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
|
Ge0.5Rh0.5
| 1
| 0
| 8
| false
|
Ge4Rh4
|
Ge4Rh4
| 0.24
|
Other
| true
|
Ge50Rh50
|
Ge-Rh
| 2
|
Supercon
|
Ge0.5Rh0.5
|
MP-mp-22239
|
Ge4Rh4
|
Ge-Rh
|
Ge50Rh50
|
P n m a
|
orthorhombic
| 3.282371
| 5.749233
| 6.567262
|
data/final/MP/cifs/Ge0.5Rh0.5-MP-mp-22239.cif
|
data/source/MP/raw/cifs/mp-22239.cif
|
mp-22239
| 0
| null |
2014-02-22 13:55:04
| 9.408424
|
10.17188/1197455
|
@misc{osti_1197455,
author = "Persson, Kristin",
title = "Materials Data on GeRh (SG:62) 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 = "10.17188/1197455",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1698150'}}
| 0
| 5.552776
| 520
| -52.310376
| -6.538797
|
{'tags': ['Rhodium(VI) germanide', 'Germanium rhodium (1/1)']}
| -52.310376
| -6.538797
| -0.545129
|
['xas', 'bandstructure']
| true
|
[44861, 637675]
| true
|
2021-05-12 10:56:59.077000
|
NM
| 8
| 8
|
mp-22239
| null |
GeRh
|
{'functional': 'PBE', 'labels': ['Ge_d', 'Rh_pv'], 'pot_type': 'paw'}
|
{'Ge': 1.0, 'Rh': 1.0}
|
GGA
|
mp-22239
|
['mp-921160', 'mp-942968', 'mp-942589', 'mp-22239', 'mp-1421767', 'mp-1698150', 'mp-1881991', 'mp-1595988']
| 0.000485
|
{'Ge': 4.0, 'Rh': 4.0}
| 123.931561
|
[]
|
NM
| false
| 62
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0]
| 0.000016
| 0.000485
| 0
| 0.00194
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-22239.cif
| false
| null |
data/final/MP/graphs/Ge0.5Rh0.5-MP-mp-22239.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Be13Th0.009U0.991
| 2
| 0.001286
| 2
| false
|
Be26Th0.018U1.982
|
Be26U2
| 0.66
|
Heavy_fermion
| true
|
Be92.857Th0.064U7.079
|
Be-Th-U
| 3
|
Supercon
|
U0.9911Th0.0089Be13
|
MP-mp-1163
|
U2Be26
|
Be-U
|
Be92.857U7.143
|
F m -3 c
|
cubic
| 7.174676
| 7.174676
| 7.174676
|
data/final/MP/cifs/Be13Th0.009U0.991-MP-mp-1163-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1163.cif
|
mp-1163
| 0
| null |
2011-05-15 13:39:09
| 4.516943
|
10.17188/1188115
|
@misc{osti_1188115,
author = "Persson, Kristin",
title = "Materials Data on UBe13 (SG:226) 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 = "10.17188/1188115",
place = "United States",
year = "2015",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1676276'}}
| 0
| 5.60901
| 520
| -121.44122
| -4.337186
|
{'tags': ['Uranium beryllium (1/13)', 'Beryllium uranium (13/1)']}
| -121.44122
| -4.337186
| -0.058345
|
['xas', 'bandstructure']
| true
|
[616470, 58748, 616481, 58747, 58749, 659562, 107528, 600563, 58750, 616488, 58751]
| true
|
2021-05-12 10:56:51.169000
|
NM
| 28
| 8
|
mp-1163
| null |
UBe13
|
{'functional': 'PBE', 'labels': ['U', 'Be_sv'], 'pot_type': 'paw'}
|
{'U': 1.0, 'Be': 13.0}
|
GGA
|
mp-1163
|
['mp-1163', 'mp-906858', 'mp-920459', 'mp-921486', 'mp-1381018', 'mp-1676276', 'mp-1775695', 'mp-1603627']
| 0.046057
|
{'U': 2.0, 'Be': 26.0}
| 261.151106
|
[]
|
NM
| false
| 226
