shreyaspullehf/supervision-alignn-tc-prediction
Updated
•
5
formula_sc
string | formula_similarity
int64 | totreldiff
float64 | formula_frac
float64 | correct_formula_frac
bool | formula_2
string | orig_formula_cif
string | tc
float64 | sc_class
string | sc_class_unique_sc
bool | norm_formula_sc
string | chemical_composition_sc
string | num_elements_sc
int64 | origin_sc
string | old_formula_sc
string | database_id_2
string | original_formula_2
string | chemical_composition_2
string | norm_formula_2
string | spacegroup_2
string | crystal_system_2
string | lata_2
float64 | latb_2
float64 | latc_2
float64 | cif
string | original_cif_2
string | material_id_2
string | band_gap_2
float64 | band_structure_2
string | created_at_2
string | density_2
float64 | doi_2
string | doi_bibtex_2
string | dos_2
string | e_above_hull_2
float64 | efermi_2
float64 | encut_2
float64 | energy_2
float64 | energy_per_atom_2
float64 | exp_2
string | final_energy_2
float64 | final_energy_per_atom_2
float64 | formation_energy_per_atom_2
float64 | has_2
string | has_bandstructure_2
bool | icsd_ids_2
string | is_ordered_2
bool | last_updated_2
string | magnetic_type_2
string | nsites_2
int64 | ntask_ids_2
int64 | original_task_id_2
string | oxide_type_2
string | pretty_formula_2
string | pseudo_potential_2
string | reduced_cell_formula_2
string | run_type_2
string | task_id_2
string | task_ids_2
string | total_magnetization_2
float64 | unit_cell_formula_2
string | cell_volume_2
float64 | warnings_2
string | ordering_2
string | is_magnetic_2
bool | exchange_symmetry_2
int64 | num_unique_magnetic_sites_2
int64 | magmoms_2
string | total_magnetization_normalized_vol_2
float64 | total_magnetization_normalized_formula_units_2
float64 | num_magnetic_sites_2
int64 | true_total_magnetization_2
float64 | origin_2
string | cif_before_synthetic_doping
string | synth_doped
bool | Reason for exclusion
float64 | graph
string | crystal_temp_2
int64 | no_crystal_temp_given_2
bool | point_group_2
string | cubic
int64 | hexagonal
int64 | monoclinic
int64 | orthorhombic
int64 | tetragonal
int64 | triclinic
int64 | trigonal
int64 | primitive
int64 | base-centered
int64 | body-centered
int64 | face-centered
int64 | weight
float64 | cif_exists
bool |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
As2Eu1Fe1.8P0.2
| 3
| 0.08
| 1
| true
|
As2Eu1Fe1.8P0.2
|
As2Eu1Fe2
| 0
|
Ferrite
| true
|
As40Eu20Fe36P4
|
As-Eu-Fe-P
| 4
|
Supercon
|
Eu1Fe1.8As2P0.2
|
MP-mp-20890
|
Eu1Fe2As2
|
As-Eu-Fe
|
As40Eu20Fe40
|
I 4/m m m
|
tetragonal
| 3.973668
| 3.973668
| 6.071206
|
data/final/MP/cifs/As2Eu1Fe1.8P0.2-MP-mp-20890-synth_doped.cif
|
data/source/MP/raw/cifs/mp-20890.cif
|
mp-20890
| 0
| null |
2014-02-21 09:03:25
| 8.079887
|
10.17188/1196086
|
@misc{osti_1196086,
author = "Persson, Kristin",
title = "Materials Data on Eu(FeAs)2 (SG:139) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1196086",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1687595'}}
| 0
| 5.690453
| 520
| -39.431805
| -7.886361
|
{'tags': ['High pressure experimental phase', 'Europium diiron diarsenide - HP', 'Europium diiron diarsenide', 'Europium iron arsenide (1/2/2)']}
| -39.431805
| -7.886361
| -0.576302
|
['xas', 'bandstructure']
| true
|
[169689, 169687, 185355, 169691, 163211, 185356, 610431, 169690, 169688, 163210]
| true
|
2021-05-12 10:56:57.051000
|
FM
| 5
| 16
|
mp-20890
| null |
Eu(FeAs)2
|
{'functional': 'PBE', 'labels': ['Eu', 'Fe_pv', 'As'], 'pot_type': 'paw'}
|
{'Eu': 1.0, 'Fe': 2.0, 'As': 2.0}
|
GGA
|
mp-20890
|
['mp-991161', 'mp-993140', 'mp-20890', 'mp-1069324', 'mp-1069480', 'mp-1069596', 'mp-1069907', 'mp-1070115', 'mp-1069978', 'mp-1442076', 'mp-1687595', 'mp-1782260', 'mp-994461', 'mp-1594012', 'mp-1069557', 'mp-1070074']
| 6.957965
|
{'Eu': 1.0, 'Fe': 2.0, 'As': 2.0}
| 84.979928
|
[]
|
FM
| true
| 139
| 1
|
[6.7, -0.0, -0.0, 0.0, 0.0]
| 0.081878
| 6.957965
| 1
| 6.957965
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-20890.cif
| true
| null |
data/final/MP/graphs/As2Eu1Fe1.8P0.2-MP-mp-20890-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Ba2Cu3Dy0.1Pr0.9O7
| 2
| 0.015385
| 1
| true
|
Ba2Cu3Dy0.1Pr0.9O7
|
Ba2Cu3Pr1O7
| 0
|
Cuprate
| true
|
Ba15.385Cu23.077Dy0.769Pr6.923O53.84615384615385
|
Ba-Cu-Dy-Pr-O
| 5
|
Supercon
|
Dy0.1Pr0.9Ba2Cu3O7
|
MP-mp-20936
|
Ba2Pr1Cu3O7
|
Ba-Cu-Pr-O
|
Ba15.385Cu23.077Pr7.692O53.84615384615385
|
P m m m
|
orthorhombic
| 3.903923
| 3.95568
| 11.916432
|
data/final/MP/cifs/Ba2Cu3Dy0.1Pr0.9O7-MP-mp-20936-synth_doped.cif
|
data/source/MP/raw/cifs/mp-20936.cif
|
mp-20936
| 0
| null |
2014-02-22 14:41:55
| 6.480718
|
10.17188/1196129
|
@misc{osti_1196129,
author = "Persson, Kristin",
title = "Materials Data on Ba2PrCu3O7 (SG:47) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1196129",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1698257'}}
| 0.0256
| 3.185146
| 520
| -78.628279
| -6.048329
|
{'tags': ['Dibarium praseodymium tricopper heptaoxide', 'Praseodymium dibarium dicopper copper(III) oxide', 'Praseodymium dibarium tricopper heptaoxide', 'Praseodymium dibarium copper(III) dicopper oxide']}
| -78.628279
| -6.048329
| -2.145007
|
['xas', 'bandstructure']
| true
|
[41452, 94377, 81168, 173910, 89221]
| true
|
2021-05-12 10:56:57.051000
|
NM
| 13
| 8
|
mp-20936
|
oxide
|
Ba2PrCu3O7
|
{'functional': 'PBE', 'labels': ['Ba_sv', 'Pr_3', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'Ba': 2.0, 'Pr': 1.0, 'Cu': 3.0, 'O': 7.0}
|
GGA
|
mp-20936
|
['mp-988090', 'mp-987725', 'mp-20936', 'mp-1417367', 'mp-1698257', 'mp-1833655', 'mp-988324', 'mp-1602318']
| 0.000723
|
{'Ba': 2.0, 'Pr': 1.0, 'Cu': 3.0, 'O': 7.0}
| 184.021529
|
[]
|
NM
| false
| 47
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000004
| 0.000723
| 0
| 0.000723
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-20936.cif
| true
| null |
data/final/MP/graphs/Ba2Cu3Dy0.1Pr0.9O7-MP-mp-20936-synth_doped.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
In1Pd1
| 1
| 0
| 1
| true
|
In1Pd1
|
In1Pd1
| 0.7
|
Other
| true
|
In50Pd50
|
In-Pd
| 2
|
Supercon
|
In1Pd1
|
MP-mp-21215
|
In1Pd1
|
In-Pd
|
In50Pd50
|
P m -3 m
|
cubic
| 3.309616
| 3.309616
| 3.309616
|
data/final/MP/cifs/In1Pd1-MP-mp-21215.cif
|
data/source/MP/raw/cifs/mp-21215.cif
|
mp-21215
| 0
| null |
2014-02-21 07:25:50
| 10.133886
|
10.17188/1196490
|
@misc{osti_1196490,
author = "Persson, Kristin",
title = "Materials Data on InPd (SG:221) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1196490",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1668217'}}
| 0
| 8.057802
| 520
| -8.922462
| -4.461231
|
{'tags': ['Indium palladium (1/1)']}
| -8.922462
| -4.461231
| -0.495448
|
['xas', 'elasticity', 'bandstructure']
| true
|
[59474, 59473, 640228]
| true
|
2021-05-12 10:56:16.728000
|
NM
| 2
| 9
|
mp-21215
| null |
InPd
|
{'functional': 'PBE', 'labels': ['In_d', 'Pd'], 'pot_type': 'paw'}
|
{'In': 1.0, 'Pd': 1.0}
|
GGA
|
mp-21215
|
['mp-991670', 'mp-993577', 'mp-21215', 'mp-1140147', 'mp-1440226', 'mp-1668217', 'mp-1791049', 'mp-994872', 'mp-1588915']
| 0.000302
|
{'In': 1.0, 'Pd': 1.0}
| 36.252071
|
[]
|
NM
| false
| 221
| 0
|
[0, 0]
| 0.000008
| 0.000302
| 0
| 0.000302
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-21215.cif
| false
| null |
data/final/MP/graphs/In1Pd1-MP-mp-21215.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Cr2Ti1
| 1
| 0
| 2
| false
|
Cr4Ti2
|
Cr4Ti2
| 0
|
Other
| true
|
Cr66.667Ti33.333
|
Cr-Ti
| 2
|
Supercon
|
Cr2Ti1
|
MP-mp-1425
|
Ti2Cr4
|
Cr-Ti
|
Cr66.667Ti33.333
|
F d -3 m
|
cubic
| 4.853745
| 4.853745
| 4.853745
|
data/final/MP/cifs/Cr2Ti1-MP-mp-1425.cif
|
data/source/MP/raw/cifs/mp-1425.cif
|
mp-1425
| 0
| null |
2011-05-13 13:19:58
| 6.237411
|
10.17188/1190580
|
@misc{osti_1190580,
author = "Persson, Kristin",
title = "Materials Data on TiCr2 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1190580",
place = "United States",
year = "2015",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1674321'}}
| 0
| 6.182499
| 520
| -55.029681
| -9.171614
|
{'tags': ['Chromium titanium (2/1) - LT', 'Chromium titanium hydride (2/1/1)', 'Chromium titanium (2/1)']}
| -55.029681
| -9.171614
| -0.104418
|
['xas', 'elasticity', 'bandstructure']
| true
|
[626917, 102851, 626918, 626910, 626124]
| true
|
2021-05-12 10:56:12.755000
|
NM
| 6
| 9
|
mp-1425
| null |
TiCr2
|
{'functional': 'PBE', 'labels': ['Ti_pv', 'Cr_pv'], 'pot_type': 'paw'}
|
{'Ti': 1.0, 'Cr': 2.0}
|
GGA
|
mp-1425
|
['mp-928359', 'mp-928861', 'mp-912344', 'mp-1425', 'mp-1077747', 'mp-1437894', 'mp-1674321', 'mp-1799932', 'mp-1588451']
| 0.003093
|
{'Ti': 2.0, 'Cr': 4.0}
| 80.856673
|
[]
|
NM
| false
| 227
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000077
| 0.003093
| 0
| 0.006187
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1425.cif
| false
| null |
data/final/MP/graphs/Cr2Ti1-MP-mp-1425.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Rh1Zr3
| 1
| 0
| 4
| false
|
Rh4Zr12
|
Rh4Zr12
| 7.103333
|
Other
| true
|
Rh25Zr75
|
Rh-Zr
| 2
|
Supercon
|
Rh1Zr3
|
MP-mp-1188413
|
Zr12Rh4
|
Rh-Zr
|
Rh25Zr75
|
I -4 2 m
|
tetragonal
| 5.750106
| 8.133163
| 8.133163
|
data/final/MP/cifs/Rh1Zr3-MP-mp-1188413.cif
|
data/source/MP/raw/cifs/mp-1188413.cif
|
mp-1188413
| 0
| null |
2019-01-11 19:25:26.786000
| 7.515208
| null | null |
{'GGA': {'task_id': 'mp-1708881'}}
| 0
| 4.736525
| 520
| -138.700395
| -8.668775
|
{'tags': []}
| -138.700395
| -8.668775
| -0.416922
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:31.620000
|
NM
| 16
| 5
|
mp-1188413
| null |
Zr3Rh
|
{'functional': 'PBE', 'labels': ['Zr_sv', 'Rh_pv'], 'pot_type': 'paw'}
|
{'Zr': 3.0, 'Rh': 1.0}
|
GGA
|
mp-1188413
|
['mp-1188413', 'mp-1426452', 'mp-1708881', 'mp-1811428', 'mp-1604423']
| 0.051845
|
{'Zr': 12.0, 'Rh': 4.0}
| 332.829986
|
[]
|
NM
| false
| 121
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000623
| 0.051845
| 0
| 0.207379
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1188413.cif
| false
| null |
data/final/MP/graphs/Rh1Zr3-MP-mp-1188413.json
| 0
| true
|
-42m
| 0
| 0
| 0
| 0
| 6
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Ge1.9La1Pd2Sn0.1
| 2
| 0.04
| 1
| true
|
Ge1.9La1Pd2Sn0.1
|
Ge2La1Pd2
| 1.25
|
Other
| true
|
Ge38La20Pd40Sn2
|
Ge-La-Pd-Sn
| 4
|
Supercon
|
La1Pd2Ge1.9Sn0.1
|
MP-mp-21033
|
La1Ge2Pd2
|
Ge-La-Pd
|
Ge40La20Pd40
|
I 4/m m m
|
tetragonal
| 4.42129
| 4.42129
| 5.970614
|
data/final/MP/cifs/Ge1.9La1Pd2Sn0.1-MP-mp-21033-synth_doped.cif
|
data/source/MP/raw/cifs/mp-21033.cif
|
mp-21033
| 0
| null |
2014-02-21 11:30:39
| 8.300326
|
10.17188/1196295
|
@misc{osti_1196295,
author = "Persson, Kristin",
title = "Materials Data on La(GePd)2 (SG:139) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1196295",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1701817'}}
| 0
| 6.148903
| 520
| -28.828176
| -5.765635
|
{'tags': ['Lanthanum palladium germanide (1/2/2)']}
| -28.828176
| -5.765635
| -0.85727
|
['xas', 'bandstructure']
| true
|
[81760, 53662]
| true
|
2021-05-12 10:56:57.051000
|
NM
| 5
| 8
|
mp-21033
| null |
La(GePd)2
|
{'functional': 'PBE', 'labels': ['La', 'Ge_d', 'Pd'], 'pot_type': 'paw'}
|
{'La': 1.0, 'Ge': 2.0, 'Pd': 2.0}
|
GGA
|
mp-21033
|
['mp-990571', 'mp-992631', 'mp-21033', 'mp-1438097', 'mp-1701817', 'mp-1796178', 'mp-994077', 'mp-1596763']
| 0.000403
|
{'La': 1.0, 'Ge': 2.0, 'Pd': 2.0}
| 99.433469
