorgchem.8b03418 | 20 | Ba Co Na O V | 25 | 0 | 25 | -111.44676 | -5.572338 | 0 | 1 | 2.368 | 0.040203 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_274 | Mn4N | Mn4N | 10.1103/PhysRev.125.1893 | 5 | Mn N | 4 | 0 | 3 | -45.169566 | -9.033913 | 0 | 0 | 0.001 | 0 | none | 0.57735027 0.57735027 0.57735027 |
MAGNDATA_0_275 | Mn3AlN | AlMn3N | 10.1103/PhysRev.125.1893 | 5 | Al Mn N | 3 | 0 | 2 | -41.433937 | -8.286787 | 0 | 3 | 1.015 | 0 | none | 0.57735027 0.57735027 0.57735027 |
MAGNDATA_0_276 | Mn3AlN | AlMn3N | 10.1103/PhysRev.125.1893 | 5 | Al Mn N | 3 | 0 | 2 | -41.433954 | -8.286791 | 0 | 3 | 1.019 | 0 | none | 0.70710678 0.70710678 0.00000000 |
MAGNDATA_0_286 | Mn5Ge3 | Ge3Mn5 | 10.1088/0953-8984/2/11/014 | 16 | Ge Mn | 12 | 0 | 11 | -120.453301 | -7.528331 | 0 | 10 | 3.087 | 0.041677 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_291 | Tl2NiMnO6 | MnNiO6Tl2 | 10.1016/j.actamat.2019.04.044 | 20 | Mn Ni O Tl | 12 | 0 | 11 | -105.951244 | -5.297562 | 0 | 4 | 1.778 | 0.048395 | max_occupancy_site | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_301 | Sr2CoTeO6 | CoO6Sr2Te | 10.1039/c5dt02026c | 20 | Co O Sr Te | 16 | 0 | 15 | -121.788887 | -6.089444 | 0 | 2 | 2.707 | 0.03488 | none | 0.44324151 0.00000000 0.89640223 |
MAGNDATA_0_307 | ScCrO3 | CrO3Sc | 10.1103/PhysRevB.95.054432 | 20 | Cr O Sc | 9 | 0 | 8 | -169.678066 | -8.483903 | 0 | 4 | 2.892 | 0.038959 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_308 | InCrO3 | CrInO3 | 10.1103/PhysRevB.95.054432 | 20 | Cr In O | 3 | 0 | 2 | -135.36345 | -6.768172 | 0 | 4 | 2.929 | 0.041141 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_309 | TlCrO3 | CrO3Tl | 10.1103/PhysRevB.95.054432 | 20 | Cr O Tl | 10 | 0 | 9 | -125.136813 | -6.256841 | 0 | 4 | 2.924 | 0.036315 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_360 | Mn2ScSbO6 | Mn2O6SbSc | 10.1039/c5dt03445k | 20 | Mn O Sb Sc | 12 | 0 | 11 | -151.767943 | -7.588397 | 0 | 4 | 4.629 | 0.044328 | max_occupancy_site | 0.34774441 0.00000000 0.93758937 |
MAGNDATA_0_364 | SrCr2As2 | As2Cr2Sr | 10.1103/PhysRevB.96.014411 | 10 | As Cr Sr | 3 | 0 | 2 | -65.675891 | -6.567589 | 0 | 4 | 2.563 | 0.009513 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_365 | BaCr2As2 | As2BaCr2 | 10.1103/PhysRevB.95.184414 | 10 | As Ba Cr | 8 | 0 | 7 | -66.204113 | -6.620411 | 0 | 4 | 2.605 | 0.041206 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_366 | BaCrFeAs2 | As2BaCr2 | 10.1103/PhysRevB.95.184414 | 10 | As Ba Cr | 9 | 0 | 8 | -66.203163 | -6.620316 | 0 | 4 | 2.633 | 0.037497 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_374 | YNi4Si | Ni4SiY | 10.1016/j.jmmm.2014.04.057 | 12 | Ni Si Y | 4 | 0 | 3 | -77.279507 | -6.439959 | 0 | 0 | 0 | 0.031928 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_395 | MnPtGa | GaMnPt | 