| 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]
| 0.000353
| 0.046057
| 0
| 0.092115
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1163.cif
| true
| null |
data/final/MP/graphs/Be13Th0.009U0.991-MP-mp-1163-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
Re0.7W0.3
| 3
| 0.1
| 8
| false
|
Re5.6W2.4
|
Re6W2
| 4.9
|
Other
| true
|
Re70W30
|
Re-W
| 2
|
Supercon
|
Re0.7W0.3
|
MP-mp-974408
|
Re6W2
|
Re-W
|
Re75W25
|
P 63/m m c
|
hexagonal
| 4.551902
| 5.592164
| 5.592164
|
data/final/MP/cifs/Re0.7W0.3-MP-mp-974408-synth_doped.cif
|
data/source/MP/raw/cifs/mp-974408.cif
|
mp-974408
| 0
| null |
2015-09-16 23:30:04
| 20.001815
|
10.17188/1314483
|
@misc{osti_1314483,
author = "Persson, Kristin",
title = "Materials Data on Re3W (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 = "10.17188/1314483",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1753563'}}
| 0.130423
| 7.034272
| 520
| -99.540031
| -12.442504
|
{'tags': []}
| -99.540031
| -12.442504
| 0.130423
|
['xas', 'bandstructure']
| true
|
[]
| true
|
2021-05-12 10:57:55.580000
|
NM
| 8
| 8
|
mp-974408
| null |
Re3W
|
{'functional': 'PBE', 'labels': ['Re_pv', 'W_pv'], 'pot_type': 'paw'}
|
{'Re': 3.0, 'W': 1.0}
|
GGA
|
mp-974408
|
['mp-974449', 'mp-974408', 'mp-974489', 'mp-1404689', 'mp-1753563', 'mp-1789838', 'mp-974542', 'mp-1618978']
| 0.000113
|
{'Re': 6.0, 'W': 2.0}
| 123.27736
|
[]
|
NM
| false
| 194
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0]
| 0.000002
| 0.000113
| 0
| 0.000226
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-974408.cif
| true
| null |
data/final/MP/graphs/Re0.7W0.3-MP-mp-974408-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B2Co2La1
| 1
| 0
| 1
| true
|
B2Co2La1
|
B2Co2La1
| 0
|
Other
| true
|
B40Co40La20
|
B-Co-La
| 3
|
Supercon
|
La1Co2B2
|
MP-mp-2967
|
La1Co2B2
|
B-Co-La
|
B40Co40La20
|
I 4/m m m
|
tetragonal
| 3.601524
| 3.601524
| 5.719602
|
data/final/MP/cifs/B2Co2La1-MP-mp-2967.cif
|
data/source/MP/raw/cifs/mp-2967.cif
|
mp-2967
| 0
| null |
2011-05-12 22:17:57
| 6.95906
|
10.17188/1204151
|
@misc{osti_1204151,
author = "Persson, Kristin",
title = "Materials Data on La(CoB)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 = "10.17188/1204151",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1672975'}}
| 0
| 7.488787
| 520
| -34.906073
| -6.981215
|
{'tags': ['Lanthanum cobalt boride (1/2/2)', 'Cobalt lanthanum boride (2/1/2)']}
| -34.906073
| -6.981215
| -0.478929
|
['xas', 'elasticity', 'bandstructure']
| true
|
[55297, 181184, 182572, 181185, 423045, 41787, 613135, 182573]
| true
|
2021-05-12 10:56:18.721000
|
NM
| 5
| 8
|
mp-2967
| null |
La(CoB)2
|
{'functional': 'PBE', 'labels': ['La', 'Co', 'B'], 'pot_type': 'paw'}
|
{'La': 1.0, 'Co': 2.0, 'B': 2.0}
|
GGA
|
mp-2967
|
['mp-1007012', 'mp-1000544', 'mp-2967', 'mp-1442119', 'mp-1672975', 'mp-1782552', 'mp-1011750', 'mp-1589504']
| 0.003647
|