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0]
| 0.000004
| 0.000403
| 0
| 0.000403
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-21033.cif
| true
| null |
data/final/MP/graphs/Ge1.9La1Pd2Sn0.1-MP-mp-21033-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
As1Fe1Nd0.95Sr0.05O1
| 2
| 0.025
| 2
| false
|
As2Fe2Nd1.9Sr0.1O2
|
As2Fe2Nd2O2
| 0
|
Ferrite
| true
|
As25Fe25Nd23.75Sr1.25O25
|
As-Fe-Nd-Sr-O
| 5
|
Supercon
|
Nd0.95Sr0.05Fe1As1O1
|
MP-mp-622621
|
Nd2Fe2As2O2
|
As-Fe-Nd-O
|
As25Fe25Nd25O25
|
P 4/n m m
|
tetragonal
| 4.074653
| 4.074653
| 9.170967
|
data/final/MP/cifs/As1Fe1Nd0.95Sr0.05O1-MP-mp-622621-synth_doped.cif
|
data/source/MP/raw/cifs/mp-622621.cif
|
mp-622621
| 0
| null |
2014-02-16 22:28:25
| 6.34728
|
10.17188/1278150
|
@misc{osti_1278150,
author = "Persson, Kristin",
title = "Materials Data on NdFeAsO (SG:129) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1278150",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA+U': {'task_id': 'mp-1677677'}}
| 0.280931
| 3.747776
| 520
| -52.708425
| -6.588553
|
{'tags': ['Neodymium iron arsenic oxide (1/1/1/1)']}
| -52.708425
| -6.588553
| -1.612995
|
['xas', 'bandstructure']
| true
|
[163547, 164679, 422001, 163546, 236651, 236650, 602466, 164680, 164676]
| true
|
2021-05-12 10:57:28.836000
|
FM
| 8
| 8
|
mp-622621
|
oxide
|
NdFeAsO
|
{'functional': 'PBE', 'labels': ['Nd_3', 'Fe_pv', 'As', 'O'], 'pot_type': 'paw'}
|
{'Nd': 1.0, 'Fe': 1.0, 'As': 1.0, 'O': 1.0}
|
GGA+U
|
mp-622621
|
['mp-622621', 'mp-1079381', 'mp-1173401', 'mp-1438697', 'mp-1677677', 'mp-1772072', 'mp-1926310', 'mp-1592869']
| 3.839543
|
{'Nd': 2.0, 'Fe': 2.0, 'As': 2.0, 'O': 2.0}
| 152.263704
|
[]
|
FM
| true
| 129
| 1
|
[0.0, 0.0, 3.6, 3.6, -0.0, -0.0, -0.0, -0.0]
| 0.050433
| 3.839543
| 2
| 7.679085
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-622621.cif
| true
| null |
data/final/MP/graphs/As1Fe1Nd0.95Sr0.05O1-MP-mp-622621-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ge12Nd1Pt4
| 1
| 0
| 1
| true
|
Ge12Nd1Pt4
|
Ge12Nd1Pt4
| 0.7
|
Other
| true
|
Ge70.588Nd5.882Pt23.529
|
Ge-Nd-Pt
| 3
|
Supercon
|
Nd1Pt4Ge12
|
MP-mp-975665
|
Nd1Ge12Pt4
|
Ge-Nd-Pt
|
Ge70.588Nd5.882Pt23.529
|
I m -3
|
cubic
| 7.55665
| 7.55665
| 7.55665
|
data/final/MP/cifs/Ge12Nd1Pt4-MP-mp-975665.cif
|
data/source/MP/raw/cifs/mp-975665.cif
|
mp-975665
| 0
| null |
2015-09-17 09:23:47
| 8.979492
|
10.17188/1314869
|
@misc{osti_1314869,
author = "Persson, Kristin",
title = "Materials Data on Nd(Ge3Pt)4 (SG:204) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1314869",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1707700'}}
| 0.012338
| 4.243693
| 520
| -91.04012
| -5.355301
|
{'tags': ['Neodymium platinum germanide (1/4/12)']}
| -91.04012
| -5.355301
| -0.38306
|
['xas', 'bandstructure']
| true
|
[174555]
| true
|
2021-05-12 10:57:55.580000
|
NM
| 17
| 8
|
mp-975665
| null |
Nd(Ge3Pt)4
|
{'functional': 'PBE', 'labels': ['Nd_3', 'Ge_d', 'Pt'], 'pot_type': 'paw'}
|
{'Nd': 1.0, 'Ge': 12.0, 'Pt': 4.0}
|
GGA
|
mp-975665
|
['mp-975665', 'mp-975820', 'mp-975763', 'mp-1504626', 'mp-1707700', 'mp-1806914', 'mp-975926', 'mp-1608664']
| 0.0024
|
{'Nd': 1.0, 'Ge': 12.0, 'Pt': 4.0}
| 332.174323
|
[]
|
NM
| false
| 204
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000007
| 0.0024
| 0
| 0.0024
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-975665.cif
| false
| null |
data/final/MP/graphs/Ge12Nd1Pt4-MP-mp-975665.json
| 0
| true
|
m-3
| 2
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Co1In5La1
| 1
| 0
| 1
| true
|
Co1In5La1
|
Co1In5La1
| 0
|
Other
| true
|
Co14.286In71.429La14.286
|
Co-In-La
| 3
|
Supercon
|
La1Co1In5
|
MP-mp-21414
|
La1In5Co1
|
Co-In-La
|
Co14.286In71.429La14.286
|
P 4/m m m
|
tetragonal
| 4.667013
| 4.667013
| 7.688877
|
data/final/MP/cifs/Co1In5La1-MP-mp-21414.cif
|
data/source/MP/raw/cifs/mp-21414.cif
|
mp-21414
| 0
| null |
2014-02-21 14:00:54
| 7.653945
|
10.17188/1196860
|
@misc{osti_1196860,
author = "Persson, Kristin",
title = "Materials Data on LaIn5Co (SG:123) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1196860",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1701108'}}
| 0.004845
| 7.974516
| 520
| -27.707856
| -3.958265
|
{'tags': ['Lanthanum cobalt indide (1/1/5)']}
| -27.707856
| -3.958265
| -0.272159
|
['xas', 'bandstructure']
| true
|
[150264, 150261]
| true
|
2021-05-12 10:56:59.077000
|
NM
| 7
| 8
|
mp-21414
| null |
LaIn5Co
|
{'functional': 'PBE', 'labels': ['La', 'In_d', 'Co'], 'pot_type': 'paw'}
|
{'La': 1.0, 'In': 5.0, 'Co': 1.0}
|
GGA
|
mp-21414
|
['mp-991097', 'mp-993086', 'mp-21414', 'mp-1433980', 'mp-1701108', 'mp-1786935', 'mp-994416', 'mp-1591465']
| 0.004488
|
{'La': 1.0, 'In': 5.0, 'Co': 1.0}
| 167.471509
|
[]
|
NM
| false
| 123
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, -0.0]
| 0.000027
| 0.004488
| 0
| 0.004488
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-21414.cif
| false
| null |
data/final/MP/graphs/Co1In5La1-MP-mp-21414.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ir0.2Ru1.8Th1
| 3
| 0.133333
| 2
| false
|
Ir0.4Ru3.6Th2
|
Ru4Th2
| 3.1
|
Other
| true
|
Ir6.667Ru60Th33.333
|
Ir-Ru-Th
| 3
|
Supercon
|
Th1Ir0.2Ru1.8
|
MP-mp-574438
|
Th2Ru4
|
Ru-Th
|
Ru66.667Th33.333
|
F d -3 m
|
cubic
| 5.433971
| 5.433971
| 5.433971
|
data/final/MP/cifs/Ir0.2Ru1.8Th1-MP-mp-574438-synth_doped.cif
|
data/source/MP/raw/cifs/mp-574438.cif
|
mp-574438
| 0
| null |
2014-02-28 05:45:15
| 12.708958
|
10.17188/1276579
|
@misc{osti_1276579,
author = "Persson, Kristin",
title = "Materials Data on ThRu2 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1276579",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-918592'}}
| 0.038487
| 8.285897
| 520
| -53.838971
| -8.973162
|
{'tags': ['Ruthenium thorium (2/1)', 'Thorium ruthenium (1/2)']}
| -53.838971
| -8.973162
| -0.318949
|
['xas', 'elasticity', 'bandstructure']
| true
|
[650730, 150740, 106002, 650723, 650729, 650731, 106003]
| true
|
2021-05-12 10:56:27.046000
|
NM
| 6
| 7
|
mp-574438
| null |
ThRu2
|
{'functional': 'PBE', 'labels': ['Th', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Th': 1.0, 'Ru': 2.0}
|
GGA
|
mp-574438
|
['mp-919588', 'mp-905408', 'mp-918592', 'mp-574438', 'mp-1439663', 'mp-1802924', 'mp-1592175']
| 0.000575
|
{'Th': 2.0, 'Ru': 4.0}
| 113.4585
|
[]
|
NM
| false
| 166
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, -0.0]
| 0.00001
| 0.000575
| 0
| 0.001151
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-574438.cif
| true
| null |
data/final/MP/graphs/Ir0.2Ru1.8Th1-MP-mp-574438-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Co35Zr65
| 2
| 0.033333
| 0.057141
| false
|
Co2Zr3.714
|
Co2Zr4
| 2.48
|
Other
| true
|
Co35Zr65
|
Co-Zr
| 2
|
Supercon
|
Co35Zr65
|
MP-mp-628
|
Zr4Co2
|
Co-Zr
|
Co33.333Zr66.667
|
I 4/m c m
|
tetragonal
| 5.277929
| 5.277929
| 5.277929
|
data/final/MP/cifs/Co35Zr65-MP-mp-628-synth_doped.cif
|
data/source/MP/raw/cifs/mp-628.cif
|
mp-628
| 0
| null |
2011-05-13 12:16:44
| 7.170771
|
10.17188/1278899
|
@misc{osti_1278899,
author = "Persson, Kristin",
title = "Materials Data on Zr2Co (SG:140) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1278899",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1677545'}}
| 0
| 4.51381
| 520
| -49.951208
| -8.325201
|
{'tags': ['Cobalt zirconium (1/2)', 'Zirconium cobalt (2/1)']}
| -49.951208
| -8.325201
| -0.257295
|
['xas', 'elasticity', 'bandstructure']
| true
|
[625671, 191386, 625688, 102740, 625665]
| true
|
2021-05-12 10:56:27.046000
|
NM
| 6
| 20
|
mp-628
| null |
Zr2Co
|
{'functional': 'PBE', 'labels': ['Zr_sv', 'Co'], 'pot_type': 'paw'}
|
{'Zr': 2.0, 'Co': 1.0}
|
GGA
|
mp-628
|
['mp-928347', 'mp-912327', 'mp-928866', 'mp-628', 'mp-1071352', 'mp-1071381', 'mp-1071431', 'mp-1071762', 'mp-1071803', 'mp-1071859', 'mp-1071883', 'mp-1071742', 'mp-1071925', 'mp-1441633', 'mp-1677545', 'mp-1802810', 'mp-1591799', 'mp-1071792', 'mp-1071416', 'mp-1071915']
| 0.000123
|
{'Zr': 4.0, 'Co': 2.0}
| 111.793531
|
[]
|
NM
| false
| 140
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000002
| 0.000123
| 0
| 0.000245
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-628.cif
| true
| null |
data/final/MP/graphs/Co35Zr65-MP-mp-628-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
N4Th3
| 1
| 0
| 1
| true
|
N4Th3
|
N4Th3
| 0
|
Other
| true
|
N57.143Th42.857
|
N-Th
| 2
|
Supercon
|
N4Th3
|
MP-mp-467
|
Th3N4
|
N-Th
|
N57.143Th42.857
|
R -3 m
|
trigonal
| 3.881764
| 3.881764
| 9.430642
|
data/final/MP/cifs/N4Th3-MP-mp-467.cif
|
data/source/MP/raw/cifs/mp-467.cif
|
mp-467
| 1.668
| null |
2011-05-13 07:10:10
| 10.448199
|
10.17188/1208328
|
@misc{osti_1208328,
author = "Persson, Kristin",
title = "Materials Data on Th3N4 (SG:166) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1208328",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1703931'}}
| 0
| 6.40253
| 520
| -66.849601
| -9.549943
|
{'tags': ['Thorium nitride (3/4)', 'Thorium nitride', 'Trithorium tetranitride']}
| -66.849601
| -9.549943
| -1.81515
|
['xas', 'elasticity', 'bandstructure']
| true
|
[644748, 9052, 644750, 14336, 192151]
| true
|
2021-05-12 10:56:20.740000
|
NM
| 7
| 9
|
mp-467
| null |
Th3N4
|
{'functional': 'PBE', 'labels': ['Th', 'N'], 'pot_type': 'paw'}
|
{'Th': 3.0, 'N': 4.0}
|
GGA
|
mp-467
|
['mp-670725', 'mp-661149', 'mp-467', 'mp-1077956', 'mp-1438219', 'mp-1703931', 'mp-1802567', 'mp-1590380', 'mp-687770']
| 0.00006
|
{'Th': 3.0, 'N': 4.0}
| 119.538253
|
[]
|
NM
| false
| 166
| 0
|
[0, 0, 0, 0, 0, 0, 0]
| 0.000001
| 0.00006
| 0
| 0.00006
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-467.cif
| false
| null |
data/final/MP/graphs/N4Th3-MP-mp-467.json
| 0
| true
|
-3m
| 0
| 0
| 0
| 0
| 0
| 0
| 6
| 1
| 0
| 0
| 0
| 1
| false
|
Bi2Cu1Sr2O6
| 1
| 0
| 2
| false
|
Bi4Cu2Sr4O12
|
Bi4Cu2Sr4O12
| 7.38
|
Cuprate
| true
|
Bi18.182Cu9.091Sr18.182O54.54545454545455
|
Bi-Cu-Sr-O
| 4
|
Supercon
|
Bi2Sr2Cu1O6
|
MP-mp-555827
|
Sr4Cu2Bi4O12
|
Bi-Cu-Sr-O
|
Bi18.182Cu9.091Sr18.182O54.54545454545455
|
C c c m
|
orthorhombic
| 5.133052
| 5.525196
| 13.018801
|
data/final/MP/cifs/Bi2Cu1Sr2O6-MP-mp-555827.cif
|
data/source/MP/raw/cifs/mp-555827.cif
|
mp-555827
| 0
| null |
2014-02-22 10:13:35
| 6.928457
|
10.17188/1269010
|
@misc{osti_1269010,
author = "Persson, Kristin",
title = "Materials Data on Sr2Cu(BiO3)2 (SG:66) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1269010",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1707731'}}
| 0.058564
| 4.753631
| 520
| -126.542222
| -5.751919
|
{'tags': ['Dibismuth distrontium copper hexaoxide']}
| -126.542222
| -5.751919
| -2.040644
|
['xas', 'bandstructure']
| true
|
[67426]
| true
|
2021-05-12 10:57:17.297000
|
NM
| 22
| 8
|
mp-555827
|
oxide
|
Sr2Cu(BiO3)2
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Cu_pv', 'Bi', 'O'], 'pot_type': 'paw'}
|
{'Sr': 2.0, 'Cu': 1.0, 'Bi': 2.0, 'O': 6.0}
|
GGA
|
mp-555827
|
['mp-932594', 'mp-931549', 'mp-918058', 'mp-555827', 'mp-1418436', 'mp-1707731', 'mp-1837530', 'mp-1605675']
| 0.006276
|
{'Sr': 4.0, 'Cu': 2.0, 'Bi': 4.0, 'O': 12.0}
| 360.818997
|
[]
|
NM
| false
| 66
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.000035
| 0.006276
| 0
| 0.012552
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-555827.cif
| false
| null |
data/final/MP/graphs/Bi2Cu1Sr2O6-MP-mp-555827.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