10.1103/PhysRevMaterials.4.044405 | 12 | Ga Mn Pt | 4 | 0 | 3 | -78.54573 | -6.545478 | 0 | 4 | 3.573 | 0.018768 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_399 | FeOOH | FeHO2 | 10.1107/S1600576714022651 | 16 | Fe H O | 25 | 0 | 24 | -97.296806 | -6.08105 | 0 | 4 | 4.311 | 0.042986 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_414 | AlFe2B2 | AlB2Fe2 | 10.1016/j.jallcom.2015.12.111 | 10 | Al B Fe | 4 | 0 | 3 | -72.108573 | -7.210857 | 0 | 4 | 1.385 | 0.026435 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_432 | KMnF3 | F3KMn | 10.1016/j.jallcom.2020.155935 | 20 | F K Mn | 2 | 0 | 1 | -112.317188 | -5.615859 | 0 | 4 | 4.67 | 0.044751 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_433 | KMnF3 | F3KMn | 10.1016/j.jallcom.2020.155935 | 20 | F K Mn | 2 | 0 | 1 | -112.274132 | -5.613707 | 0 | 4 | 4.668 | 0.025214 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_434 | K2ReI6 | I6K2Re | 10.1021/acs.jpcc.8b1137 | 18 | I K Re | 9 | 0 | 8 | -59.222924 | -3.290162 | 0 | 2 | 2.197 | 0.0402 | none | 0.99998134 0.00000000 -0.00610861 |
MAGNDATA_0_445 | MnCoGe | CoGeMn | 10.1103/PhysRevMaterials.4.104407 | 12 | Co Ge Mn | 12 | 0 | 11 | -85.572862 | -7.131072 | 0 | 8 | 3.175 | 0.046212 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_464 | BaMn2P2 | BaMn2P2 | 10.1006/jssc.1994.1375 | 10 | Ba Mn P | 6 | 0 | 5 | -69.927569 | -6.992757 | 0 | 4 | 3.048 | 0.005851 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_470 | BaMn2Sb2 | BaMn2Sb2 | 10.1103/PhysRevB.99.184416 | 10 | Ba Mn Sb | 6 | 0 | 5 | -61.143 | -6.1143 | 0 | 4 | 3.668 | 0.012033 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_471 | Ba2Mn3Sb2O2 | Ba2Mn3O2Sb2 | 10.1103/PhysRevB.99.184416 | 18 | Ba Mn O Sb | 7 | 0 | 6 | -101.434093 | -5.635227 | 0 | 4 | 4.405 | 0.028607 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_482 | SrMn2As2 | As2Mn2Sr | 10.1088/0953-8984/29/3/035802 | 5 | As Mn Sr | 8 | 0 | 7 | -32.245678 | -6.449136 | 0 | 2 | 3.665 | 0.044212 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_501 | LiFe2F6 | F6Fe2Li | 10.1103/PhysRevB.6.1968 | 18 | F Fe Li | 6 | 0 | 5 | -95.006643 | -5.278147 | 0 | 4 | 4.179 | 0.02834 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_512 | Mn3As2 | As2Mn3 | 10.1016/j.jssc.2020.121901 | 20 | As Mn | 12 | 0 | 11 | -151.077257 | -7.553863 | 0 | 12 | 3.375 | 0.032051 | none | 0.00000000 -1.00000000 0.00000000 |
MAGNDATA_0_513 | YRuO3 | O3RuY | 10.1103/PhysRevMaterials.4.091402 | 20 | O Ru Y | 10 | 0 | 9 | -165.038804 | -8.25194 | 0 | 0 | 0.004 | 0.043339 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_523 | CaMn2Sb2 | CaMn2Sb2 | 10.1016/j.jmmm.2009.07.015 | 5 | Ca Mn Sb | 17 | 0 | 16 | -30.091194 | -6.018239 | 0 | 2 | 3.801 | 0.030048 | none | -0.90595610 0.00000000 0.42337164 |