{'La': 1.0, 'Co': 2.0, 'B': 2.0}
| 66.429072
|
[]
|
NM
| false
| 139
| 0
|
[0.0, -0.0, -0.0, 0.0, 0.0]
| 0.000055
| 0.003647
| 0
| 0.003647
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-2967.cif
| false
| null |
data/final/MP/graphs/B2Co2La1-MP-mp-2967.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Ga0.6Si0.4V3
| 2
| 0.05
| 2
| false
|
Ga1.2Si0.8V6
|
Ga1Si1V6
| 9.5
|
Other
| true
|
Ga15Si10V75
|
Ga-Si-V
| 3
|
Supercon
|
V3Ga0.6Si0.4
|
MP-mp-1216440
|
V6Ga1Si1
|
Ga-Si-V
|
Ga12.5Si12.5V75
|
P m -3
|
cubic
| 4.747019
| 4.747019
| 4.747019
|
data/final/MP/cifs/Ga0.6Si0.4V3-MP-mp-1216440-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1216440.cif
|
mp-1216440
| 0
| null |
2019-01-12 17:56:57.356000
| 6.263023
| null | null |
{'GGA': {'task_id': 'mp-1752355'}}
| 0.001212
| 6.464448
| 520
| -65.495396
| -8.186924
|
{'tags': []}
| -65.495396
| -8.186924
| -0.308444
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:39.488000
|
FM
| 8
| 5
|
mp-1216440
| null |
V6GaSi
|
{'functional': 'PBE', 'labels': ['V_pv', 'Ga_d', 'Si'], 'pot_type': 'paw'}
|
{'V': 6.0, 'Ga': 1.0, 'Si': 1.0}
|
GGA
|
mp-1216440
|
['mp-1216440', 'mp-1444194', 'mp-1752355', 'mp-1875781', 'mp-1620045']
| 2.026844
|
{'V': 6.0, 'Ga': 1.0, 'Si': 1.0}
| 106.970225
|
[]
|
FM
| true
| 47
| 1
|
[0.2, 0.3, 0.3, 0.2, 0.3, 0.3, 0.0, 0.0]
| 0.018948
| 2.026844
| 6
| 2.026844
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1216440.cif
| true
| null |
data/final/MP/graphs/Ga0.6Si0.4V3-MP-mp-1216440-synth_doped.json
| 0
| true
|
m-3
| 2
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B4Ru4Yb1
| 1
| 0
| 4
| false
|
B16Ru16Yb4
|
B16Ru16Yb4
| 0
|
Heavy_fermion
| true
|
B44.444Ru44.444Yb11.111
|
B-Ru-Yb
| 3
|
Supercon
|
Yb1Ru4B4
|
MP-mp-1200533
|
Yb4B16Ru16
|
B-Ru-Yb
|
B44.444Ru44.444Yb11.111
|
I 41/a c d
|
tetragonal
| 7.410006
| 7.410006
| 9.234024
|
data/final/MP/cifs/B4Ru4Yb1-MP-mp-1200533.cif
|
data/source/MP/raw/cifs/mp-1200533.cif
|
mp-1200533
| 0
| null |
2019-01-12 04:55:21.446000
| 9.872915
| null | null |
{'GGA': {'task_id': 'mp-1735025'}}
| 0
| 6.553183
| 520
| -276.663518
| -7.685098
|
{'tags': ['Ytterbium ruthenium boride (1/4/4)']}
| -276.663518
| -7.685098
| -0.423461
|
['bandstructure']
| true
|
[615409]
| true
|
2021-05-12 10:58:37.524000
|
NM
| 36
| 5
|
mp-1200533
| null |
Yb(BRu)4
|
{'functional': 'PBE', 'labels': ['Yb_2', 'B', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Yb': 1.0, 'B': 4.0, 'Ru': 4.0}
|
GGA
|
mp-1200533
|
['mp-1200533', 'mp-1404069', 'mp-1735025', 'mp-1815213', 'mp-1622918']
| 0.000256
|
{'Yb': 4.0, 'B': 16.0, 'Ru': 16.0}
| 417.49403
|
[]
|
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]
| 0.000002
| 0.000256
| 0
| 0.001023
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1200533.cif
| false
| null |
data/final/MP/graphs/B4Ru4Yb1-MP-mp-1200533.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
S1Ti1
| 1
| 0
| 1
| true