B2Cr0.02Mg0.98
| 2
| 0.013333
| 1
| true
|
B2Cr0.02Mg0.98
|
B2Mg1
| 35.3
|
Other
| true
|
B66.667Cr0.667Mg32.667
|
B-Cr-Mg
| 3
|
Supercon
|
Mg0.98Cr0.02B2
|
MP-mp-763
|
Mg1B2
|
B-Mg
|
B66.667Mg33.333
|
P 6/m m m
|
hexagonal
| 3.07368
| 3.07368
| 3.53435
|
data/final/MP/cifs/B2Cr0.02Mg0.98-MP-mp-763-synth_doped.cif
|
data/source/MP/raw/cifs/mp-763.cif
|
mp-763
| 0
| null |
2011-05-12 17:25:30
| 2.637301
| null | null |
{'GGA': {'task_id': 'mp-1671065'}}
| 0
| 5.985521
| 520
| -15.350083
| -5.116694
|
{'tags': ['Mgnesium boride (1/2)', 'Magnesium boride (1/2)', 'Magnesium boride (1/1)', 'High pressure experimental phase', 'Magensium diboride']}
| -15.350083
| -5.116694
| -0.13034
|
['bandstructure', 'elasticity']
| true
|
[193379, 186389, 94257, 237010, 181869, 96704, 96705, 248441, 96906, 150598, 92831, 155349, 181870, 94256, 182537, 236951, 108064, 93925, 186763, 26675, 248442, 96703, 155347, 153657, 191393, 96706, 92832, 94255, 155348]
| true
|
2021-05-12 10:56:29.056000
|
NM
| 3
| 39
|
mp-763
| null |
MgB2
|
{'functional': 'PBE', 'labels': ['Mg_pv', 'B'], 'pot_type': 'paw'}
|
{'Mg': 1.0, 'B': 2.0}
|
GGA
|
mp-763
|
['mp-905361', 'mp-919554', 'mp-918565', 'mp-763', 'mp-1061708', 'mp-1061762', 'mp-1061948', 'mp-1061909', 'mp-1061934', 'mp-1062061', 'mp-1061740', 'mp-1062105', 'mp-1062081', 'mp-1062570', 'mp-1062589', 'mp-1062612', 'mp-1062861', 'mp-1062883', 'mp-1062892', 'mp-1062941', 'mp-1062925', 'mp-1062999', 'mp-1063048', 'mp-1063024', 'mp-1062914', 'mp-1063249', 'mp-1063291', 'mp-1063269', 'mp-1440873', 'mp-1671065', 'mp-1791068', 'mp-1062931', 'mp-1063035', 'mp-1061942', 'mp-1062096', 'mp-1062604', 'mp-1061753', 'mp-1062912', 'mp-1063282']
| 0.000248
|
{'Mg': 1.0, 'B': 2.0}
| 28.917284
|
[]
|
NM
| false
| 191
| 0
|
[0, 0, 0]
| 0.000009
| 0.000248
| 0
| 0.000248
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-763.cif
| true
| null |
data/final/MP/graphs/B2Cr0.02Mg0.98-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Cu1La2O4.086
| 2
| 0.010403
| 0.978984
| true
|
Cu0.979La1.958O4
|
Cu1La2O4
| 45.2
|
Cuprate
| true
|
Cu14.112La28.225O57.66299745977985
|
Cu-La-O
| 3
|
Supercon
|
La2Cu1O4.086
|
MP-mp-1077929
|
La2Cu1O4
|
Cu-La-O
|
Cu14.286La28.571O57.142857142857146
|
I 4/m m m
|
tetragonal
| 4.008632
| 4.008632
| 6.924232
|
data/final/MP/cifs/Cu1La2O4.086-MP-mp-1077929-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1077929.cif
|
mp-1077929
| 0
| null |
2018-04-10 02:46:14
| 6.630535
| null | null |
{'GGA': {'task_id': 'mp-1699222'}}
| 0
| 6.192985
| 520
| -52.30922
| -7.472746
|
{'tags': ['Dilanthanum tetraoxocuprate(II) - T', "Dilanthanum copper tetraoxide - T'", 'Dilanthanum tetraoxocuprate(II) - T phase, HT']}
| -52.30922
| -7.472746
| -3.042022
|
['bandstructure']
| true
|
[180586, 261659, 261660, 421550]
| true
|
2021-05-12 10:58:14.654000
|
NM
| 7
| 8
|
mp-1077929
|
oxide
|
La2CuO4
|
{'functional': 'PBE', 'labels': ['La', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'La': 2.0, 'Cu': 1.0, 'O': 4.0}
|
GGA
|
mp-1077929
|
['mp-1077929', 'mp-1078177', 'mp-1078187', 'mp-1078189', 'mp-1442004', 'mp-1699222', 'mp-1924066', 'mp-1589927']
| 0.000313
|
{'La': 2.0, 'Cu': 1.0, 'O': 4.0}
| 101.51625
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0, 0, 0]
| 0.000003
| 0.000313
| 0
| 0.000313
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1077929.cif
| true
| null |
data/final/MP/graphs/Cu1La2O4.086-MP-mp-1077929-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Ce2Co1In8
| 1
| 0
| 1
| true
|
Ce2Co1In8
|
Ce2Co1In8
| 0.4
|
Heavy_fermion
| true
|
Ce18.182Co9.091In72.727
|
Ce-Co-In
| 3
|
Supercon
|
Ce2Co1In8
|
MP-mp-19989
|
Ce2In8Co1
|
Ce-Co-In
|
Ce18.182Co9.091In72.727
|
P 4/m m m
|
tetragonal
| 4.663109
| 4.663109
| 12.345552
|
data/final/MP/cifs/Ce2Co1In8-MP-mp-19989.cif
|
data/source/MP/raw/cifs/mp-19989.cif
|
mp-19989
| 0
| null |
2014-02-22 19:40:37
| 7.779787
|
10.17188/1195167
|
@misc{osti_1195167,
author = "Persson, Kristin",
title = "Materials Data on Ce2In8Co (SG:123) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1195167",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1700296'}}
| 0
| 7.903363
| 520
| -44.338071
| -4.030734
|
{'tags': ['Cerium cobalt indium (2/1/8)']}
| -44.338071
| -4.030734
| -0.304555
|
['xas', 'bandstructure']
| true
|
[102109]
| true
|
2021-05-12 10:56:57.051000
|
FiM
| 11
| 7
|
mp-19989
| null |
Ce2In8Co
|
{'functional': 'PBE', 'labels': ['Ce', 'In_d', 'Co'], 'pot_type': 'paw'}
|
{'Ce': 2.0, 'In': 8.0, 'Co': 1.0}
|
GGA
|
mp-19989
|
['mp-991629', 'mp-993547', 'mp-19989', 'mp-1421802', 'mp-1700296', 'mp-994958', 'mp-1608422']
| 0.275921
|
{'Ce': 2.0, 'In': 8.0, 'Co': 1.0}
| 268.448912
|
[]
|
FiM
| true
| 123
| 2
|
[0.1, 0.1, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, -0.1]
| 0.001028
| 0.275921
| 3
| 0.275921
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-19989.cif
| false
| null |
data/final/MP/graphs/Ce2Co1In8-MP-mp-19989.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ba0.199Cu1La1.801O4
| 3
| 0.056857
| 1
| true
|
Ba0.199Cu1La1.801O4
|
Cu1La2O4
| 23.5
|
Cuprate
| true
|
Ba2.843Cu14.286La25.729O57.142857142857146
|
Ba-Cu-La-O
| 4
|
Supercon
|
La1.801Ba0.199Cu1O4
|
MP-mp-1077929
|
La2Cu1O4
|
Cu-La-O
|
Cu14.286La28.571O57.142857142857146
|
I 4/m m m
|
tetragonal
| 4.008632
| 4.008632
| 6.924232
|
data/final/MP/cifs/Ba0.199Cu1La1.801O4-MP-mp-1077929-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1077929.cif
|
mp-1077929
| 0
| null |
2018-04-10 02:46:14
| 6.630535
| null | null |
{'GGA': {'task_id': 'mp-1699222'}}
| 0
| 6.192985
| 520
| -52.30922
| -7.472746
|
{'tags': ['Dilanthanum tetraoxocuprate(II) - T', "Dilanthanum copper tetraoxide - T'", 'Dilanthanum tetraoxocuprate(II) - T phase, HT']}
| -52.30922
| -7.472746
| -3.042022
|
['bandstructure']
| true
|
[180586, 261659, 261660, 421550]
| true
|
2021-05-12 10:58:14.654000
|
NM
| 7
| 8
|
mp-1077929
|
oxide
|
La2CuO4
|
{'functional': 'PBE', 'labels': ['La', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'La': 2.0, 'Cu': 1.0, 'O': 4.0}
|
GGA
|
mp-1077929
|
['mp-1077929', 'mp-1078177', 'mp-1078187', 'mp-1078189', 'mp-1442004', 'mp-1699222', 'mp-1924066', 'mp-1589927']
| 0.000313
|
{'La': 2.0, 'Cu': 1.0, 'O': 4.0}
| 101.51625
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0, 0, 0]
| 0.000003
| 0.000313
| 0
| 0.000313
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1077929.cif
| true
| null |
data/final/MP/graphs/Ba0.199Cu1La1.801O4-MP-mp-1077929-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Nb0.71Sn0.29
| 3
| 0.08
| 8
| false
|
Nb5.68Sn2.32
|
Nb6Sn2
| 18.3
|
Other
| true
|
Nb71Sn29
|
Nb-Sn
| 2
|
Supercon
|
Nb0.71Sn0.29
|
MP-mp-1326
|
Nb6Sn2
|
Nb-Sn
|
Nb75Sn25
|
P m -3 n
|
cubic
| 5.334611
| 5.334611
| 5.334611
|
data/final/MP/cifs/Nb0.71Sn0.29-MP-mp-1326-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1326.cif
|
mp-1326
| 0
| null |
2011-05-14 09:51:48
| 8.694218
|
10.17188/1189484
|
@misc{osti_1189484,
author = "Persson, Kristin",
title = "Materials Data on Nb3Sn (SG:223) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1189484",
place = "United States",
year = "2015",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1668415'}}
| 0
| 6.593725
| 520
| -69.93787
| -8.742234
|
{'tags': ['Niobium tin (3/1)']}
| -69.93787
| -8.742234
| -0.163862
|
['xas', 'elasticity', 'bandstructure']
| true
|
[105230, 645503, 645489, 105231, 645498, 645485, 645474, 645496, 645480, 645488, 645482, 645487, 645500, 645493, 645477, 645484, 645502, 645483, 150878, 645479, 645481, 645486, 645473]
| true
|
2021-05-12 10:56:12.755000
|
NM
| 8
| 9
|
mp-1326
| null |
Nb3Sn
|
{'functional': 'PBE', 'labels': ['Nb_pv', 'Sn_d'], 'pot_type': 'paw'}
|
{'Nb': 3.0, 'Sn': 1.0}
|
GGA
|
mp-1326
|
['mp-930046', 'mp-913770', 'mp-930577', 'mp-1326', 'mp-1440651', 'mp-1668415', 'mp-1880085', 'mp-1594093', 'mp-1594507']
| 0.620231
|
{'Nb': 6.0, 'Sn': 2.0}
| 151.812757
|
[]
|
NM
| false
| 223
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0]
| 0.008171
| 0.620231
| 0
| 1.240462
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1326.cif
| true
| null |
data/final/MP/graphs/Nb0.71Sn0.29-MP-mp-1326-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
C1S1
| 1
| 0
| 2
| false
|
C2S2
|
C2S2
| 9
|
Other
| true
|
C50S50
|
C-S
| 2
|
Supercon
|
C1S1
|
MP-mp-1147643
|
C2S2
|
C-S
|
C50S50
|
P 4/n m m
|
tetragonal
| 3.564824
| 3.564824
| 4.126673
|
data/final/MP/cifs/C1S1-MP-mp-1147643.cif
|
data/source/MP/raw/cifs/mp-1147643.cif
|
mp-1147643
| 0
| null |
2018-12-27 11:39:53.428000
| 2.791271
| null | null |
{'GGA': {'task_id': 'mp-1766782'}}
| 1.346285
| 6.504064
| 520
| -21.207055
| -5.301764
|
{'tags': []}
| -21.207055
| -5.301764
| 1.128351
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:22.271000
|
NM
| 4
| 5
|
mp-1147643
| null |
CS
|
{'functional': 'PBE', 'labels': ['C', 'S'], 'pot_type': 'paw'}
|
{'C': 1.0, 'S': 1.0}
|
GGA
|
mp-1147643
|
['mp-1147643', 'mp-1437515', 'mp-1766782', 'mp-1794510', 'mp-1585021']
| 0.000064
|
{'C': 2.0, 'S': 2.0}
| 52.441637
|
[]
|
NM
| false
| 129
| 0
|
[0, 0, 0, 0]
| 0.000002
| 0.000064
| 0
| 0.000129
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1147643.cif
| false
| null |
data/final/MP/graphs/C1S1-MP-mp-1147643.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Rh1Se2
| 1
| 0
| 8
| false
|
Rh8Se16
|
Rh8Se16
| 4.35
|
Other
| true
|
Rh33.333Se66.667
|
Rh-Se
| 2
|
Supercon
|
Rh1Se2
|
MP-mp-1192175
|
Rh8Se16
|
Rh-Se
|
Rh33.333Se66.667
|
P n m a
|
orthorhombic
| 3.789183
| 6.02896
| 21.222951
|
data/final/MP/cifs/Rh1Se2-MP-mp-1192175.cif
|
data/source/MP/raw/cifs/mp-1192175.cif
|
mp-1192175
| 0
| null |
2019-01-11 22:16:22.535000
| 7.146533
| null | null |
{'GGA': {'task_id': 'mp-1735789'}}
| 0
| 4.944093
| 520
| -125.115543
| -5.213148
|
{'tags': ['Rhodium selenide (1/2)']}
| -125.115543
| -5.213148
| -0.742437
|
['bandstructure']
| true
|
[650286]
| true
|
2021-05-12 10:58:35.561000
|
NM
| 24
| 5
|
mp-1192175
| null |
RhSe2
|
{'functional': 'PBE', 'labels': ['Rh_pv', 'Se'], 'pot_type': 'paw'}
|
{'Rh': 1.0, 'Se': 2.0}
|
GGA
|
mp-1192175
|
['mp-1192175', 'mp-1400105', 'mp-1735789', 'mp-1823453', 'mp-1585083']
| 0.000022
|
{'Rh': 8.0, 'Se': 16.0}
| 484.834766
|
[]
|
NM
| false
| 62
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0
| 0.000022
| 0
| 0.00018
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1192175.cif
| false
| null |
data/final/MP/graphs/Rh1Se2-MP-mp-1192175.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Pd1Tl2
| 1
| 0
| 2
| false
|
Pd2Tl4
|
Pd2Tl4
| 1.32
|
Other
| true
|
Pd33.333Tl66.667
|
Pd-Tl
| 2
|
Supercon
|
Pd1Tl2
|
MP-mp-570896
|
Tl4Pd2
|
Pd-Tl
|
Pd33.333Tl66.667
|
I 4/m c m
|
tetragonal
| 5.690532
| 5.690532
| 5.690532
|
data/final/MP/cifs/Pd1Tl2-MP-mp-570896.cif
|
data/source/MP/raw/cifs/mp-570896.cif
|
mp-570896
| 0
| null |
2014-02-16 13:07:44
| 12.240631
|
10.17188/1275990
|
@misc{osti_1275990,
author = "Persson, Kristin",
title = "Materials Data on Tl2Pd (SG:140) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1275990",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1699723'}}
| 0
| 6.60457
| 520
| -20.557013
| -3.426169
|
{'tags': ['Palladium thallium (1/2)']}
| -20.557013
| -3.426169
| -0.124446
|
['xas', 'elasticity', 'bandstructure']
| true
|
[649064, 102796, 649057]
| true
|
2021-05-12 10:56:27.046000
