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material_id
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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
End of preview. Expand in Data Studio

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_mask identifies the sign pattern (0 = all seed spins parallel), and config_id is mag<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.

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_step keeps 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. Use is_endpoint to find the final frames.
  • All endpoints except two have a maximum atomic force below 0.05 eV/Å. The exceptions are MAGNDATA_1_461 exp (0.092 eV/Å) and MAGNDATA_1_556 mag2 (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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