MAGNDATA_0_528 | CrSb | CrSb | 10.1039/d0dt03277h | 4 | Cr Sb | 5 | 0 | 4 | -27.403854 | -6.850963 | 0 | 2 | 2.78 | 0 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_541 | Mn2FeReO6 | FeMn2O6Re | 10.1002/anie.201506540 | 20 | Fe Mn O Re | 21 | 0 | 20 | -145.762652 | -7.288133 | 0 | 8 | 4.196 | 0.035547 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_542 | Mn2FeReO6 | FeMn2O6Re | 10.1002/anie.201506540 | 20 | Fe Mn O Re | 14 | 0 | 13 | -155.99871 | -7.799935 | 0 | 8 | 4.621 | 0.034258 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_543 | Mn2FeReO6 | FeMn2O6Re | 10.1002/anie.201506540 | 20 | Fe Mn O Re | 15 | 0 | 14 | -155.998177 | -7.799909 | 0 | 8 | 4.621 | 0.034942 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_546 | Mn2FeReO6 | FeMn2O6Re | 10.1002/anie.201506456 | 20 | Fe Mn O Re | 74 | 3 | 76 | -146.3434 | -7.31717 | 0 | 8 | 3.725 | 0.044478 | max_occupancy_site | 0.70710678 0.00000000 0.70710678 |
MAGNDATA_0_547 | Mn2FeReO6 | FeMn2O6Re | 10.1002/anie.201506456 | 20 | Fe Mn O Re | 25 | 0 | 24 | -145.770263 | -7.288513 | 0 | 8 | 4.191 | 0.03686 | max_occupancy_site | 0.70710678 0.00000000 0.70710678 |
MAGNDATA_0_553 | K2ReI6 | I6K2Re | 10.1021/acs.jpcc.8b11371 | 18 | I K Re | 9 | 0 | 8 | -59.222927 | -3.290163 | 0 | 2 | 2.197 | 0.04016 | none | 0.99998134 0.00000000 -0.00610861 |
MAGNDATA_0_554 | Co2MnSi | Co2MnSi | 10.1016/j.jallcom.2018.12.018 | 16 | Co Mn Si | 3 | 0 | 2 | -122.445399 | -7.652837 | 0 | 12 | 2.962 | 0 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_586 | YCrO3 | CrO3Y | 10.1063/1.1708325 | 20 | Cr O Y | 8 | 0 | 7 | -171.58647 | -8.579324 | 0 | 4 | 2.895 | 0.040033 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_598 | AlCr2 | AlCr2 | 10.1063/1.1696459 | 6 | Al Cr | 4 | 0 | 3 | -46.947437 | -7.824573 | 0 | 4 | 1.269 | 0.006959 | none | 0.00000000 -0.90506568 -0.42527182 |
MAGNDATA_0_599 | CaMnSi | CaMnSi | 10.1016/0038-1098(95)00693-1 | 6 | Ca Mn Si | 10 | 0 | 9 | -35.492881 | -5.91548 | 0 | 2 | 3.05 | 0.036819 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_600 | CaMnSi | CaMnSi | 10.1016/0038-1098(95)00693-1 | 6 | Ca Mn Si | 10 | 0 | 9 | -35.496676 | -5.916113 | 0 | 2 | 3.009 | 0.02725 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_601 | CaMnGe | CaGeMn | 10.1016/0038-1098(95)00693-1 | 6 | Ca Ge Mn | 11 | 0 | 10 | -33.926404 | -5.654401 | 0 | 2 | 3.375 | 0.043895 | none | -0.55952424 0.00000000 0.82881399 |
MAGNDATA_0_602 | CaMnGe | CaGeMn | 10.1016/0038-1098(95)00693-1 | 6 | Ca Ge Mn | 14 | 0 | 13 | -33.926062 | -5.654344 | 0 | 2 | 3.384 | 0.013065 | none | -0.44061286 0.00000000 0.89769723 |