|
NM
| 6
| 10
|
mp-570896
| null |
Tl2Pd
|
{'functional': 'PBE', 'labels': ['Tl_d', 'Pd'], 'pot_type': 'paw'}
|
{'Tl': 2.0, 'Pd': 1.0}
|
GGA
|
mp-570896
|
['mp-941536', 'mp-941235', 'mp-934754', 'mp-570896', 'mp-1077324', 'mp-1077371', 'mp-1417388', 'mp-1699723', 'mp-1779615', 'mp-1591346']
| 0.001807
|
{'Tl': 4.0, 'Pd': 2.0}
| 139.778333
|
[]
|
NM
| false
| 140
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000026
| 0.001807
| 0
| 0.003613
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-570896.cif
| false
| null |
data/final/MP/graphs/Pd1Tl2-MP-mp-570896.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
C1Rh1
| 1
| 0
| 1
| true
|
C1Rh1
|
C1Rh1
| 1.666667
|
Other
| true
|
C50Rh50
|
C-Rh
| 2
|
Supercon
|
C1Rh1
|
MP-mp-1009696
|
Rh1C1
|
C-Rh
|
C50Rh50
|
F -4 3 m
|
cubic
| 3.253717
| 3.253717
| 3.253717
|
data/final/MP/cifs/C1Rh1-MP-mp-1009696.cif
|
data/source/MP/raw/cifs/mp-1009696.cif
|
mp-1009696
| 0
| null |
2016-09-22 04:22:47
| 7.834407
|
10.17188/1326274
|
@misc{osti_1326274,
author = "Persson, Kristin",
title = "Materials Data on RhC (SG:216) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1326274",
place = "United States",
year = "2016",
month = "9",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1687924'}}
| 0.559717
| 5.945287
| 520
| -15.471655
| -7.735828
|
{'tags': ['Rhodium carbide (1/1) - ZB-type']}
| -15.471655
| -7.735828
| 0.559717
|
['xas', 'elasticity', 'bandstructure']
| true
|
[183172]
| true
|
2021-05-12 10:56:08.727000
|
NM
| 2
| 12
|
mp-1009696
| null |
RhC
|
{'functional': 'PBE', 'labels': ['Rh_pv', 'C'], 'pot_type': 'paw'}
|
{'Rh': 1.0, 'C': 1.0}
|
GGA
|
mp-1009696
|
['mp-1059717', 'mp-1059778', 'mp-1059740', 'mp-1009696', 'mp-1009744', 'mp-1009758', 'mp-1436316', 'mp-1687924', 'mp-1793336', 'mp-1009772', 'mp-1612052', 'mp-1059763']
| 0.000867
|
{'Rh': 1.0, 'C': 1.0}
| 24.357024
|
[]
|
NM
| false
| 216
| 0
|
[0, 0]
| 0.000036
| 0.000867
| 0
| 0.000867
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1009696.cif
| false
| null |
data/final/MP/graphs/C1Rh1-MP-mp-1009696.json
| 0
| true
|
-43m
| 5
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
La0.9Sr0.1Ti1O3
| 3
| 0.093333
| 3
| false
|
La2.7Sr0.3Ti3O9
|
La2Sr1Ti3O9
| 0
|
Oxide
| true
|
La18Sr2Ti20O60
|
La-Sr-Ti-O
| 4
|
Supercon
|
La0.9Sr0.1Ti1O3
|
MP-mp-1218904
|
Sr1La2Ti3O9
|
La-Sr-Ti-O
|
La13.333Sr6.667Ti20O60
|
P -3 m 1
|
trigonal
| 5.585068
| 5.585068
| 6.830672
|
data/final/MP/cifs/La0.9Sr0.1Ti1O3-MP-mp-1218904-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1218904.cif
|
mp-1218904
| 0
| null |
2019-01-12 19:59:48.166000
| 5.876638
| null | null |
{'GGA': {'task_id': 'mp-1736640'}}
| 0.023044
| 8.532925
| 520
| -127.76199
| -8.517466
|
{'tags': []}
| -127.76199
| -8.517466
| -3.611024
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:42.526000
|
NM
| 15
| 4
|
mp-1218904
|
oxide
|
SrLa2Ti3O9
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'La', 'Ti_pv', 'O'], 'pot_type': 'paw'}
|
{'Sr': 1.0, 'La': 2.0, 'Ti': 3.0, 'O': 9.0}
|
GGA
|
mp-1218904
|
['mp-1218904', 'mp-1406224', 'mp-1736640', 'mp-1828534']
| 0.000405
|
{'Sr': 1.0, 'La': 2.0, 'Ti': 3.0, 'O': 9.0}
| 184.523216
|
[]
|
NM
| false
| 164
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000002
| 0.000405
| 0
| 0.000405
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1218904.cif
| true
| null |
data/final/MP/graphs/La0.9Sr0.1Ti1O3-MP-mp-1218904-synth_doped.json
| 0
| true
|
-3m
| 0
| 0
| 0
| 0
| 0
| 0
| 6
| 1
| 0
| 0
| 0
| 1
| false
|
B1.96F0.04Mg1
| 2
| 0.026667
| 1
| true
|
B1.96F0.04Mg1
|
B2Mg1
| 30
|
Other
| true
|
B65.333F1.333Mg33.333
|
B-F-Mg
| 3
|
Supercon
|
Mg1B1.96F0.04
|
MP-mp-763
|
Mg1B2
|
B-Mg
|
B66.667Mg33.333
|
P 6/m m m
|
hexagonal
| 3.07368
| 3.07368
| 3.53435
|
data/final/MP/cifs/B1.96F0.04Mg1-MP-mp-763-synth_doped.cif
|
data/source/MP/raw/cifs/mp-763.cif
|
mp-763
| 0
| null |
2011-05-12 17:25:30
| 2.637301
| null | null |
{'GGA': {'task_id': 'mp-1671065'}}
| 0
| 5.985521
| 520
| -15.350083
| -5.116694
|
{'tags': ['Mgnesium boride (1/2)', 'Magnesium boride (1/2)', 'Magnesium boride (1/1)', 'High pressure experimental phase', 'Magensium diboride']}
| -15.350083
| -5.116694
| -0.13034
|
['bandstructure', 'elasticity']
| true
|
[193379, 186389, 94257, 237010, 181869, 96704, 96705, 248441, 96906, 150598, 92831, 155349, 181870, 94256, 182537, 236951, 108064, 93925, 186763, 26675, 248442, 96703, 155347, 153657, 191393, 96706, 92832, 94255, 155348]
| true
|
2021-05-12 10:56:29.056000
|
NM
| 3
| 39
|
mp-763
| null |
MgB2
|
{'functional': 'PBE', 'labels': ['Mg_pv', 'B'], 'pot_type': 'paw'}
|
{'Mg': 1.0, 'B': 2.0}
|
GGA
|
mp-763
|
['mp-905361', 'mp-919554', 'mp-918565', 'mp-763', 'mp-1061708', 'mp-1061762', 'mp-1061948', 'mp-1061909', 'mp-1061934', 'mp-1062061', 'mp-1061740', 'mp-1062105', 'mp-1062081', 'mp-1062570', 'mp-1062589', 'mp-1062612', 'mp-1062861', 'mp-1062883', 'mp-1062892', 'mp-1062941', 'mp-1062925', 'mp-1062999', 'mp-1063048', 'mp-1063024', 'mp-1062914', 'mp-1063249', 'mp-1063291', 'mp-1063269', 'mp-1440873', 'mp-1671065', 'mp-1791068', 'mp-1062931', 'mp-1063035', 'mp-1061942', 'mp-1062096', 'mp-1062604', 'mp-1061753', 'mp-1062912', 'mp-1063282']
| 0.000248
|
{'Mg': 1.0, 'B': 2.0}
| 28.917284
|
[]
|
NM
| false
| 191
| 0
|
[0, 0, 0]
| 0.000009
| 0.000248
| 0
| 0.000248
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-763.cif
| true
| null |
data/final/MP/graphs/B1.96F0.04Mg1-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B2Er1Rh3
| 1
| 0
| 1
| true
|
B2Er1Rh3
|
B2Er1Rh3
| 0
|
Other
| true
|
B33.333Er16.667Rh50
|
B-Er-Rh
| 3
|
Supercon
|
Er1Rh3B2
|
MP-mp-5678
|
Er1B2Rh3
|
B-Er-Rh
|
B33.333Er16.667Rh50
|
P 6/m m m
|
hexagonal
| 3.121585
| 5.425844
| 5.425843
|
data/final/MP/cifs/B2Er1Rh3-MP-mp-5678.cif
|
data/source/MP/raw/cifs/mp-5678.cif
|
mp-5678
| 0
| null |
2011-05-13 09:49:54
| 10.382142
|
10.17188/1274057
|
@misc{osti_1274057,
author = "Persson, Kristin",
title = "Materials Data on ErB2Rh3 (SG:191) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1274057",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1677748'}}
| 0.012206
| 6.36128
| 520
| -44.267623
| -7.377937
|
{'tags': ['Erbium trirhodium(I) boride', 'Erbium rhodium boride (1/3/2)']}
| -44.267623
| -7.377937
| -0.708033
|
['xas', 'bandstructure']
| true
|
[81614, 72568, 613803, 656228]
| true
|
2021-05-12 10:57:23.123000
|
NM
| 6
| 9
|
mp-5678
| null |
ErB2Rh3
|
{'functional': 'PBE', 'labels': ['Er_3', 'B', 'Rh_pv'], 'pot_type': 'paw'}
|
{'Er': 1.0, 'B': 2.0, 'Rh': 3.0}
|
GGA
|
mp-5678
|
['mp-5678', 'mp-923599', 'mp-922818', 'mp-908517', 'mp-1077574', 'mp-1438488', 'mp-1677748', 'mp-1799957', 'mp-1587673']
| 0.006878
|
{'Er': 1.0, 'B': 2.0, 'Rh': 3.0}
| 79.58667
|
[]
|
NM
| false
| 191
| 0
|
[-0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.000086
| 0.006878
| 0
| 0.006878
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-5678.cif
| false
| null |
data/final/MP/graphs/B2Er1Rh3-MP-mp-5678.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ga1Mn0.102V2.898
| 3
| 0.051
| 2
| false
|
Ga2Mn0.204V5.796
|
Ga2V6
| 9
|
Other
| true
|
Ga25Mn2.55V72.45
|
Ga-Mn-V
| 3
|
Supercon
|
V2.898Mn0.102Ga1
|
MP-mp-22568
|
V6Ga2
|
Ga-V
|
Ga25V75
|
P m -3 n
|
cubic
| 4.789645
| 4.789645
| 4.789645
|
data/final/MP/cifs/Ga1Mn0.102V2.898-MP-mp-22568-synth_doped.cif
|
data/source/MP/raw/cifs/mp-22568.cif
|
mp-22568
| 0
| null |
2014-02-22 11:36:40
| 6.726542
|
10.17188/1198793
|
@misc{osti_1198793,
author = "Persson, Kristin",
title = "Materials Data on V3Ga (SG:223) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1198793",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1686867'}}
| 0
| 5.674522
| 520
| -61.952443
| -7.744055
|
{'tags': ['Gallium vanadium (1/3)']}
| -61.952443
| -7.744055
| -0.174102
|
['xas', 'elasticity', 'bandstructure']
| true
|
[635643, 635628, 635619, 635634, 104021, 635646, 635604, 635610, 635617, 635624, 635626, 635605, 635631, 635625, 635636, 635603, 104020, 635616, 635607]
| true
|
2021-05-12 10:56:16.728000
|
FM
| 8
| 9
|
mp-22568
| null |
V3Ga
|
{'functional': 'PBE', 'labels': ['V_pv', 'Ga_d'], 'pot_type': 'paw'}
|
{'V': 3.0, 'Ga': 1.0}
|
GGA
|
mp-22568
|
['mp-941343', 'mp-941663', 'mp-934924', 'mp-22568', 'mp-1440749', 'mp-1686867', 'mp-1804076', 'mp-1593784', 'mp-1595713']
| 0.090636
|
{'V': 6.0, 'Ga': 2.0}
| 109.877805
|
[]
|
FM
| true
| 131
| 1
|
[0.0, 0.0, 0.1, 0.1, 0.0, 0.0, -0.0, -0.0]
| 0.00165
| 0.090636
| 2
| 0.181273
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-22568.cif
| true
| null |
data/final/MP/graphs/Ga1Mn0.102V2.898-MP-mp-22568-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
As1Fe1Gd1O0.85
| 3
| 0.058442
| 2
| false
|
As2Fe2Gd2O1.7
|
As2Fe2Gd2O2
| 53.5
|
Ferrite
| true
|
As25.974Fe25.974Gd25.974O22.07792207792208
|
As-Fe-Gd-O
| 4
|
Supercon
|
Gd1Fe1As1O0.85
|
MP-mp-1078679
|
Gd2Fe2As2O2
|
As-Fe-Gd-O
|
As25Fe25Gd25O25
|
P 4/n m m
|
tetragonal
| 3.996524
| 3.996524
| 9.110606
|
data/final/MP/cifs/As1Fe1Gd1O0.85-MP-mp-1078679-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1078679.cif
|
mp-1078679
| 0
| null |
2018-04-12 14:54:44
| 6.938465
| null | null |
{'GGA+U': {'task_id': 'mp-1704492'}}
| 0.275698
| 4.068827
| 520
| -71.784984
| -8.973123
|
{'tags': ['Gadolinium iron arsenic oxide (1/1/1/1)']}
| -71.784984
| -8.973123
| -1.67057
|
['bandstructure']
| true
|
[425013, 422003, 425006, 425015, 425010, 236655, 425016]
| true
|
2021-05-12 10:58:16.596000
|
FM
| 8
| 10
|
mp-1078679
|
oxide
|
GdFeAsO
|
{'functional': 'PBE', 'labels': ['Gd', 'Fe_pv', 'As', 'O'], 'pot_type': 'paw'}
|
{'Gd': 1.0, 'Fe': 1.0, 'As': 1.0, 'O': 1.0}
|
GGA+U
|
mp-1078679
|
['mp-1078679', 'mp-1079389', 'mp-1079927', 'mp-1080502', 'mp-1080613', 'mp-1095209', 'mp-1438268', 'mp-1704492', 'mp-1864230', 'mp-1589235']
| 10.799094
|
{'Gd': 2.0, 'Fe': 2.0, 'As': 2.0, 'O': 2.0}
| 145.516458
|
[]
|
FM
| true
| 129
| 2
|
[6.9, 6.9, 3.6, 3.6, 0.0, 0.0, 0.0, 0.0]
| 0.148424
| 10.799094
| 4
| 21.598188
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1078679.cif
| true
| null |
data/final/MP/graphs/As1Fe1Gd1O0.85-MP-mp-1078679-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B5Mo1.7Ti0.3
| 3
| 0.085714
| 1
| true
|
B5Mo1.7Ti0.3
|
B5Mo2
| 7.1
|
Other
| true
|
B71.429Mo24.286Ti4.286
|
B-Mo-Ti
| 3
|
Supercon
|
B5Mo1.7Ti0.3
|
MP-mp-7229
|
B5Mo2
|
B-Mo
|
B71.429Mo28.571
|
R -3 m
|
trigonal
| 3.086062
| 3.086062
| 7.383175
|
data/final/MP/cifs/B5Mo1.7Ti0.3-MP-mp-7229-synth_doped.cif
|
data/source/MP/raw/cifs/mp-7229.cif
|
mp-7229
| 0
| null |
2011-05-27 17:15:57
| 6.910598
|
10.17188/1287525
|
@misc{osti_1287525,
author = "Persson, Kristin",
title = "Materials Data on B5Mo2 (SG:166) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1287525",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1678538'}}
| 0.435474
| 10.261596
| 520
| -54.63027
| -7.804324
|
{'tags': ['Molybdenum boride (2/5)', 'Molybdenum boride (1/2.5) - epsilon']}
| -54.63027
| -7.804324
| 0.065425
|
['bandstructure']
| true
|
[157530, 614795, 614810, 24282]
| true
|
2021-05-12 10:58:55.498000
|
NM
| 7
| 11
|
mp-7229
| null |
B5Mo2
|
{'functional': 'PBE', 'labels': ['B', 'Mo_pv'], 'pot_type': 'paw'}
|
{'B': 5.0, 'Mo': 2.0}
|
GGA
|
mp-7229
|
['mp-1001204', 'mp-7229', 'mp-1007569', 'mp-1077992', 'mp-1078025', 'mp-1078031', 'mp-1441558', 'mp-1678538', 'mp-1793658', 'mp-1012321', 'mp-1593525']