|
S1Ti1
|
S1Ti1
| 0
|
Other
| true
|
S50Ti50
|
S-Ti
| 2
|
Supercon
|
S1Ti1
|
MP-mp-1018028
|
Ti1S1
|
S-Ti
|
S50Ti50
|
P -6 m 2
|
hexagonal
| 3.219077
| 3.273882
| 3.273881
|
data/final/MP/cifs/S1Ti1-MP-mp-1018028.cif
|
data/source/MP/raw/cifs/mp-1018028.cif
|
mp-1018028
| 0
| null |
2017-04-06 22:57:05
| 4.442034
|
10.17188/1350110
|
@article{osti_1350110,
author = "Persson, Kristin",
title = "Materials Data on TiS (SG:187) 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 = "10.17188/1350110",
place = "United States",
year = "2017",
month = "4"
}
|
{'GGA': {'task_id': 'mp-1671827'}}
| 0
| 8.309589
| 520
| -14.968608
| -7.484304
|
{'tags': ['Titanium(II) sulfide']}
| -14.968608
| -7.484304
| -1.719833
|
['bandstructure', 'elasticity']
| true
|
[52193]
| true
|
2021-05-12 10:56:08.727000
|
NM
| 2
| 13
|
mp-1018028
| null |
TiS
|
{'functional': 'PBE', 'labels': ['Ti_pv', 'S'], 'pot_type': 'paw'}
|
{'Ti': 1.0, 'S': 1.0}
|
GGA
|
mp-1018028
|
['mp-1018185', 'mp-1018322', 'mp-1018445', 'mp-1018028', 'mp-1058248', 'mp-1058222', 'mp-1058274', 'mp-1115474', 'mp-1439018', 'mp-1671827', 'mp-1781459', 'mp-1589995', 'mp-1058264']
| 0.000395
|
{'Ti': 1.0, 'S': 1.0}
| 29.880502
|
[]
|
NM
| false
| 187
| 0
|
[0, 0]
| 0.000013
| 0.000395
| 0
| 0.000395
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1018028.cif
| false
| null |
data/final/MP/graphs/S1Ti1-MP-mp-1018028.json
| 0
| true
|
-62m
| 0
| 6
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ca0.113Cu1La1.887O4
| 2
| 0.032286
| 1
| true
|
Ca0.113Cu1La1.887O4
|
Cu1La2O4
| 20.1
|
Cuprate
| true
|
Ca1.614Cu14.286La26.957O57.142857142857146
|
Ca-Cu-La-O
| 4
|
Supercon
|
La1.887Ca0.1125Cu1O4
|
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/Ca0.113Cu1La1.887O4-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/Ca0.113Cu1La1.887O4-MP-mp-1077929-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
B2C1Cu0.1Ni1.9Y1
| 2
| 0.033333
| 1
| true
|
B2C1Cu0.1Ni1.9Y1
|
B2C1Ni2Y1
| 13.75
|
Other
| true
|
B33.333C16.667Cu1.667Ni31.667Y16.667
|
B-C-Cu-Ni-Y
| 5
|
Supercon
|
Y1Ni1.9Cu0.1B2C1
|
MP-mp-6576
|
Y1Ni2B2C1
|
B-C-Ni-Y
|
B33.333C16.667Ni33.333Y16.667
|
I 4/m m m
|
tetragonal
| 3.54879
| 3.54879
| 5.761441
|
data/final/MP/cifs/B2C1Cu0.1Ni1.9Y1-MP-mp-6576-synth_doped.cif
|
data/source/MP/raw/cifs/mp-6576.cif
|
mp-6576
| 0
| null |
2011-05-13 05:21:43
| 6.099731
|
10.17188/1281366
|
@misc{osti_1281366,
author = "Persson, Kristin",
title = "Materials Data on YNi2B2C (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 = "10.17188/1281366",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1688230'}}
| 0
| 6.81083
| 520
| -43.677878
| -7.279646
|
{'tags': []}
| -43.677878
| -7.279646
| -0.510928
|
['xas', 'bandstructure']
| true
|
[75816, 89142, 83231, 79574, 41549]
| true
|
2021-05-12 10:57:32.679000
|
NM
| 6
| 8
|
mp-6576
| null |
YNi2B2C
|
{'functional': 'PBE', 'labels': ['Y_sv', 'Ni_pv', 'B', 'C'], 'pot_type': 'paw'}