MAGNDATA_0_603 | CaMn2Ge2 | CaGe2Mn2 | 10.1016/0925-8388(94)90140-6 | 10 | Ca Ge Mn | 3 | 0 | 2 | -62.259764 | -6.225976 | 0 | 4 | 3.047 | 0.041917 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_604 | CaMn2Ge2 | CaGe2Mn2 | 10.1016/0925-8388(94)90140-6 | 10 | Ca Ge Mn | 2 | 0 | 1 | -62.262016 | -6.226202 | 0 | 4 | 3.034 | 0.036542 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_605 | BaMn2Ge2 | BaGe2Mn2 | 10.1016/0925-8388(94)90140-6 | 10 | Ba Ge Mn | 12 | 0 | 11 | -61.36496 | -6.136496 | 0 | 4 | 3.268 | 0.018567 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_606 | BaMn2Ge2 | BaGe2Mn2 | 10.1016/0925-8388(94)90140-6 | 10 | Ba Ge Mn | 11 | 0 | 10 | -61.368335 | -6.136834 | 0 | 4 | 3.24 | 0.010924 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_607 | RuO2 | O2Ru | 10.1103/PhysRevLett.118.077201 | 6 | O Ru | 9 | 0 | 8 | -44.327862 | -7.387977 | 0 | 0 | 0 | 0.020074 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_611 | BaMnSb2 | BaMnSb2 | 10.1038/srep30525 | 16 | Ba Mn Sb | 6 | 0 | 5 | -85.853081 | -5.365818 | 0 | 4 | 3.759 | 0.043166 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_617 | KMnSb | KMnSb | 10.1002/(SICI)1521-3749(199901)625:1<31::AID-ZAAC31>3.0.CO;2-S | 6 | K Mn Sb | 5 | 0 | 4 | -30.329593 | -5.054932 | 0 | 2 | 3.855 | 0.013702 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_618 | KMnBi | BiKMn | 10.1002/(SICI)1521-3749(199901)625:1<31::AID-ZAAC31>3.0.CO;2-S | 6 | Bi K Mn | 4 | 0 | 3 | -28.904367 | -4.817394 | 0 | 2 | 3.957 | 0.045481 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_626 | NaMnP | MnNaP | 10.1002/zaac.19865390816 | 6 | Mn Na P | 7 | 0 | 6 | -34.718541 | -5.786424 | 0 | 2 | 3.217 | 0.036599 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_627 | NaMnP | MnNaP | 10.1002/zaac.19865390816 | 6 | Mn Na P | 11 | 0 | 10 | -34.71843 | -5.786405 | 0 | 2 | 3.22 | 0.039358 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_628 | NaMnP | MnNaP | 10.1002/zaac.19865390816 | 6 | Mn Na P | 14 | 0 | 13 | -34.718718 | -5.786453 | 0 | 2 | 3.216 | 0.035753 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_629 | NaMnAs | AsMnNa | 10.1002/zaac.19865390816 | 6 | As Mn Na | 10 | 0 | 9 | -32.819755 | -5.469959 | 0 | 2 | 3.518 | 0.010804 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_630 | NaMnAs | AsMnNa | 10.1002/zaac.19865390816 | 6 | As Mn Na | 7 | 0 | 6 | -32.816635 | -5.469439 | 0 | 2 | 3.529 | 0.047889 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_631 | NaMnSb | MnNaSb | 10.1002/zaac.19865390816 | 6 | Mn Na Sb | 2 | 0 | 1 | -30.688306 | -5.114718 | 0 | 2 | 3.702 | 0.045217 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_632 | NaMnSb | MnNaSb | 10.1002/zaac.19865390816 | 6 | Mn Na Sb | 4 | 0 | 3 | -30.687959 | -5.11466 | 0 | 2 | 3.694 | 0.047756 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_633 | KFeS2 | FeKS2 | 10.1016/0022-4596(87)90065-X | 16 | Fe K S | 9 | 0 | 8 | -84.887241 | -5.305453 | 0 | 4 | 2.772 | 0.04619 | none | 0.39674590 0.00000000 -0.91792848 |