| 0.01891
|
{'B': 5.0, 'Mo': 2.0}
| 59.09542
|
[]
|
NM
| false
| 166
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, -0.0, -0.0]
| 0.00032
| 0.01891
| 0
| 0.01891
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-7229.cif
| true
| null |
data/final/MP/graphs/B5Mo1.7Ti0.3-MP-mp-7229-synth_doped.json
| 0
| true
|
-3m
| 0
| 0
| 0
| 0
| 0
| 0
| 6
| 1
| 0
| 0
| 0
| 1
| false
|
Au0.7Nb3Rh0.3
| 3
| 0.15
| 1
| true
|
Au0.7Nb3Rh0.3
|
Au1Nb3
| 9.5
|
Other
| true
|
Au17.5Nb75Rh7.5
|
Au-Nb-Rh
| 3
|
Supercon
|
Nb3Rh0.3Au0.7
|
MP-mp-1220645
|
Nb3Au1
|
Au-Nb
|
Au25Nb75
|
C m m m
|
orthorhombic
| 2.825692
| 2.825692
| 9.314665
|
data/final/MP/cifs/Au0.7Nb3Rh0.3-MP-mp-1220645-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1220645.cif
|
mp-1220645
| 0
| null |
2019-01-12 21:27:35.806000
| 10.906576
| null | null |
{'GGA': {'task_id': 'mp-1767853'}}
| 0.020744
| 5.246022
| 520
| -33.863543
| -8.465886
|
{'tags': []}
| -33.863543
| -8.465886
| -0.071436
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:43.502000
|
NM
| 4
| 5
|
mp-1220645
| null |
Nb3Au
|
{'functional': 'PBE', 'labels': ['Nb_pv', 'Au'], 'pot_type': 'paw'}
|
{'Nb': 3.0, 'Au': 1.0}
|
GGA
|
mp-1220645
|
['mp-1220645', 'mp-1416545', 'mp-1767853', 'mp-1799245', 'mp-1612990']
| 0.005137
|
{'Nb': 3.0, 'Au': 1.0}
| 72.423709
|
[]
|
NM
| false
| 65
| 0
|
[0, 0, 0, 0]
| 0.000071
| 0.005137
| 0
| 0.005137
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1220645.cif
| true
| null |
data/final/MP/graphs/Au0.7Nb3Rh0.3-MP-mp-1220645-synth_doped.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Ga0.999V3Zn0.001
| 2
| 0.0005
| 2
| false
|
Ga1.998V6Zn0.002
|
Ga2V6
| 10.2
|
Other
| true
|
Ga24.975V75Zn0.025
|
Ga-V-Zn
| 3
|
Supercon
|
V3Ga0.999Zn0.001
|
MP-mp-22568
|
V6Ga2
|
Ga-V
|
Ga25V75
|
P m -3 n
|
cubic
| 4.789645
| 4.789645
| 4.789645
|
data/final/MP/cifs/Ga0.999V3Zn0.001-MP-mp-22568-synth_doped.cif
|
data/source/MP/raw/cifs/mp-22568.cif
|
mp-22568
| 0
| null |
2014-02-22 11:36:40
| 6.726542
|
10.17188/1198793
|
@misc{osti_1198793,
author = "Persson, Kristin",
title = "Materials Data on V3Ga (SG:223) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1198793",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1686867'}}
| 0
| 5.674522
| 520
| -61.952443
| -7.744055
|
{'tags': ['Gallium vanadium (1/3)']}
| -61.952443
| -7.744055
| -0.174102
|
['xas', 'elasticity', 'bandstructure']
| true
|
[635643, 635628, 635619, 635634, 104021, 635646, 635604, 635610, 635617, 635624, 635626, 635605, 635631, 635625, 635636, 635603, 104020, 635616, 635607]
| true
|
2021-05-12 10:56:16.728000
|
FM
| 8
| 9
|
mp-22568
| null |
V3Ga
|
{'functional': 'PBE', 'labels': ['V_pv', 'Ga_d'], 'pot_type': 'paw'}
|
{'V': 3.0, 'Ga': 1.0}
|
GGA
|
mp-22568
|
['mp-941343', 'mp-941663', 'mp-934924', 'mp-22568', 'mp-1440749', 'mp-1686867', 'mp-1804076', 'mp-1593784', 'mp-1595713']
| 0.090636
|
{'V': 6.0, 'Ga': 2.0}
| 109.877805
|
[]
|
FM
| true
| 131
| 1
|
[0.0, 0.0, 0.1, 0.1, 0.0, 0.0, -0.0, -0.0]
| 0.00165
| 0.090636
| 2
| 0.181273
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-22568.cif
| true
| null |
data/final/MP/graphs/Ga0.999V3Zn0.001-MP-mp-22568-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
C0.77Nb1
| 3
| 0.129944
| 1
| true
|
C0.77Nb1
|
C1Nb1
| 0
|
Other
| true
|
C43.503Nb56.497
|
C-Nb
| 2
|
Supercon
|
Nb1C0.77
|
MP-mp-910
|
Nb1C1
|
C-Nb
|
C50Nb50
|
F m -3 m
|
cubic
| 3.186343
| 3.186343
| 3.186343
|
data/final/MP/cifs/C0.77Nb1-MP-mp-910-synth_doped.cif
|
data/source/MP/raw/cifs/mp-910.cif
|
mp-910
| 0
| null |
2011-05-12 17:28:40
| 7.616099
|
10.17188/1282001
|
@misc{osti_1282001,
author = "Persson, Kristin",
title = "Materials Data on NbC (SG:225) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1282001",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1686610'}}
| 0.040875
| 7.39993
| 520
| -20.246334
| -10.123167
|
{'tags': ['Niobium carbide (1/1)', 'Niobium carbide (1/1) - RS-type']}
| -20.246334
| -10.123167
| -0.459124
|
['xas', 'elasticity', 'bandstructure']
| true
|
[618465, 77214, 187077, 618456, 181792, 618453, 94449, 618472, 183163, 237582, 618457, 159872, 618480, 618475, 618482, 618469, 155164, 618466, 44355, 618450, 618458, 618449, 44496, 618463, 618462, 618460, 618481, 618471, 618476, 181052, 601142, 618448, 189089, 618478, 26955, 618473, 618484, 618483]
| true
|
2021-05-12 10:56:35.166000
|
NM
| 2
| 25
|
mp-910
| null |
NbC
|
{'functional': 'PBE', 'labels': ['Nb_pv', 'C'], 'pot_type': 'paw'}
|
{'Nb': 1.0, 'C': 1.0}
|
GGA
|
mp-910
|
['mp-1000444', 'mp-1001333', 'mp-910', 'mp-1057158', 'mp-1057178', 'mp-1057130', 'mp-1057651', 'mp-1057669', 'mp-1057682', 'mp-1057771', 'mp-1057779', 'mp-1057802', 'mp-1060960', 'mp-1060978', 'mp-1061015', 'mp-1440938', 'mp-1686610', 'mp-1805660', 'mp-1007673', 'mp-1593845', 'mp-1596940', 'mp-1061007', 'mp-1057677', 'mp-1057792', 'mp-1057174']
| 0.000033
|
{'Nb': 1.0, 'C': 1.0}
| 22.875085
|
[]
|
NM
| false
| 225
| 0
|
[0, 0]
| 0.000001
| 0.000033
| 0
| 0.000033
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-910.cif
| true
| null |
data/final/MP/graphs/C0.77Nb1-MP-mp-910-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
La1N0.98
| 2
| 0.010101
| 2
| false
|
La2N1.96
|
La2N2
| 0
|
Other
| true
|
La50.505N49.495
|
La-N
| 2
|
Supercon
|
La1N0.98
|
MP-mp-567290
|
La2N2
|
La-N
|
La50N50
|
P 63 m c
|
hexagonal
| 4.132864
| 4.132865
| 5.960067
|
data/final/MP/cifs/La1N0.98-MP-mp-567290-synth_doped.cif
|
data/source/MP/raw/cifs/mp-567290.cif
|
mp-567290
| 1.1489
| null |
2013-09-22 15:00:24
| 5.760193
|
10.17188/1273789
|
@misc{osti_1273789,
author = "Persson, Kristin",
title = "Materials Data on LaN (SG:186) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1273789",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1712385'}}
| 0
| 6.322369
| 520
| -31.828084
| -7.957021
|
{'tags': ['Lanthanum nitride']}
| -31.828084
| -7.957021
| -1.50127
|
['piezo', 'bandstructure', 'diel', 'phonons', 'elasticity']
| true
|
[162195]
| true
|
2021-05-12 10:56:22.739000
|
NM
| 4
| 10
|
mp-567290
| null |
LaN
|
{'functional': 'PBE', 'labels': ['La', 'N'], 'pot_type': 'paw'}
|
{'La': 1.0, 'N': 1.0}
|
GGA
|
mp-567290
|
['mp-655510', 'mp-663539', 'mp-658377', 'mp-567290', 'mp-1141817', 'mp-1119521', 'mp-1434771', 'mp-1712385', 'mp-1801348', 'mp-1617444']
| 0.000006
|
{'La': 2.0, 'N': 2.0}
| 88.162541
|
[]
|
NM
| false
| 186
| 0
|
[0, 0, 0, 0]
| 0
| 0.000006
| 0
| 0.000012
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-567290.cif
| true
| null |
data/final/MP/graphs/La1N0.98-MP-mp-567290-synth_doped.json
| 0
| true
|
6mm
| 0
| 5
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ge1.85La1
| 2
| 0.035088
| 2
| false
|
Ge3.7La2
|
Ge4La2
| 2.17
|
Other
| true
|
Ge64.912La35.088
|
Ge-La
| 2
|
Supercon
|
Ge1.85La1
|
MP-mp-19761
|
La2Ge4
|
Ge-La
|
Ge66.667La33.333
|
I 41/a m d
|
tetragonal
| 4.320984
| 4.320984
| 8.414846
|
data/final/MP/cifs/Ge1.85La1-MP-mp-19761-synth_doped.cif
|
data/source/MP/raw/cifs/mp-19761.cif
|
mp-19761
| 0
| null |
2014-02-21 13:34:05
| 6.447172
|
10.17188/1194966
|
@misc{osti_1194966,
author = "Persson, Kristin",
title = "Materials Data on LaGe2 (SG:141) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1194966",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1703381'}}
| 0.005902
| 6.245638
| 520
| -32.498392
| -5.416399
|
{'tags': ['Lanthanum germanide (1/2)', 'Germanium lanthanum (2/1)']}
| -32.498392
| -5.416399
| -0.689044
|
['xas', 'elasticity', 'bandstructure']
| true
|
[636796, 636784, 57072]
| true
|
2021-05-12 10:56:14.760000
|
NM
| 6
| 6
|
mp-19761
| null |
LaGe2
|
{'functional': 'PBE', 'labels': ['La', 'Ge_d'], 'pot_type': 'paw'}
|
{'La': 1.0, 'Ge': 2.0}
|
GGA
|
mp-19761
|
['mp-19761', 'mp-20013', 'mp-1438339', 'mp-1703381', 'mp-1780058', 'mp-1596448']
| 0.000228
|
{'La': 2.0, 'Ge': 4.0}
| 146.39009
|
[]
|
NM
| false
| 141
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000003
| 0.000228
| 0
| 0.000455
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-19761.cif
| true
| null |
data/final/MP/graphs/Ge1.85La1-MP-mp-19761-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Ce1In5Ir0.978Pt0.022
| 2
| 0.006286
| 1
| true
|
Ce1In5Ir0.978Pt0.022
|
Ce1In5Ir1
| 0.734
|
Heavy_fermion
| true
|
Ce14.286In71.429Ir13.971Pt0.314
|
Ce-In-Ir-Pt
| 4
|
Supercon
|
Ce1Ir0.978Pt0.022In5
|
MP-mp-20975
|
Ce1In5Ir1
|
Ce-In-Ir
|
Ce14.286In71.429Ir14.286
|
P 4/m m m
|
tetragonal
| 4.724199
| 4.724199
| 7.575801
|
data/final/MP/cifs/Ce1In5Ir0.978Pt0.022-MP-mp-20975-synth_doped.cif
|
data/source/MP/raw/cifs/mp-20975.cif
|
mp-20975
| 0
| null |
2014-02-21 16:15:16
| 8.902154
|
10.17188/1196209
|
@misc{osti_1196209,
author = "Persson, Kristin",
title = "Materials Data on CeIn5Ir (SG:123) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1196209",
place = "United States",
year = "2015",
month = "1",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1688300'}}
| 0
| 8.149849
| 520
| -31.206957
| -4.458137
|
{'tags': ['Cerium iridium indide (1/1/5)']}
| -31.206957
| -4.458137
| -0.382431
|
['xas', 'bandstructure']
| true
|
[150225]
| true
|
2021-05-12 10:56:57.051000
|
FM
| 7
| 8
|
mp-20975
| null |
CeIn5Ir
|
{'functional': 'PBE', 'labels': ['Ce', 'In_d', 'Ir'], 'pot_type': 'paw'}
|
{'Ce': 1.0, 'In': 5.0, 'Ir': 1.0}
|
GGA
|
mp-20975
|
['mp-919528', 'mp-918523', 'mp-905302', 'mp-20975', 'mp-1300982', 'mp-1688300', 'mp-1832383', 'mp-1591628']
| 0.104019
|
{'Ce': 1.0, 'In': 5.0, 'Ir': 1.0}
| 169.077152
|
[]
|
FM
| true
| 123
| 1
|
[0.1, -0.0, -0.0, -0.0, -0.0, -0.0, -0.0]
| 0.000615
| 0.104019
| 1
| 0.104019
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-20975.cif
| true
| null |
data/final/MP/graphs/Ce1In5Ir0.978Pt0.022-MP-mp-20975-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Pt0.5W0.5
| 1
| 0
| 2
| false
|
Pt1W1
|
Pt1W1
| 1.45
|
Other
| true
|
Pt50W50
|
Pt-W
| 2
|
Supercon
|
Pt0.5W0.5
|
MP-mp-1219711
|
Pt1W1
|
Pt-W
|
Pt50W50
|
R -3 m
|
trigonal
| 2.813372
| 2.813372
| 4.88791
|
data/final/MP/cifs/Pt0.5W0.5-MP-mp-1219711.cif
|
data/source/MP/raw/cifs/mp-1219711.cif
|
mp-1219711
| 0
| null |
2019-01-12 20:40:23.171000
| 19.911454
| null | null |
{'GGA': {'task_id': 'mp-1674667'}}
| 0.206545
| 7.591108
| 520
| -19.120089
| -9.560044
|
{'tags': []}
| -19.120089
| -9.560044
| -0.045527
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:41.460000
|
NM
| 2
| 5
|
mp-1219711
| null |
PtW
|
{'functional': 'PBE', 'labels': ['Pt', 'W_pv'], 'pot_type': 'paw'}
|
{'Pt': 1.0, 'W': 1.0}
|
GGA
|
mp-1219711
|
['mp-1219711', 'mp-1414335', 'mp-1674667', 'mp-1792593', 'mp-1609705']
| 0.000001
|
{'Pt': 1.0, 'W': 1.0}
| 31.600812
|
[]
|
NM
| false
| 166
| 0
|
[0, 0]
| 0
| 0.000001
| 0
| 0.000001
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1219711.cif
| false
| null |
data/final/MP/graphs/Pt0.5W0.5-MP-mp-1219711.json
| 0
| true
|
-3m
| 0
| 0
| 0
| 0
| 0
| 0
| 6
| 1
| 0
| 0
| 0
| 1
| false
|
Ba2Cu3Ho1O7
| 1
| 0
| 1
| true
|
Ba2Cu3Ho1O7
|
Ba2Cu3Ho1O7
| 92.475
|
Cuprate
| true
|
Ba15.385Cu23.077Ho7.692O53.84615384615385
|
Ba-Cu-Ho-O
| 4
|
Supercon
|
Ho1Ba2Cu3O7
|
MP-mp-6616
|
Ba2Ho1Cu3O7
|
Ba-Cu-Ho-O
|
Ba15.385Cu23.077Ho7.692O53.84615384615385
|
P m m m
|
orthorhombic
| 3.836729
| 3.919335
| 11.791186
|
data/final/MP/cifs/Ba2Cu3Ho1O7-MP-mp-6616.cif
|
data/source/MP/raw/cifs/mp-6616.cif
|
mp-6616
| 0