|
{'Y': 1.0, 'Ni': 2.0, 'B': 2.0, 'C': 1.0}
|
GGA
|
mp-6576
|
['mp-6576', 'mp-1007054', 'mp-1000583', 'mp-1439516', 'mp-1688230', 'mp-1794280', 'mp-1011792', 'mp-1597064']
| 0.00066
|
{'Y': 1.0, 'Ni': 2.0, 'B': 2.0, 'C': 1.0}
| 65.315244
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.00001
| 0.00066
| 0
| 0.00066
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-6576.cif
| true
| null |
data/final/MP/graphs/B2C1Cu0.1Ni1.9Y1-MP-mp-6576-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
B2Mg0.99Ti0.01
| 2
| 0.006667
| 1
| true
|
B2Mg0.99Ti0.01
|
B2Mg1
| 38.6
|
Other
| true
|
B66.667Mg33Ti0.333
|
B-Mg-Ti
| 3
|
Supercon
|
Mg0.99Ti0.01B2
|
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/B2Mg0.99Ti0.01-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/B2Mg0.99Ti0.01-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Cu1La2O4.022
| 2
| 0.002685
| 0.994677
| true
|
Cu0.995La1.989O4
|
Cu1La2O4
| 42
|
Cuprate
| true
|
Cu14.241La28.482O57.27712902307035
|
Cu-La-O
| 3
|
Supercon
|
La2Cu1O4.022
|
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/Cu1La2O4.022-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/Cu1La2O4.022-MP-mp-1077929-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Al0.15B2Mg0.85
| 3
| 0.1
| 1
| true
|
Al0.15B2Mg0.85
|
B2Mg1
| 31.5
|
Other
| true
|
Al5B66.667Mg28.333
|
Al-B-Mg
| 3
|
Supercon
|
Mg0.85Al0.15B2
|
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/Al0.15B2Mg0.85-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/Al0.15B2Mg0.85-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ba1Pb0.75Sb0.25O3
| 3
| 0.1
| 2
| false
|
Ba2Pb1.5Sb0.5O6
|
Ba2Pb2O6
| 3.5
|
Oxide
| true
|
Ba20Pb15Sb5O60
|
Ba-Pb-Sb-O
| 4
|
Supercon
|
Ba1Pb0.75Sb0.25O3
|
MP-mp-22230
|
Ba2Pb2O6
|
Ba-Pb-O
|
Ba20Pb20O60
|
I m m a
|
orthorhombic
| 6.133862
| 6.155867
| 6.155867
|
data/final/MP/cifs/Ba1Pb0.75Sb0.25O3-MP-mp-22230-synth_doped.cif
|
data/source/MP/raw/cifs/mp-22230.cif
|
mp-22230
| 0.2094
| null |
2014-02-21 02:34:22
| 7.878976
|
10.17188/1197446
|
@misc{osti_1197446,
author = "Persson, Kristin",
title = "Materials Data on BaPbO3 (SG:74) 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 = "10.17188/1197446",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1677620'}}
| 0
| 2.992944
| 520
| -57.917512
| -5.791751
|
{'tags': ['Barium plumbate(IV)', 'Barium lead oxide', 'Barium plumbate', 'Barium lead(IV) oxide']}
| -57.917512
| -5.791751
| -2.108851
|
['xas', 'bandstructure']
| true
|
[252031, 94313, 154038, 245600, 51657, 94312, 245601, 78681, 154039, 15933, 67811, 245602]
| true
|
2021-05-12 10:56:59.077000
|
NM
| 10
| 7
|
mp-22230
|
oxide
|
BaPbO3
|
{'functional': 'PBE', 'labels': ['Ba_sv', 'Pb_d', 'O'], 'pot_type': 'paw'}
|
{'Ba': 1.0, 'Pb': 1.0, 'O': 3.0}
|
GGA
|
mp-22230
|
['mp-547522', 'mp-22230', 'mp-1078282', 'mp-1437547', 'mp-1677620', 'mp-1828697', 'mp-1589590']