MAGNDATA_0_634 | NaMnBi | BiMnNa | 10.1002/zaac.19865390816 | 6 | Bi Mn Na | 11 | 0 | 10 | -29.195421 | -4.865903 | 0 | 2 | 3.819 | 0.035665 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_635 | NaMnBi | BiMnNa | 10.1002/zaac.19865390816 | 6 | Bi Mn Na | 9 | 0 | 8 | -29.195496 | -4.865916 | 0 | 2 | 3.821 | 0.024881 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_636 | RbFeS2 | FeRbS2 | 10.1016/0022-4596(87)90065-X | 16 | Fe Rb S | 10 | 0 | 9 | -84.518558 | -5.28241 | 0 | 4 | 2.796 | 0.047832 | none | 0.32317631 0.00000000 -0.94633877 |
MAGNDATA_0_638 | RbFeSe2 | FeRbSe2 | 10.1016/0022-4596(87)90065-X | 16 | Fe Rb Se | 9 | 0 | 8 | -77.772795 | -4.8608 | 0 | 4 | 2.96 | 0.02254 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_639 | Mn2Au | AuMn2 | 10.1038/ncomms3892 | 6 | Au Mn | 8 | 0 | 7 | -43.643542 | -7.273924 | 0 | 4 | 3.516 | 0.02145 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_640 | Mn2Au | AuMn2 | 10.1038/ncomms3892 | 6 | Au Mn | 7 | 0 | 6 | -43.643332 | -7.273889 | 0 | 4 | 3.527 | 0.008704 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_662 | Mn3Sn2 | Mn3Sn2 | 10.1103/PhysRevB.81.174427 | 20 | Mn Sn | 18 | 0 | 17 | -138.072865 | -6.903643 | 0 | 4 | 2.57 | 0.040001 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_673 | MnFe4Si3 | Fe5Si3 | 10.1016/j.jssc.2014.05.001 | 16 | Fe Si | 6 | 0 | 5 | -123.038687 | -7.689918 | 0 | 10 | 1.882 | 0.034331 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_674 | MnFe4Si3 | Fe5Si3 | 10.1016/j.jssc.2014.05.001 | 16 | Fe Si | 5 | 0 | 4 | -123.367915 | -7.710495 | 0 | 10 | 1.822 | 0.043058 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_675 | MnFe4Si3 | Fe5Si3 | 10.1002/pssa.2210190145 | 16 | Fe Si | 11 | 0 | 10 | -123.36825 | -7.710516 | 0 | 10 | 1.823 | 0.028853 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_682 | Ca2FeOsO6 | Ca2FeO6Os | 10.1021/ic5006715 | 20 | Ca Fe O Os | 11 | 0 | 10 | -141.237338 | -7.061867 | 0 | 4 | 4.243 | 0.037522 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_683 | SrCaFeOsO6 | Ca2FeO6Os | 10.1021/ic5006715 | 20 | Ca Fe O Os | 14 | 0 | 13 | -141.250376 | -7.062519 | 0 | 4 | 4.243 | 0.048836 | max_occupancy_site | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_699 | LiMn6Sn6 | LiMn6Sn6 | 10.1140/epjb/e2006-00207-9 | 13 | Li Mn Sn | 7 | 0 | 6 | -81.529404 | -6.271493 | 0 | 6 | 2.451 | 0.040779 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_712 | VNb3S6 | Nb3S6V | 10.1103/PhysRevMaterials.4.054416 | 20 | Nb S V | 8 | 0 | 7 | -151.61432 | -7.580716 | 0 | 2 | 1.802 | 0.027242 | none | 1.00000000 0.00000000 0.00000000 |