| null |
2011-05-15 07:21:38
| 6.951038
|
10.17188/1281393
|
@misc{osti_1281393,
author = "Persson, Kristin",
title = "Materials Data on Ba2HoCu3O7 (SG:47) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1281393",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1702487'}}
| 0.031852
| 3.24846
| 520
| -79.032084
| -6.079391
|
{'tags': ['Holmium dibarium dicopper copper(III) oxide', 'Holmium dibarium tricopper heptaoxide']}
| -79.032084
| -6.079391
| -2.191337
|
['bandstructure']
| true
|
[81174, 68044]
| true
|
2021-05-12 10:58:51.532000
|
NM
| 13
| 8
|
mp-6616
|
oxide
|
Ba2HoCu3O7
|
{'functional': 'PBE', 'labels': ['Ba_sv', 'Ho_3', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'Ba': 2.0, 'Ho': 1.0, 'Cu': 3.0, 'O': 7.0}
|
GGA
|
mp-6616
|
['mp-922636', 'mp-923410', 'mp-908210', 'mp-6616', 'mp-1475744', 'mp-1702487', 'mp-1831544', 'mp-1602206']
| 0.000595
|
{'Ba': 2.0, 'Ho': 1.0, 'Cu': 3.0, 'O': 7.0}
| 177.30909
|
[]
|
NM
| false
| 47
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000003
| 0.000595
| 0
| 0.000595
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-6616.cif
| false
| null |
data/final/MP/graphs/Ba2Cu3Ho1O7-MP-mp-6616.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ba0.635Bi1K0.365O3
| 2
| 0.012667
| 3
| false
|
Ba1.905Bi3K1.095O9
|
Ba2Bi3K1O9
| 30.4
|
Oxide
| true
|
Ba12.7Bi20K7.3O60
|
Ba-Bi-K-O
| 4
|
Supercon
|
Ba0.635K0.365Bi1O3
|
MP-mp-1223518
|
K1Ba2Bi3O9
|
Ba-Bi-K-O
|
Ba13.333Bi20K6.667O60
|
P -3 m 1
|
trigonal
| 6.187564
| 6.187564
| 7.581401
|
data/final/MP/cifs/Ba0.635Bi1K0.365O3-MP-mp-1223518-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1223518.cif
|
mp-1223518
| 0
| null |
2019-01-12 23:54:06.965000
| 7.165301
| null | null |
{'GGA': {'task_id': 'mp-1729135'}}
| 0.001552
| 3.46143
| 520
| -85.222714
| -5.681514
|
{'tags': []}
| -85.222714
| -5.681514
| -2.017041
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:52.054000
|
NM
| 15
| 4
|
mp-1223518
|
oxide
|
KBa2(BiO3)3
|
{'functional': 'PBE', 'labels': ['K_sv', 'Ba_sv', 'Bi', 'O'], 'pot_type': 'paw'}
|
{'K': 1.0, 'Ba': 2.0, 'Bi': 3.0, 'O': 9.0}
|
GGA
|
mp-1223518
|
['mp-1223518', 'mp-1391182', 'mp-1729135', 'mp-1775199']
| 0.00005
|
{'K': 1.0, 'Ba': 2.0, 'Bi': 3.0, 'O': 9.0}
| 251.373527
|
[]
|
NM
| false
| 164
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0
| 0.00005
| 0
| 0.00005
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1223518.cif
| true
| null |
data/final/MP/graphs/Ba0.635Bi1K0.365O3-MP-mp-1223518-synth_doped.json
| 0
| true
|
-3m
| 0
| 0
| 0
| 0
| 0
| 0
| 6
| 1
| 0
| 0
| 0
| 1
| false
|
As1Ce1F0.16Fe1O0.84
| 3
| 0.08
| 2
| false
|
As2Ce2F0.32Fe2O1.68
|
As2Ce2Fe2O2
| 40.85
|
Ferrite
| true
|
As25Ce25F4Fe25O21
|
As-Ce-F-Fe-O
| 5
|
Supercon
|
Ce1Fe1As1F0.16O0.84
|
MP-mp-605060
|
Ce2Fe2As2O2
|
As-Ce-Fe-O
|
As25Ce25Fe25O25
|
P 4 m m
|
tetragonal
| 3.992256
| 3.992256
| 9.041971
|
data/final/MP/cifs/As1Ce1F0.16Fe1O0.84-MP-mp-605060-synth_doped.cif
|
data/source/MP/raw/cifs/mp-605060.cif
|
mp-605060
| 0
| null |
2014-02-14 20:12:08
| 6.611234
|
10.17188/1277425
|
@misc{osti_1277425,
author = "Persson, Kristin",
title = "Materials Data on CeFeAsO (SG:99) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1277425",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA+U': {'task_id': 'mp-1751604'}}
| 0.207258
| 6.302884
| 520
| -55.742716
| -6.967839
|
{'tags': []}
| -55.742716
| -6.967839
| -1.701045
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:51.532000
|
FiM
| 8
| 10
|
mp-605060
|
oxide
|
CeFeAsO
|
{'functional': 'PBE', 'labels': ['Ce', 'Fe_pv', 'As', 'O'], 'pot_type': 'paw'}
|
{'Ce': 1.0, 'Fe': 1.0, 'As': 1.0, 'O': 1.0}
|
GGA+U
|
mp-605060
|
['mp-605060', 'mp-917114', 'mp-918266', 'mp-919274', 'mp-1443189', 'mp-1751604', 'mp-1770633', 'mp-1779614', 'mp-1873964', 'mp-1622328']
| 2.999453
|
{'Ce': 2.0, 'Fe': 2.0, 'As': 2.0, 'O': 2.0}
| 144.11191
|
[]
|
FiM
| true
| 99
| 3
|
[-0.5, -0.5, 3.5, 3.5, 0.0, 0.0, 0.0, 0.0]
| 0.041627
| 2.999453
| 4
| 5.998907
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-605060.cif
| true
| null |
data/final/MP/graphs/As1Ce1F0.16Fe1O0.84-MP-mp-605060-synth_doped.json
| 0
| true
|
4mm
| 0
| 0
| 0
| 0
| 5
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Gd1Ru2
| 1
| 0
| 2
| false
|
Gd2Ru4
|
Gd2Ru4
| 0
|
Other
| true
|
Gd33.333Ru66.667
|
Gd-Ru
| 2
|
Supercon
|
Gd1Ru2
|
MP-mp-646926
|
Gd2Ru4
|
Gd-Ru
|
Gd33.333Ru66.667
|
F d -3 m
|
cubic
| 5.369017
| 5.369017
| 5.369017
|
data/final/MP/cifs/Gd1Ru2-MP-mp-646926.cif
|
data/source/MP/raw/cifs/mp-646926.cif
|
mp-646926
| 0
| null |
2014-02-24 13:37:21
| 10.90626
|
10.17188/1280660
|
@misc{osti_1280660,
author = "Persson, Kristin",
title = "Materials Data on GdRu2 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1280660",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1688626'}}
| 0
| 5.664192
| 520
| -66.789723
| -11.131621
|
{'tags': ['Gadolinium ruthenium (1/2)']}
| -66.789723
| -11.131621
| -0.256653
|
['xas', 'bandstructure']
| true
|
[106830]
| true
|
2021-05-12 10:57:32.679000
|
FiM
| 6
| 6
|
mp-646926
| null |
GdRu2
|
{'functional': 'PBE', 'labels': ['Gd', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Gd': 1.0, 'Ru': 2.0}
|
GGA
|
mp-646926
|
['mp-646926', 'mp-1300993', 'mp-1659202', 'mp-1688626', 'mp-1804665', 'mp-1589222']
| 6.623878
|
{'Gd': 2.0, 'Ru': 4.0}
| 109.438272
|
[]
|
FiM
| true
| 166
| 2
|
[7.0, 7.0, -0.2, -0.3, -0.3, -0.3]
| 0.121052
| 6.623878
| 6
| 13.247756
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-646926.cif
| false
| null |
data/final/MP/graphs/Gd1Ru2-MP-mp-646926.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Hf2Ru3Si4
| 1
| 0
| 4
| false
|
Hf8Ru12Si16
|
Hf8Ru12Si16
| 0
|
Other
| true
|
Hf22.222Ru33.333Si44.444
|
Hf-Ru-Si
| 3
|
Supercon
|
Hf2Ru3Si4
|
MP-mp-31022
|
Hf8Si16Ru12
|
Hf-Ru-Si
|
Hf22.222Ru33.333Si44.444
|
C 1 2/c 1
|
monoclinic
| 5.357558
| 9.87356
| 10.974775
|
data/final/MP/cifs/Hf2Ru3Si4-MP-mp-31022.cif
|
data/source/MP/raw/cifs/mp-31022.cif
|
mp-31022
| 0
| null |
2014-02-21 05:16:21
| 9.55042
|
10.17188/1205354
|
@misc{osti_1205354,
author = "Persson, Kristin",
title = "Materials Data on Hf2Si4Ru3 (SG:15) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1205354",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1736740'}}
| 0.006915
| 8.810562
| 520
| -308.045812
| -8.556828
|
{'tags': ['Hafnium ruthenium silicide (2/3/4)']}
| -308.045812
| -8.556828
| -0.80985
|
['xas', 'bandstructure']
| true
|
[60071]
| true
|
2021-05-12 10:57:04.957000
|
NM
| 36
| 8
|
mp-31022
| null |
Hf2Si4Ru3
|
{'functional': 'PBE', 'labels': ['Hf_pv', 'Si', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Hf': 2.0, 'Si': 4.0, 'Ru': 3.0}
|
GGA
|
mp-31022
|
['mp-943288', 'mp-942231', 'mp-933023', 'mp-31022', 'mp-1144740', 'mp-1400101', 'mp-1736740', 'mp-1869729']
| 0.000201
|
{'Hf': 8.0, 'Si': 16.0, 'Ru': 12.0}
| 537.283
|
[]
|
NM
| false
| 15
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000001
| 0.000201
| 0
| 0.000806
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-31022.cif
| false
| null |
data/final/MP/graphs/Hf2Ru3Si4-MP-mp-31022.json
| 0
| true
|
2/m
| 0
| 0
| 3
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Ce1Pt3Si1
| 1
| 0
| 1
| true
|
Ce1Pt3Si1
|
Ce1Pt3Si1
| 0.669222
|
Heavy_fermion
| true
|
Ce20Pt60Si20
|
Ce-Pt-Si
| 3
|
Supercon
|
Ce1Pt3Si1
|
MP-mp-1207119
|
Ce1Si1Pt3
|
Ce-Pt-Si
|
Ce20Pt60Si20
|
P 4 m m
|
tetragonal
| 4.067884
| 4.067884
| 5.552623
|
data/final/MP/cifs/Ce1Pt3Si1-MP-mp-1207119.cif
|
data/source/MP/raw/cifs/mp-1207119.cif
|
mp-1207119
| 0
| null |
2019-01-12 10:17:34.047000
| 13.616649
| null | null | null | 0
| 7.991878
| 520
| -34.846669
| -6.969334
|
{'tags': ['CePt3Si', 'CePt3B']}
| -34.846669
| -6.969334
| -1.040909
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:19.396000
|
NM
| 5
| 2
|
mp-1207119
| null |
CeSiPt3
|
{'functional': 'PBE', 'labels': ['Ce', 'Si', 'Pt'], 'pot_type': 'paw'}
|
{'Ce': 1.0, 'Si': 1.0, 'Pt': 3.0}
|
GGA
|
mp-1207119
|
['mp-1207119', 'mp-1923489']
| 0.009918
|
{'Ce': 1.0, 'Si': 1.0, 'Pt': 3.0}
| 91.88303
|
[]
|
NM
| false
| 99
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0]
| 0.000108
| 0.009918
| 0
| 0.009918
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1207119.cif
| false
| null |
data/final/MP/graphs/Ce1Pt3Si1-MP-mp-1207119.json
| 0
| true
|
4mm
| 0
| 0
| 0
| 0
| 5
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Nd0.2Ru2Th0.8
| 3
| 0.133333
| 2
| false
|
Nd0.4Ru4Th1.6
|
Ru4Th2
| 4.55
|
Other
| true
|
Nd6.667Ru66.667Th26.667
|
Nd-Ru-Th
| 3
|
Supercon
|
Th0.8Nd0.2Ru2
|
MP-mp-574438
|
Th2Ru4
|
Ru-Th
|
Ru66.667Th33.333
|
F d -3 m
|
cubic
| 5.433971
| 5.433971
| 5.433971
|
data/final/MP/cifs/Nd0.2Ru2Th0.8-MP-mp-574438-synth_doped.cif
|
data/source/MP/raw/cifs/mp-574438.cif
|
mp-574438
| 0
| null |
2014-02-28 05:45:15
| 12.708958
|
10.17188/1276579
|
@misc{osti_1276579,
author = "Persson, Kristin",
title = "Materials Data on ThRu2 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1276579",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-918592'}}
| 0.038487
| 8.285897
| 520
| -53.838971
| -8.973162
|
{'tags': ['Ruthenium thorium (2/1)', 'Thorium ruthenium (1/2)']}
| -53.838971
| -8.973162
| -0.318949
|
['xas', 'elasticity', 'bandstructure']
| true
|
[650730, 150740, 106002, 650723, 650729, 650731, 106003]
| true
|
2021-05-12 10:56:27.046000
|
NM
| 6
| 7
|
mp-574438
| null |
ThRu2
|
{'functional': 'PBE', 'labels': ['Th', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Th': 1.0, 'Ru': 2.0}
|
GGA
|
mp-574438
|
['mp-919588', 'mp-905408', 'mp-918592', 'mp-574438', 'mp-1439663', 'mp-1802924', 'mp-1592175']
| 0.000575
|
{'Th': 2.0, 'Ru': 4.0}
| 113.4585
|
[]
|
NM
| false
| 166
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, -0.0]
| 0.00001
| 0.000575
| 0
| 0.001151
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-574438.cif
| true
| null |
data/final/MP/graphs/Nd0.2Ru2Th0.8-MP-mp-574438-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Cu1.2Rh1.8S4
| 3
| 0.057143
| 2
| false
|
Cu2.4Rh3.6S8
|
Cu2Rh4S8
| 5.08
|
Other
| true
|
Cu17.143Rh25.714S57.143
|
Cu-Rh-S
| 3
|
Supercon
|
Cu1.2Rh1.8S4
|
MP-mp-15613
|
Cu2Rh4S8
|
Cu-Rh-S
|
Cu14.286Rh28.571S57.143
|
F d -3 m
|
cubic
| 6.987438
| 6.987438
| 6.987438
|
data/final/MP/cifs/Cu1.2Rh1.8S4-MP-mp-15613-synth_doped.cif
|
data/source/MP/raw/cifs/mp-15613.cif
|
mp-15613
| 0
| null |
2011-06-05 06:28:04
| 5.474004
|
10.17188/1191271
|
@misc{osti_1191271,
author = "Persson, Kristin",
title = "Materials Data on Cu(RhS2)2 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1191271",
place = "United States",
year = "2015",
month = "3",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1676515'}}
| 0
| 5.288849
| 520
| -76.758795
| -5.482771
|
{'tags': ['Copper rhodium sulfide (1/2/4)', 'Copper dirhodium sulfide', 'Cuprorhodsite']}
| -76.758795
| -5.482771
| -0.716825
|
['xas', 'bandstructure']
| true
|
[628767, 41900]
| true
|
2021-05-12 10:56:53.126000
|
NM
| 14
| 8
|
mp-15613
| null |
Cu(RhS2)2
|
{'functional': 'PBE', 'labels': ['Cu_pv', 'Rh_pv', 'S'], 'pot_type': 'paw'}
|
{'Cu': 1.0, 'Rh': 2.0, 'S': 4.0}
|
GGA
|
mp-15613
|
['mp-920968', 'mp-942816', 'mp-942447', 'mp-15613', 'mp-1475540', 'mp-1676515', 'mp-1774816', 'mp-1603317']
| 0.008336
|
{'Cu': 2.0, 'Rh': 4.0, 'S': 8.0}
| 241.234245
|
[]
|
NM
| false
| 227