| 0.000057
|
{'Ba': 2.0, 'Pb': 2.0, 'O': 6.0}
| 165.453838
|
[]
|
NM
| false
| 74
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000001
| 0.000057
| 0
| 0.000113
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-22230.cif
| true
| null |
data/final/MP/graphs/Ba1Pb0.75Sb0.25O3-MP-mp-22230-synth_doped.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0.5
| false
|
Ce1Ge0.06Pt3Si0.94
| 2
| 0.024
| 1
| true
|
Ce1Ge0.06Pt3Si0.94
|
Ce1Pt3Si1
| 0.50525
|
Heavy_fermion
| true
|
Ce20Ge1.2Pt60Si18.8
|
Ce-Ge-Pt-Si
| 4
|
Supercon
|
Ce1Pt3Si0.94Ge0.06
|
MP-mp-1207119
|
Ce1Si1Pt3
|
Ce-Pt-Si
|
Ce20Pt60Si20
|
P 4 m m
|
tetragonal
| 4.067884
| 4.067884
| 5.552623
|
data/final/MP/cifs/Ce1Ge0.06Pt3Si0.94-MP-mp-1207119-synth_doped.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
| true
| null |
data/final/MP/graphs/Ce1Ge0.06Pt3Si0.94-MP-mp-1207119-synth_doped.json
| 0
| true
|
4mm
| 0
| 0
| 0
| 0
| 5
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Bi2Ca0.7Cu2I1Sr2Y0.3O8
| 3
| 0.0375
| 2
| false
|
Bi4Ca1.4Cu4I2Sr4Y0.6O16
|
Bi4Ca2Cu4I2Sr4O16
| 79
|
Cuprate
| true
|
Bi12.5Ca4.375Cu12.5I6.25Sr12.5Y1.875O50
|
Bi-Ca-Cu-I-Sr-Y-O
| 7
|
Supercon
|
Bi2Sr2Ca0.7Y0.3Cu2I1O8
|
MP-mp-1209124
|
Sr4Ca2Cu4Bi4I2O16
|
Bi-Ca-Cu-I-Sr-O
|
Bi12.5Ca6.25Cu12.5I6.25Sr12.5O50
|
P m n a
|
orthorhombic
| 5.21493
| 5.481615
| 19.120353
|
data/final/MP/cifs/Bi2Ca0.7Cu2I1Sr2Y0.3O8-MP-mp-1209124-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1209124.cif
|
mp-1209124
| 0
| null |
2019-01-12 11:54:40.777000
| 6.168903
| null | null | null | 0.092595
| 3.559223
| 520
| -175.928127
| -5.497754
|
{'tags': ['Sr2CaCu2Bi2IO8']}
| -175.928127
| -5.497754
| -1.960518
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:21.818000
|
NM
| 32
| 3
|
mp-1209124
|
oxide
|
Sr2CaCu2Bi2IO8
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Ca_sv', 'Cu_pv', 'Bi', 'I', 'O'], 'pot_type': 'paw'}
|
{'Sr': 2.0, 'Ca': 1.0, 'Cu': 2.0, 'Bi': 2.0, 'I': 1.0, 'O': 8.0}
|
GGA
|
mp-1209124
|
['mp-1209124', 'mp-1361882', 'mp-1929533']
| 0.311952
|
{'Sr': 4.0, 'Ca': 2.0, 'Cu': 4.0, 'Bi': 4.0, 'I': 2.0, 'O': 16.0}
| 546.578971
|
[]
|
NM
| false
| 53
| 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, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.001141
| 0.311952
| 0
| 0.623905
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1209124.cif
| true
| null |
data/final/MP/graphs/Bi2Ca0.7Cu2I1Sr2Y0.3O8-MP-mp-1209124-synth_doped.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Pt1Th1
| 1
| 0
| 2
| false
|
Pt2Th2
|
Pt2Th2
| 0.44
|
Other
| true
|
Pt50Th50
|
Pt-Th
| 2
|
Supercon
|
Pt1Th1
|
MP-mp-12754
|
Th2Pt2
|
Pt-Th
|
Pt50Th50
|
C m c m
|
orthorhombic
| 3.933814
| 4.483058
| 5.973476
|
data/final/MP/cifs/Pt1Th1-MP-mp-12754.cif
|
data/source/MP/raw/cifs/mp-12754.cif
|
mp-12754
| 0
| null |
2011-05-28 02:33:37
| 14.260536
|
10.17188/1189166
|
@misc{osti_1189166,