MAGNDATA_0_732 | SrRuO3 | O3RuSr | 10.1016/j.jmmm.2006.02.089 | 20 | O Ru Sr | 15 | 0 | 14 | -138.817663 | -6.940883 | 0 | 4 | 1.391 | 0.04438 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_739 | YBaMn2O5 | BaMn2O5Y | 10.1016/S0025-5408(98)00214-1 | 18 | Ba Mn O Y | 11 | 0 | 10 | -139.474693 | -7.748594 | 0 | 4 | 4.499 | 0.023665 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_767 | SrMnSb2 | MnSb2Sr | 10.1038/NMAT4953 | 16 | Mn Sb Sr | 15 | 0 | 14 | -80.679632 | -5.042477 | 0 | 0 | 0.022 | 0.034648 | none | 0.00000000 1.00000000 0.00000000 |
MAGNDATA_0_787 | YVO3 | O3VY | 10.1103/PhysRevB.73.094440 | 20 | O V Y | 8 | 0 | 7 | -172.000776 | -8.600039 | 0 | 4 | 1.823 | 0.036148 | none | 0.00000000 0.00000000 1.00000000 |
MAGNDATA_0_795 | Sr2YRuO6 | O6RuSr2Y | 10.1016/j.jssc.2017.03.001 | 20 | O Ru Sr Y | 16 | 0 | 15 | -146.410186 | -7.320509 | 0 | 2 | 1.903 | 0.044555 | none | 0.98237956 0.00000000 -0.18689678 |
MAGNDATA_0_796 | Ca2NiOsO6 | Ca2NiO6Os | 10.1021/acs.chemmater.6b00254 | 20 | Ca Ni O Os | 10 | 0 | 9 | -133.2193 | -6.660965 | 0 | 4 | 1.747 | 0.039801 | none | 0.99998719 0.00000000 -0.00506143 |
MAG188
MAG188 is a DFT benchmark of 188 experimentally characterized collinear magnetic materials from the MAGNDATA database. All structures were recomputed with spin-polarized DFT and relaxed. MAG188 contains two benchmarks:
- MAG188-EXP: the relaxed experimentally reported magnetic state of each material (188 endpoints). It measures accuracy on experimentally established magnetic states.
- MAG188-SAMPLE: 1,195 relaxed endpoints that cover several self-consistent collinear spin configurations of each material: the 188 experimental states plus 1,007 relaxations from other spin sign patterns. It measures how well a model resolves competing magnetic states of the same material. For a spin-agnostic model, these states differ only through small changes in geometry.
Both benchmarks come with their full relaxation trajectories. Every frame has an energy, forces, stress and site-resolved DFT spins. MAG188 is the magnetic benchmark of the Prophet technical report (Section 8).
| MAG188-EXP | MAG188-SAMPLE | |
|---|---|---|
| Materials (MAGNDATA entries) | 188 | 188 |
| Relaxed endpoints (benchmark) | 188 | 1,195 (188 exp + 1,007 sampled) |
| Relaxation frames (all ionic steps) | 1,887 | 14,642 |
| Configurations per material | 1 | 1–10 (178 materials with ≥ 2) |
Both benchmarks cover 140 distinct reduced compositions, 50 elements and 4–20 atoms per cell. 177 materials have at least one magnetic site (|m| > 0.5 μB); there are 721 such sites in the experimental states.
In MAG188-SAMPLE:
- 163 materials have ≥ 2 distinct energy levels, where levels count as distinct when they are ≥ 1 meV/atom apart.
- The spread between the highest and lowest endpoint of a material has a median of 32.6 meV/atom and a maximum of 518.6 meV/atom.
- The experimental state is the lowest DFT endpoint for 145 of the 188 materials, and within 1 meV/atom of the lowest for 164.