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.000069
| 0.008336
| 0
| 0.016672
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-15613.cif
| true
| null |
data/final/MP/graphs/Cu1.2Rh1.8S4-MP-mp-15613-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
H3.63Th1
| 3
| 0.068035
| 0.826223
| true
|
H3Th0.826
|
H3Th1
| 8.35
|
Other
| true
|
H78.402Th21.598
|
H-Th
| 2
|
Supercon
|
H3.63Th1
|
MP-mp-861653
|
Th1H3
|
H-Th
|
H75Th25
|
I 4/m m m
|
tetragonal
| 3.526436
| 3.526436
| 4.128162
|
data/final/MP/cifs/H3.63Th1-MP-mp-861653-synth_doped.cif
|
data/source/MP/raw/cifs/mp-861653.cif
|
mp-861653
| 0
| null |
2014-08-22 13:34:37
| 9.540443
|
10.17188/1309247
|
@misc{osti_1309247,
author = "Persson, Kristin",
title = "Materials Data on ThH3 (SG:139) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1309247",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1766008'}}
| 0.049082
| 7.122476
| 520
| -19.260845
| -4.815211
|
{'tags': []}
| -19.260845
| -4.815211
| -0.551452
|
['bandstructure', 'elasticity']
| true
|
[]
| true
|
2021-05-12 10:56:31.128000
|
NM
| 4
| 11
|
mp-861653
| null |
ThH3
|
{'functional': 'PBE', 'labels': ['Th', 'H'], 'pot_type': 'paw'}
|
{'Th': 1.0, 'H': 3.0}
|
GGA
|
mp-861653
|
['mp-861653', 'mp-1002788', 'mp-1004363', 'mp-1049481', 'mp-1049496', 'mp-1417433', 'mp-1766008', 'mp-1790587', 'mp-1010066', 'mp-1611510', 'mp-1049488']
| 0.001335
|
{'Th': 1.0, 'H': 3.0}
| 40.913135
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0]
| 0.000033
| 0.001335
| 0
| 0.001335
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-861653.cif
| true
| null |
data/final/MP/graphs/H3.63Th1-MP-mp-861653-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Gd0.064La0.936Sn3
| 2
| 0.032
| 1
| true
|
Gd0.064La0.936Sn3
|
La1Sn3
| 3.76
|
Other
| true
|
Gd1.6La23.4Sn75
|
Gd-La-Sn
| 3
|
Supercon
|
La0.936Gd0.064Sn3
|
MP-mp-633
|
La1Sn3
|
La-Sn
|
La25Sn75
|
P m -3 m
|
cubic
| 4.820061
| 4.820061
| 4.820061
|
data/final/MP/cifs/Gd0.064La0.936Sn3-MP-mp-633-synth_doped.cif
|
data/source/MP/raw/cifs/mp-633.cif
|
mp-633
| 0
| null |
2011-05-13 04:30:54
| 7.340537
|
10.17188/1279358
|
@misc{osti_1279358,
author = "Persson, Kristin",
title = "Materials Data on LaSn3 (SG:221) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1279358",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1688008'}}
| 0
| 8.68748
| 520
| -19.264824
| -4.816206
|
{'tags': ['Lanthanum stannide (1/3)', 'Lanthanum tin (1/3)']}
| -19.264824
| -4.816206
| -0.575025
|
['xas', 'bandstructure']
| true
|
[641991, 104721, 641986, 261870, 104720, 151359, 642000, 641998, 191074]
| true
|
2021-05-12 10:57:30.779000
|
NM
| 4
| 12
|
mp-633
| null |
LaSn3
|
{'functional': 'PBE', 'labels': ['La', 'Sn_d'], 'pot_type': 'paw'}
|
{'La': 1.0, 'Sn': 3.0}
|
GGA
|
mp-633
|
['mp-991111', 'mp-993073', 'mp-633', 'mp-1066557', 'mp-1066573', 'mp-1066594', 'mp-1442023', 'mp-1688008', 'mp-1787436', 'mp-994393', 'mp-1590336', 'mp-1066601']
| 0.005556
|
{'La': 1.0, 'Sn': 3.0}
| 111.98442
|
[]
|
NM
| false
| 221
| 0
|
[0, 0, 0, 0]
| 0.00005
| 0.005556
| 0
| 0.005556
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-633.cif
| true
| null |
data/final/MP/graphs/Gd0.064La0.936Sn3-MP-mp-633-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ce0.95La0.05Ru2
| 2
| 0.033333
| 2
| false
|
Ce1.9La0.1Ru4
|
Ce2Ru4
| 7.181
|
Heavy_fermion
| true
|
Ce31.667La1.667Ru66.667
|
Ce-La-Ru
| 3
|
Supercon
|
La0.05Ce0.95Ru2
|
MP-mp-607
|
Ce2Ru4
|
Ce-Ru
|
Ce33.333Ru66.667
|
F d -3 m
|
cubic
| 5.359031
| 5.359031
| 5.359031
|
data/final/MP/cifs/Ce0.95La0.05Ru2-MP-mp-607-synth_doped.cif
|
data/source/MP/raw/cifs/mp-607.cif
|
mp-607
| 0
| null |
2011-05-13 22:34:26
| 10.44447
|
10.17188/1277529
|
@misc{osti_1277529,
author = "Persson, Kristin",
title = "Materials Data on CeRu2 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1277529",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1686879'}}
| 0
| 8.614192
| 520
| -50.664136
| -8.444023
|
{'tags': ['Cerium ruthenium (1/2)', 'Cerium ruthenium hydride (1/2/4)']}
| -50.664136
| -8.444023
| -0.2834
|
['xas', 'elasticity', 'bandstructure']
| true
|
[621326, 656077, 621978, 621973, 621980, 621984, 102277, 621972, 621976, 621979, 604113, 621977, 621982, 621983, 102276, 656078]
| true
|
2021-05-12 10:56:27.046000
|
NM
| 6
| 14
|
mp-607
| null |
CeRu2
|
{'functional': 'PBE', 'labels': ['Ce', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Ce': 1.0, 'Ru': 2.0}
|
GGA
|
mp-607
|
['mp-928203', 'mp-912221', 'mp-928809', 'mp-607', 'mp-1071462', 'mp-1071593', 'mp-1071613', 'mp-1077792', 'mp-1440763', 'mp-1686879', 'mp-1803198', 'mp-1591928', 'mp-1591642', 'mp-1071635']
| 0.00001
|
{'Ce': 2.0, 'Ru': 4.0}
| 108.828779
|
[]
|
NM
| false
| 227
| 0
|
[0, 0, 0, 0, 0, 0]
| 0
| 0.00001
| 0
| 0.00002
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-607.cif
| true
| null |
data/final/MP/graphs/Ce0.95La0.05Ru2-MP-mp-607-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Ba0.85K0.15Sb2Ti2O1
| 2
| 0.05
| 1
| true
|
Ba0.85K0.15Sb2Ti2O1
|
Ba1Sb2Ti2O1
| 5.86
|
Oxide
| true
|
Ba14.167K2.5Sb33.333Ti33.333O16.666666666666668
|
Ba-K-Sb-Ti-O
| 5
|
Supercon
|
Ba0.85K0.15Ti2Sb2O1
|
MP-mp-1070806
|
Ba1Ti2Sb2O1
|
Ba-Sb-Ti-O
|
Ba16.667Sb33.333Ti33.333O16.666666666666668
|
P 4/m m m
|
tetragonal
| 4.113474
| 4.113474
| 8.312382
|
data/final/MP/cifs/Ba0.85K0.15Sb2Ti2O1-MP-mp-1070806-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1070806.cif
|
mp-1070806
| 0
| null |
2018-03-22 04:02:04
| 5.815449
| null | null |
{'GGA': {'task_id': 'mp-1702174'}}
| 0
| 5.897515
| 520
| -39.149326
| -6.524888
|
{'tags': []}
| -39.149326
| -6.524888
| -1.550735
|
['bandstructure']
| true
|
[430061, 237789, 430060]
| true
|
2021-05-12 10:58:14.654000
|
NM
| 6
| 16
|
mp-1070806
|
oxide
|
BaTi2Sb2O
|
{'functional': 'PBE', 'labels': ['Ba_sv', 'Ti_pv', 'Sb', 'O'], 'pot_type': 'paw'}
|
{'Ba': 1.0, 'Ti': 2.0, 'Sb': 2.0, 'O': 1.0}
|
GGA
|
mp-1070806
|
['mp-1071055', 'mp-1071068', 'mp-1071083', 'mp-1071088', 'mp-1070806', 'mp-1071124', 'mp-1070846', 'mp-1070900', 'mp-1071137', 'mp-1423542', 'mp-1702174', 'mp-1785425', 'mp-1588663', 'mp-1070899', 'mp-1071129', 'mp-1071119']
| 0.001055
|
{'Ba': 1.0, 'Ti': 2.0, 'Sb': 2.0, 'O': 1.0}
| 140.651059
|
[]
|
NM
| false
| 123
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000008
| 0.001055
| 0
| 0.001055
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1070806.cif
| true
| null |
data/final/MP/graphs/Ba0.85K0.15Sb2Ti2O1-MP-mp-1070806-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B1.88C0.12Mg1
| 3
| 0.08
| 1
| true
|
B1.88C0.12Mg1
|
B2Mg1
| 32.9
|
Other
| true
|
B62.667C4Mg33.333
|
B-C-Mg
| 3
|
Supercon
|
Mg1B1.88C0.12
|
MP-mp-763
|
Mg1B2
|
B-Mg
|
B66.667Mg33.333
|
P 6/m m m
|
hexagonal
| 3.07368
| 3.07368
| 3.53435
|
data/final/MP/cifs/B1.88C0.12Mg1-MP-mp-763-synth_doped.cif
|
data/source/MP/raw/cifs/mp-763.cif
|
mp-763
| 0
| null |
2011-05-12 17:25:30
| 2.637301
| null | null |
{'GGA': {'task_id': 'mp-1671065'}}
| 0
| 5.985521
| 520
| -15.350083
| -5.116694
|
{'tags': ['Mgnesium boride (1/2)', 'Magnesium boride (1/2)', 'Magnesium boride (1/1)', 'High pressure experimental phase', 'Magensium diboride']}
| -15.350083
| -5.116694
| -0.13034
|
['bandstructure', 'elasticity']
| true
|
[193379, 186389, 94257, 237010, 181869, 96704, 96705, 248441, 96906, 150598, 92831, 155349, 181870, 94256, 182537, 236951, 108064, 93925, 186763, 26675, 248442, 96703, 155347, 153657, 191393, 96706, 92832, 94255, 155348]
| true
|
2021-05-12 10:56:29.056000
|
NM
| 3
| 39
|
mp-763
| null |
MgB2
|
{'functional': 'PBE', 'labels': ['Mg_pv', 'B'], 'pot_type': 'paw'}
|
{'Mg': 1.0, 'B': 2.0}
|
GGA
|
mp-763
|
['mp-905361', 'mp-919554', 'mp-918565', 'mp-763', 'mp-1061708', 'mp-1061762', 'mp-1061948', 'mp-1061909', 'mp-1061934', 'mp-1062061', 'mp-1061740', 'mp-1062105', 'mp-1062081', 'mp-1062570', 'mp-1062589', 'mp-1062612', 'mp-1062861', 'mp-1062883', 'mp-1062892', 'mp-1062941', 'mp-1062925', 'mp-1062999', 'mp-1063048', 'mp-1063024', 'mp-1062914', 'mp-1063249', 'mp-1063291', 'mp-1063269', 'mp-1440873', 'mp-1671065', 'mp-1791068', 'mp-1062931', 'mp-1063035', 'mp-1061942', 'mp-1062096', 'mp-1062604', 'mp-1061753', 'mp-1062912', 'mp-1063282']
| 0.000248
|
{'Mg': 1.0, 'B': 2.0}
| 28.917284
|
[]
|
NM
| false
| 191
| 0
|
[0, 0, 0]
| 0.000009
| 0.000248
| 0
| 0.000248
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-763.cif
| true
| null |
data/final/MP/graphs/B1.88C0.12Mg1-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B4Nd1Ru4
| 1
| 0
| 4
| false
|
B16Nd4Ru16
|
B16Nd4Ru16
| 0
|
Other
| true
|
B44.444Nd11.111Ru44.444
|
B-Nd-Ru
| 3
|
Supercon
|
Nd1Ru4B4
|
MP-mp-1198170
|
Nd4B16Ru16
|
B-Nd-Ru
|
B44.444Nd11.111Ru44.444
|
I 41/a c d
|
tetragonal
| 7.5667
| 7.5667
| 9.266274
|
data/final/MP/cifs/B4Nd1Ru4-MP-mp-1198170.cif
|
data/source/MP/raw/cifs/mp-1198170.cif
|
mp-1198170
| 0
| null |
2019-01-12 03:00:19.181000
| 9.074237
| null | null |
{'GGA': {'task_id': 'mp-1751362'}}
| 0
| 6.90611
| 520
| -290.583836
| -8.071773
|
{'tags': ['Neodymium ruthenium boride (1/4/4)']}
| -290.583836
| -8.071773
| -0.45141
|
['bandstructure']
| true
|
[614967, 421310]
| true
|
2021-05-12 10:58:37.524000
|
NM
| 36
| 6
|
mp-1198170
| null |
Nd(BRu)4
|
{'functional': 'PBE', 'labels': ['Nd_3', 'B', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Nd': 1.0, 'B': 4.0, 'Ru': 4.0}
|
GGA
|
mp-1198170
|
['mp-1198170', 'mp-1198952', 'mp-1444137', 'mp-1751362', 'mp-1820483', 'mp-1622934']
| 0.001266
|
{'Nd': 4.0, 'B': 16.0, 'Ru': 16.0}
| 433.160655
|
[]
|
NM
| false
| 142
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000012
| 0.001266
| 0
| 0.005062
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1198170.cif
| false
| null |
data/final/MP/graphs/B4Nd1Ru4-MP-mp-1198170.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Li1.1Ti1.9O4
| 2
| 0.028571
| 2
| false
|
Li2.2Ti3.8O8
|
Li2Ti4O8
| 10.05
|
Oxide
| true
|
Li15.714Ti27.143O57.142857142857146
|
Li-Ti-O
| 3
|
Supercon
|
Li1.1Ti1.9O4
|
MP-mp-5670
|
Li2Ti4O8
|
Li-Ti-O
|
Li14.286Ti28.571O57.142857142857146
|
F d -3 m
|
cubic
| 5.986032
| 5.986032
| 5.986032
|
data/final/MP/cifs/Li1.1Ti1.9O4-MP-mp-5670-synth_doped.cif
|
data/source/MP/raw/cifs/mp-5670.cif
|
mp-5670
| 0
| null |
2011-05-14 11:10:22
| 3.649565
|
10.17188/1273637
|
@misc{osti_1273637,
author = "Persson, Kristin",
title = "Materials Data on LiTi2O4 (SG:227) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1273637",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1699404'}}
| 0
| 5.031168
| 520
| -114.934447
| -8.209603
|
{'tags': ['Lithium titanium oxide (1/2/4)', 'Lithium titanium(III) titanium(IV) oxide', 'Lithium titanium(III) titanium oxide', 'Lithium titanium titanium(III) oxide', 'Lithium titano(III)titanate', 'Spinel-(Li,Ti)']}
| -114.934447
| -8.209603
| -3.24621
|
['bandstructure', 'elasticity']
| true
|
[72859, 78482, 154982, 81329, 15789, 48127]
| true
|
2021-05-12 10:56:22.739000
|
NM
| 14
| 7
|
mp-5670
|
oxide
|
LiTi2O4
|
{'functional': 'PBE', 'labels': ['Li_sv', 'Ti_pv', 'O'], 'pot_type': 'paw'}
|
{'Li': 1.0, 'Ti': 2.0, 'O': 4.0}
|
GGA
|
mp-5670
|
['mp-923613', 'mp-922835', 'mp-908534', 'mp-5670', 'mp-1418091', 'mp-1699404', 'mp-1787951']
| 0.052108
|
{'Li': 2.0, 'Ti': 4.0, 'O': 8.0}
| 151.670864
|
[]
|
NM
| false
| 227
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000687
| 0.052108