author = "Persson, Kristin",
title = "Materials Data on ThPt (SG:63) 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 = "10.17188/1189166",
place = "United States",
year = "2015",
month = "1",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1698852'}}
| 0
| 7.577259
| 520
| -31.82949
| -7.957373
|
{'tags': ['Thorium platinum (1/1)', 'Platinum thorium (1/1)']}
| -31.82949
| -7.957373
| -1.21499
|
['xas', 'bandstructure']
| true
|
[649759, 150541]
| true
|
2021-05-12 10:56:53.126000
|
NM
| 4
| 8
|
mp-12754
| null |
ThPt
|
{'functional': 'PBE', 'labels': ['Th', 'Pt'], 'pot_type': 'paw'}
|
{'Th': 1.0, 'Pt': 1.0}
|
GGA
|
mp-12754
|
['mp-919551', 'mp-905349', 'mp-918556', 'mp-12754', 'mp-1441702', 'mp-1698852', 'mp-1795835', 'mp-1591220']
| 0.000248
|
{'Th': 2.0, 'Pt': 2.0}
| 99.470714
|
[]
|
NM
| false
| 63
| 0
|
[0, 0, 0, 0]
| 0.000005
| 0.000248
| 0
| 0.000497
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-12754.cif
| false
| null |
data/final/MP/graphs/Pt1Th1-MP-mp-12754.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Cu2Gd1Ir0.05Ru0.95Sr2O8
| 2
| 0.007143
| 2
| false
|
Cu4Gd2Ir0.1Ru1.9Sr4O16
|
Cu4Gd2Ru2Sr4O16
| 32.5
|
Cuprate
| true
|
Cu14.286Gd7.143Ir0.357Ru6.786Sr14.286O57.142857142857146
|
Cu-Gd-Ir-Ru-Sr-O
| 6
|
Supercon
|
Ru0.95Ir0.05Sr2Gd1Cu2O8
|
MP-mp-1194240
|
Sr4Gd2Cu4Ru2O16
|
Cu-Gd-Ru-Sr-O
|
Cu14.286Gd7.143Ru7.143Sr14.286O57.142857142857146
|
P 4/m b m
|
tetragonal
| 5.472451
| 5.472451
| 11.740702
|
data/final/MP/cifs/Cu2Gd1Ir0.05Ru0.95Sr2O8-MP-mp-1194240-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1194240.cif
|
mp-1194240
| 0
| null |
2019-01-11 23:51:58.932000
| 6.504562
| null | null |
{'GGA': {'task_id': 'mp-1765260'}}
| 0.021345
| 3.935028
| 520
| -201.553522
| -7.19834
|
{'tags': ['Sr2Cu2GdRuO8 orth', 'Sr2Cu2GdRuO8', 'Ruthenium distrontium gadolinium dicopper octaoxide']}
| -201.553522
| -7.19834
| -2.268654
|
['bandstructure']
| true
|
[245741]
| true
|
2021-05-12 10:58:35.561000
|
FiM
| 28
| 6
|
mp-1194240
|
oxide
|
Sr2GdCu2RuO8
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Gd', 'Cu_pv', 'Ru_pv', 'O'], 'pot_type': 'paw'}
|
{'Sr': 2.0, 'Gd': 1.0, 'Cu': 2.0, 'Ru': 1.0, 'O': 8.0}
|
GGA
|
mp-1194240
|
['mp-1194240', 'mp-1396976', 'mp-1659973', 'mp-1765260', 'mp-1841948', 'mp-1638264']
| 4.236967
|
{'Sr': 4.0, 'Gd': 2.0, 'Cu': 4.0, 'Ru': 2.0, 'O': 16.0}
| 351.607255
|
[]
|
FiM
| true
| 127
| 2
|
[-0.0, -0.0, -0.0, -0.0, 6.9, 6.9, 0.0, 0.0, 0.0, 0.0, -1.8, -1.8, -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]
| 0.024101
| 4.236967
| 4
| 8.473934
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1194240.cif
| true
| null |
data/final/MP/graphs/Cu2Gd1Ir0.05Ru0.95Sr2O8-MP-mp-1194240-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
C1Mo0.95Nb0.05
| 2
| 0.05
| 1
| true
|
C1Mo0.95Nb0.05
|
C1Mo1
| 13.5
|
Other
| true
|
C50Mo47.5Nb2.5
|
C-Mo-Nb
| 3
|
Supercon
|
Nb0.05Mo0.95C1
|