Files
| File | Contents |
|---|---|
MAG188-EXP/mag188_exp.extxyz |
188 relaxed endpoints, one per material (MAG188-EXP benchmark set) |
MAG188-EXP/mag188_exp_trajectories.extxyz |
all 1,887 ionic steps of the 188 relaxations |
MAG188-EXP/mag188_exp_index.csv |
one row per material (composition, endpoint energy, spins, endpoint max force, …) |
MAG188-SAMPLE/mag188_sample.extxyz |
1,195 relaxed endpoints (MAG188-SAMPLE benchmark set) |
MAG188-SAMPLE/mag188_sample_trajectories.extxyz |
all 14,642 ionic steps of the 1,195 relaxations |
MAG188-SAMPLE/mag188_sample_index.csv |
one row per relaxation, including the energy above the material's lowest endpoint (e_rel_meV_per_atom) |
SHA256SUMS |
checksums of all data files |
In the trajectory files, the final frame of each relaxation has is_endpoint=T. The exp endpoints and
trajectories of MAG188-SAMPLE are identical to MAG188-EXP, so the two sets overlap by design.
Construction
- Structures. Commensurate, collinear magnetic structures from MAGNDATA with at most 20 atoms per cell
and no f-block elements. For the 15 entries with partially occupied sites, the species with the highest
occupancy was kept (
occupancy_policy=max_occupancy_site). - DFT. VASP with PAW potentials and the PBE functional (PBE+U where the Materials Project applies it).
Inputs follow pymatgen
MPRelaxSet, which is the ELEMENTA protocol. All calculations are spin-polarized and collinear, and both atomic positions and the cell are relaxed. - Energies. Energies are raw VASP total energies, with no Materials Project (MP2020) compatibility corrections.
- Experimental states (
exp). Each relaxation starts from the experimentally reported spin ordering. - Sampled states (
sampled, MAG188-SAMPLE only). For each material, seed spins on the magnetic sites were given different collinear sign patterns, and each pattern was relaxed self-consistently.mag_sample_maskidentifies the sign pattern (0= all seed spins parallel), andconfig_idismag<mask>. Symmetry-equivalent patterns can converge to the same state. When ranking the states of a material, treat endpoints within 1 meV/atom of each other as one level. - Held out. No reduced formula in MAG188 appears in the training data of Prophet-Spin.
Data fields
The files are standard extended XYZ, and both benchmarks share one schema.
Per atom (the Properties columns):
| Field | Unit | Description |
|---|---|---|
species, pos |
Å | element and Cartesian position |
forces |
eV/Å | DFT forces |
magmoms |
μB | DFT site spins: VASP's collinear site-projected magnetization, with sign |
Per frame (comment line):
| Field | Unit | Description |
|---|---|---|
energy |
eV | DFT total energy of the cell |
stress |
eV/ų | full 3×3 stress in the ASE sign convention (negative = compressive) |
magmom |
μB | total cell magnetization (not exactly equal to the sum of the site magmoms) |
material_id |
– | MAGNDATA_<i>_<j> = MAGNDATA entry <i>.<j> (e.g. MAGNDATA_0_1150 → entry 0.1150) |
formula, doi |
– | cell formula and literature reference of the MAGNDATA entry |
config_id |
– | exp, or mag<mask> for sampled configurations; (material_id, config_id) is unique |
config_type |
– | exp or sampled |
mag_sample_mask |
– | seed sign-pattern id (-1 for exp) |
ionic_step |
– | original VASP ionic-step index |
is_endpoint |
– | T for the final frame of each relaxation (trajectory files only) |
n_scf_steps |
– | electronic (SCF) iterations of this ionic step |
collinear_axis |
– | experimental spin direction from MAGNDATA (exp frames only). The DFT is collinear, so only each spin's sign is used |
occupancy_policy |
– | none, or max_occupancy_site for the 15 disordered entries |
Usage
The files load with ASE (tested with ASE 3.29). Energy, forces, stress, site spins and total magnetization all load as calculator results:
from collections import defaultdict
from ase.io import read
exp = read("MAG188-EXP/mag188_exp.extxyz", index=":") # 188 endpoints
sample = read("MAG188-SAMPLE/mag188_sample.extxyz", index=":") # 1,195 endpoints
a = exp[0]
a.info["material_id"], a.info["config_id"]
a.get_potential_energy() # eV
a.get_forces() # eV/Å
a.get_stress(voigt=False) # eV/ų, ASE convention
a.get_magnetic_moments() # per-site DFT spins, μB
a.get_magnetic_moment() # total cell magnetization, μB
states = defaultdict(list) # competing magnetic states of each material
for s in sample:
states[s.info["material_id"]].append(s)
Benchmark protocols
Energy and force accuracy. Evaluate on the endpoint files: 188 frames for MAG188-EXP and 1,195 for MAG188-SAMPLE.