| 0
| 0.104216
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-5670.cif
| true
| null |
data/final/MP/graphs/Li1.1Ti1.9O4-MP-mp-5670-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
C1Pb1Ti2
| 1
| 0
| 2
| false
|
C2Pb2Ti4
|
C2Pb2Ti4
| 0
|
Other
| true
|
C25Pb25Ti50
|
C-Pb-Ti
| 3
|
Supercon
|
C1Pb1Ti2
|
MP-mp-20661
|
Ti4Pb2C2
|
C-Pb-Ti
|
C25Pb25Ti50
|
P 63/m m c
|
hexagonal
| 3.226602
| 3.226603
| 14.060364
|
data/final/MP/cifs/C1Pb1Ti2-MP-mp-20661.cif
|
data/source/MP/raw/cifs/mp-20661.cif
|
mp-20661
| 0
| null |
2014-12-22 15:50:36
| 8.250785
|
10.17188/1195790
|
@misc{osti_1195790,
author = "Persson, Kristin",
title = "Materials Data on Ti2PbC (SG:194) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1195790",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1701863'}}
| 0
| 8.066973
| 520
| -62.009611
| -7.751201
|
{'tags': ['Titanium lead carbide (2/1/1)']}
| -62.009611
| -7.751201
| -0.568598
|
['xas', 'elasticity', 'bandstructure']
| true
|
[42926]
| true
|
2021-05-12 10:56:14.760000
|
NM
| 8
| 8
|
mp-20661
| null |
Ti2PbC
|
{'functional': 'PBE', 'labels': ['Ti_pv', 'Pb_d', 'C'], 'pot_type': 'paw'}
|
{'Ti': 2.0, 'Pb': 1.0, 'C': 1.0}
|
GGA
|
mp-20661
|
['mp-909903', 'mp-925463', 'mp-20661', 'mp-1422083', 'mp-1701863', 'mp-1790408', 'mp-925873', 'mp-1587924']
| 0.002707
|
{'Ti': 4.0, 'Pb': 2.0, 'C': 2.0}
| 126.77047
|
[]
|
NM
| false
| 194
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0]
| 0.000043
| 0.002707
| 0
| 0.005415
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-20661.cif
| false
| null |
data/final/MP/graphs/C1Pb1Ti2-MP-mp-20661.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Pb0.986Te1Tl0.014
| 2
| 0.014
| 1
| true
|
Pb0.986Te1Tl0.014
|
Pb1Te1
| 1.38
|
Other
| true
|
Pb49.3Te50Tl0.7
|
Pb-Te-Tl
| 3
|
Supercon
|
Pb0.986Tl0.014Te1
|
MP-mp-19717
|
Te1Pb1
|
Pb-Te
|
Pb50Te50
|
F m -3 m
|
cubic
| 4.642633
| 4.642633
| 4.642633
|
data/final/MP/cifs/Pb0.986Te1Tl0.014-MP-mp-19717-synth_doped.cif
|
data/source/MP/raw/cifs/mp-19717.cif
|
mp-19717
| 1.0582
| null |
2013-09-21 09:56:54
| 7.856997
|
10.17188/1194927
|
@misc{osti_1194927,
author = "Persson, Kristin",
title = "Materials Data on TePb (SG:225) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1194927",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1686920'}}
| 0
| 4.973521
| 520
| -7.667439
| -3.83372
|
{'tags': ['Altaite', 'Lead telluride (1/1)', 'High pressure experimental phase', 'Lead telluride']}
| -7.667439
| -3.83372
| -0.616746
|
['eos', 'xas', 'bandstructure', 'diel', 'phonons', 'elasticity']
| true
|
[194220, 648583, 648588, 648607, 63099, 648584, 648590, 604178, 648595, 96500, 648608, 648596, 648597, 182660, 648599, 648593, 648603, 96504, 648591, 648586, 96506, 600843, 600522, 648614, 182662, 648606, 186788, 96505, 153711, 648581, 648605, 648587, 248494, 648585, 190437, 648600, 648617, 602956, 38295, 648589, 648615, 63098, 648592, 290707, 648612, 648594, 182661, 648616, 248495, 648613]
| true
|
2021-05-12 10:56:14.760000
|
NM
| 2
| 34
|
mp-19717
| null |
TePb
|
{'functional': 'PBE', 'labels': ['Te', 'Pb_d'], 'pot_type': 'paw'}
|
{'Te': 1.0, 'Pb': 1.0}
|
GGA
|
mp-19717
|
['mp-658057', 'mp-655294', 'mp-656827', 'mp-19717', 'mp-1056883', 'mp-1056867', 'mp-1056875', 'mp-1059285', 'mp-1059296', 'mp-1059300', 'mp-1059866', 'mp-1059872', 'mp-1059851', 'mp-1060231', 'mp-1060244', 'mp-1060254', 'mp-1061267', 'mp-1061381', 'mp-1061396', 'mp-1061412', 'mp-1061239', 'mp-1061250', 'mp-1142129', 'mp-1440755', 'mp-1686920', 'mp-1801248', 'mp-1594316', 'mp-1595339', 'mp-1059310', 'mp-1060260', 'mp-1061273', 'mp-1061416', 'mp-1056891', 'mp-1059878']
| 0.001484
|
{'Te': 1.0, 'Pb': 1.0}
| 70.758392
|
[]
|
NM
| false
| 225
| 0
|
[0, 0]
| 0.000021
| 0.001484
| 0
| 0.001484
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-19717.cif
| true
| null |
data/final/MP/graphs/Pb0.986Te1Tl0.014-MP-mp-19717-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Ir0.8Rh0.2
| 3
| 0.1
| 4
| false
|
Ir3.2Rh0.8
|
Ir3Rh1
| 0.03
|
Other
| true
|
Ir80Rh20
|
Ir-Rh
| 2
|
Supercon
|
Ir0.8Rh0.2
|
MP-mp-1184771
|
Ir3Rh1
|
Ir-Rh
|
Ir75Rh25
|
P m -3 m
|
cubic
| 3.869173
| 3.869173
| 3.869173
|
data/final/MP/cifs/Ir0.8Rh0.2-MP-mp-1184771-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1184771.cif
|
mp-1184771
| 0
| null |
2019-01-11 13:02:54.339000
| 19.481403
| null | null |
{'GGA': {'task_id': 'mp-1733856'}}
| 0.009459
| 9.119651
| 520
| -33.925887
| -8.481472
|
{'tags': []}
| -33.925887
| -8.481472
| -0.011572
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:27.755000
|
NM
| 4
| 5
|
mp-1184771
| null |
Ir3Rh
|
{'functional': 'PBE', 'labels': ['Ir', 'Rh_pv'], 'pot_type': 'paw'}
|
{'Ir': 3.0, 'Rh': 1.0}
|
GGA
|
mp-1184771
|
['mp-1184771', 'mp-1415898', 'mp-1733856', 'mp-1795000', 'mp-1618109']
| 0.000701
|
{'Ir': 3.0, 'Rh': 1.0}
| 57.923453
|
[]
|
NM
| false
| 221
| 0
|
[0, 0, 0, 0]
| 0.000012
| 0.000701
| 0
| 0.000701
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1184771.cif
| true
| null |
data/final/MP/graphs/Ir0.8Rh0.2-MP-mp-1184771-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ge3Pt1Sr1
| 1
| 0
| 1
| true
|
Ge3Pt1Sr1
|
Ge3Pt1Sr1
| 1
|
Other
| true
|
Ge60Pt20Sr20
|
Ge-Pt-Sr
| 3
|
Supercon
|
Sr1Pt1Ge3
|
MP-mp-1068239
|
Sr1Ge3Pt1
|
Ge-Pt-Sr
|
Ge60Pt20Sr20
|
I 4 m m
|
tetragonal
| 4.52679
| 4.52679
| 6.089297
|
data/final/MP/cifs/Ge3Pt1Sr1-MP-mp-1068239.cif
|
data/source/MP/raw/cifs/mp-1068239.cif
|
mp-1068239
| 0
| null |
2018-03-21 22:42:23
| 7.831418
| null | null |
{'GGA': {'task_id': 'mp-1704974'}}
| 0
| 4.36569
| 520
| -24.736331
| -4.947266
|
{'tags': ['Strontium platinum germanide (1/1/3)']}
| -24.736331
| -4.947266
| -0.621369
|
['bandstructure']
| true
|
[168863]
| true
|
2021-05-12 10:58:14.654000
|
NM
| 5
| 8
|
mp-1068239
| null |
SrGe3Pt
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Ge_d', 'Pt'], 'pot_type': 'paw'}
|
{'Sr': 1.0, 'Ge': 3.0, 'Pt': 1.0}
|
GGA
|
mp-1068239
|
['mp-1068355', 'mp-1068239', 'mp-1068295', 'mp-1428559', 'mp-1704974', 'mp-1924808', 'mp-1587710', 'mp-1068345']
| 0.000119
|
{'Sr': 1.0, 'Ge': 3.0, 'Pt': 1.0}
| 106.150086
|
[]
|
NM
| false
| 107
| 0
|
[0, 0, 0, 0, 0]
| 0.000001
| 0.000119
| 0
| 0.000119
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1068239.cif
| false
| null |
data/final/MP/graphs/Ge3Pt1Sr1-MP-mp-1068239.json
| 0
| true
|
4mm
| 0
| 0
| 0
| 0
| 5
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
B4Lu0.75Rh4Th0.25
| 3
| 0.055556
| 2
| false
|
B8Lu1.5Rh8Th0.5
|
B8Lu2Rh8
| 11.93
|
Other
| true
|
B44.444Lu8.333Rh44.444Th2.778
|
B-Lu-Rh-Th
| 4
|
Supercon
|
Lu0.75Th0.25Rh4B4
|
MP-mp-1188110
|
Lu2B8Rh8
|
B-Lu-Rh
|
B44.444Lu11.111Rh44.444
|
P 42/n m c
|
tetragonal
| 5.325657
| 5.325657
| 7.420215
|
data/final/MP/cifs/B4Lu0.75Rh4Th0.25-MP-mp-1188110-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1188110.cif
|
mp-1188110
| 0
| null |
2019-01-11 19:11:41.748000
| 9.938976
| null | null |
{'GGA': {'task_id': 'mp-1669462'}}
| 0.022432
| 6.832217
| 520
| -131.704992
| -7.316944
|
{'tags': ['Lutetium rhodium boride (1/4/4)']}
| -131.704992
| -7.316944
| -0.572972
|
['bandstructure']
| true
|
[601519, 614706]
| true
|
2021-05-12 10:58:31.620000
|
NM
| 18
| 6
|
mp-1188110
| null |
Lu(BRh)4
|
{'functional': 'PBE', 'labels': ['Lu_3', 'B', 'Rh_pv'], 'pot_type': 'paw'}
|
{'Lu': 1.0, 'B': 4.0, 'Rh': 4.0}
|
GGA
|
mp-1188110
|
['mp-1188110', 'mp-1188735', 'mp-1504954', 'mp-1669462', 'mp-1830476', 'mp-1597780']
| 0.000827
|
{'Lu': 2.0, 'B': 8.0, 'Rh': 8.0}
| 210.456757
|
[]
|
NM
| false
| 137
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000008
| 0.000827
| 0
| 0.001654
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1188110.cif
| true
| null |
data/final/MP/graphs/B4Lu0.75Rh4Th0.25-MP-mp-1188110-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
N0.97Sc1
| 2
| 0.015228
| 1
| true
|
N0.97Sc1
|
N1Sc1
| 0
|
Other
| true
|
N49.239Sc50.761
|
N-Sc
| 2
|
Supercon
|
N0.97Sc1
|
MP-mp-2857
|
Sc1N1
|
N-Sc
|
N50Sc50
|
F m -3 m
|
cubic
| 3.194928
| 3.194928
| 3.194928
|
data/final/MP/cifs/N0.97Sc1-MP-mp-2857-synth_doped.cif
|
data/source/MP/raw/cifs/mp-2857.cif
|
mp-2857
| 0.325
| null |
2011-05-12 17:49:06
| 4.245782
|
10.17188/1202670
|
@misc{osti_1202670,
author = "Persson, Kristin",
title = "Materials Data on ScN (SG:225) by Materials Project",
abstractNote = "Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations",
doi = "10.17188/1202670",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1688369'}}
| 0
| 5.464105
| 520
| -18.494454
| -9.247227
|
{'tags': ['Scandium nitride', 'Scandium nitride - B1 (LP)', 'Scandium nitride - B1(NP)', 'Scandium nitride (1/1)']}
| -18.494454
| -9.247227
| -2.093245
|
['xas', 'elasticity', 'bandstructure']
| true
|
[290470, 236800, 236799, 290709, 644668, 180829, 155049, 644666, 26948, 644667, 157501]
| true
|
2021-05-12 10:56:18.721000
|
NM
| 2
| 25
|
mp-2857
| null |
ScN
|
{'functional': 'PBE', 'labels': ['Sc_sv', 'N'], 'pot_type': 'paw'}
|
{'Sc': 1.0, 'N': 1.0}
|
GGA
|
mp-2857
|
['mp-905831', 'mp-918802', 'mp-919788', 'mp-2857', 'mp-1057143', 'mp-1057113', 'mp-1057124', 'mp-1057375', 'mp-1057403', 'mp-1057387', 'mp-1057969', 'mp-1057923', 'mp-1057941', 'mp-1058953', 'mp-1058990', 'mp-1058937', 'mp-1440773', 'mp-1688369', 'mp-1793214', 'mp-1595747', 'mp-1587388', 'mp-1058981', 'mp-1057960', 'mp-1057406', 'mp-1057140']
| 0.0001
|
{'Sc': 1.0, 'N': 1.0}
| 23.060466
|
[]
|
NM
| false
| 225
| 0
|
[0, 0]
| 0.000004
| 0.0001
| 0
| 0.0001
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-2857.cif
| true
| null |
data/final/MP/graphs/N0.97Sc1-MP-mp-2857-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Bi1Er1Pd1
| 1
| 0
| 1
| true
|
Bi1Er1Pd1
|
Bi1Er1Pd1
| 1.24
|
Other
| true
|
Bi33.333Er33.333Pd33.333
|
Bi-Er-Pd
| 3
|
Supercon
|
Er1Pd1Bi1
|
MP-mp-1206953
|
Er1Bi1Pd1
|
Bi-Er-Pd
|
Bi33.333Er33.333Pd33.333
|
F -4 3 m
|
cubic
| 4.733632
| 4.733632
| 4.733632
|
data/final/MP/cifs/Bi1Er1Pd1-MP-mp-1206953.cif
|
data/source/MP/raw/cifs/mp-1206953.cif
|
mp-1206953
| 0
| null |
2019-01-12 10:09:37.533000
| 10.686156
| null | null |
{'GGA': {'task_id': 'mp-1765996'}}
| 0
| 5.473264
| 520
| -16.410082
| -5.470027
|
{'tags': ['MgAgAs', 'ErPdBi']}
| -16.410082
| -5.470027
| -0.924149
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:39.488000
|
NM
| 3
| 5
|
mp-1206953
| null |
ErBiPd
|
{'functional': 'PBE', 'labels': ['Er_3', 'Bi', 'Pd'], 'pot_type': 'paw'}
|
{'Er': 1.0, 'Bi': 1.0, 'Pd': 1.0}
|
GGA
|
mp-1206953
|
['mp-1206953', 'mp-1418391', 'mp-1765996', 'mp-1801263', 'mp-1611095']
| 0.000906
|
{'Er': 1.0, 'Bi': 1.0, 'Pd': 1.0}
| 75.001227
|
[]
|
NM
| false
| 216
| 0
|
[0, 0, 0]
| 0.000012
| 0.000906
| 0
| 0.000906
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1206953.cif
| false
| null |
data/final/MP/graphs/Bi1Er1Pd1-MP-mp-1206953.json
| 0
| true
|
-43m
| 5
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
This dataset contains 5,773 superconducting materials for training ML models to predict critical temperatures.
material_id: Unique identifiercif_id: Materials Project IDTc: Critical temperature (K)formula: Chemical formulacif_path: Path to CIF filefrom datasets import load_dataset
dataset = load_dataset("shreyaspulle98/superconductor-3dsc")
train_data = dataset["train"]
Court, C.J., et al. "3-D Inorganic Crystal Structure Generation" (2020)
MIT License