- Energy MAE: mean over endpoints of |E_pred − E_DFT| / N_atoms, reported in meV/atom on raw total energies.
- Force MAE: mean absolute error pooled over all Cartesian force components of all atoms, in meV/Å.
Magnetic-state ranking (MAG188-SAMPLE). For each material with ≥ 2 configurations, compare the model's energy ordering of its endpoints with the DFT ordering. Report, for example, whether the lowest DFT state is identified, and the Spearman correlation. Merge endpoints within 1 meV/atom first.
Spin input. A spin-conditioned model can be run in two ways, and results should say which was used:
- DFT-converged: the model receives the DFT site spins (
magmoms) as input. - Predicted: the model receives only the structure and initial spin guesses.
Spin-agnostic models are evaluated on the structure alone.
- DFT-converged: the model receives the DFT site spins (
Reference results
These are the energy and force MAEs on the benchmark endpoints from the Prophet technical report. Energies are raw. Prophet models share the ELEMENTA reference; the public models (*) use their own isolated-atom references.
| Model | Spin source | EXP E (meV/atom) | EXP F (meV/Å) | SAMPLE E (meV/atom) | SAMPLE F (meV/Å) |
|---|---|---|---|---|---|
| Prophet-OAME-MBD | – | 62.84 | 33.4 | 35.63 | 31.0 |
| MACE-MP-0 | – | 71.97* | 40.1 | 45.69* | 38.3 |
| MACE-MPA-0 | – | 65.08* | 37.5 | 39.94* | 34.0 |
| MatterSim v1 | – | 66.03* | 45.3 | 36.90* | 43.6 |
| EquiformerV3 | – | 64.95* | 40.1 | 37.72* | 37.0 |
| ORB v3 | – | 66.51* | 42.8 | 40.96* | 38.1 |
| Nequix-MP-1 | – | 65.48* | 37.3 | 38.91* | 34.0 |
| Nequix-OAM-1 | – | 65.70* | 36.1 | 40.83* | 32.5 |
| Prophet-Spin | DFT-converged | 19.23 | 18.3 | 16.34 | 20.1 |
| Prophet-Spin | spin-denoised (predicted) | 30.73 | 26.8 | 20.75 | 30.9 |
Notes
ionic_stepkeeps VASP's original numbering. Frames were removed upstream from some trajectories, which either start after step 0 or have gaps: 4 in MAG188-EXP and 71 in MAG188-SAMPLE. Useis_endpointto find the final frames.- All endpoints except two have a maximum atomic force below 0.05 eV/Å. The exceptions are
MAGNDATA_1_461exp(0.092 eV/Å) andMAGNDATA_1_556mag2(0.074 eV/Å). - MAG188 is a held-out test set. Please do not train on it if you report results on it.
Citation and License
If you use MAG188, please cite the Prophet technical report and the MAGNDATA database:
Prophet: Scaling Atomistic Foundation Models Across Composition, Configuration, and Spin, Kairos Materials (2026).
@article{gallego2016magndata,
title = {{MAGNDATA}: Towards a Database of Magnetic Structures. {I}. The Commensurate Case},
author = {Gallego, Samuel V. and Perez-Mato, J. Manuel and Elcoro, Luis and Tasci, Emre S. and
Hanson, Robert M. and Momma, Koichi and Aroyo, Mois I. and Madariaga, Gotzon},
journal = {Journal of Applied Crystallography},
volume = {49}, number = {5}, pages = {1750--1776}, year = {2016},
doi = {10.1107/S1600576716012863}
}
Released under CC-BY-NC-4.0. The starting structures come from MAGNDATA (Bilbao Crystallographic
Server). The literature source of each entry is given in its doi field.
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