MP-mp-2305
|
Mo1C1
|
C-Mo
|
C50Mo50
|
P -6 m 2
|
hexagonal
| 2.835086
| 2.924106
| 2.924105
|
data/final/MP/cifs/C1Mo0.95Nb0.05-MP-mp-2305-synth_doped.cif
|
data/source/MP/raw/cifs/mp-2305.cif
|
mp-2305
| 0
| null |
2011-05-12 17:49:42
| 8.538698
|
10.17188/1199194
|
@misc{osti_1199194,
author = "Persson, Kristin",
title = "Materials Data on MoC (SG:187) 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 = "10.17188/1199194",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1668222'}}
| 0.001024
| 8.626582
| 520
| -20.240148
| -10.120074
|
{'tags': ['Molybdenum carbide (1/1)']}
| -20.240148
| -10.120074
| -0.083862
|
['xas', 'elasticity', 'bandstructure']
| true
|
[77156, 618300]
| true
|
2021-05-12 10:56:16.728000
|
NM
| 2
| 9
|
mp-2305
| null |
MoC
|
{'functional': 'PBE', 'labels': ['Mo_pv', 'C'], 'pot_type': 'paw'}
|
{'Mo': 1.0, 'C': 1.0}
|
GGA
|
mp-2305
|
['mp-927633', 'mp-927239', 'mp-911174', 'mp-2305', 'mp-1116092', 'mp-1440368', 'mp-1668222', 'mp-1791400', 'mp-1638434']
| 0.000198
|
{'Mo': 1.0, 'C': 1.0}
| 20.993406
|
[]
|
NM
| false
| 187
| 0
|
[0, 0]
| 0.000009
| 0.000198
| 0
| 0.000198
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-2305.cif
| true
| null |
data/final/MP/graphs/C1Mo0.95Nb0.05-MP-mp-2305-synth_doped.json
| 0
| true
|
-62m
| 0
| 6
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
As2Ba0.85Fe2Na0.15
| 3
| 0.073333
| 3
| false
|
As6Ba2.55Fe6Na0.45
|
As6Ba2Fe6Na1
| 5.3
|
Ferrite
| true
|
As40Ba17Fe40Na3
|
As-Ba-Fe-Na
| 4
|
Supercon
|
Ba0.85Na0.15Fe2As2
|
MP-mp-1228583
|
Ba2Na1Fe6As6
|
As-Ba-Fe-Na
|
As40Ba13.333Fe40Na6.667
|
C 1 2/m 1
|
monoclinic
| 5.50216
| 6.99761
| 8.802836
|
data/final/MP/cifs/As2Ba0.85Fe2Na0.15-MP-mp-1228583-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1228583.cif
|
mp-1228583
| 0
| null |
2019-01-13 04:16:43.045000
| 6.084136
| null | null | null | 0.023893
| 4.38667
| 520
| -90.457989
| -6.030533
|
{'tags': []}
| -90.457989
| -6.030533
| -0.434851
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:59.151000
|
FM
| 15
| 3
|
mp-1228583
| null |
Ba2Na(FeAs)6
|
{'functional': 'PBE', 'labels': ['Ba_sv', 'Na_pv', 'Fe_pv', 'As'], 'pot_type': 'paw'}
|
{'Ba': 2.0, 'Na': 1.0, 'Fe': 6.0, 'As': 6.0}
|
GGA
|
mp-1228583
|
['mp-1228583', 'mp-1329033', 'mp-1656554']
| 1.37544
|
{'Ba': 2.0, 'Na': 1.0, 'Fe': 6.0, 'As': 6.0}
| 295.375951
|
[]
|
FM
| true
| 12
| 2
|
[0.0, 0.0, 0.0, 0.3, 0.2, 0.2, 0.2, 0.2, 0.3, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.004657
| 1.37544
| 6
| 1.37544
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1228583.cif
| true
| null |
data/final/MP/graphs/As2Ba0.85Fe2Na0.15-MP-mp-1228583-synth_doped.json
| 0
| true
|
2/m
| 0
| 0
| 3
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Ge2.2La1Pt1.8
| 3
| 0.08
| 1
| true
|
Ge2.2La1Pt1.8
|
Ge2La1Pt2
| 1.95
|
Other
| true
|
Ge44La20Pt36
|
Ge-La-Pt
| 3
|
Supercon
|
La1Pt1.8Ge2.2
|
MP-mp-21057
|
La1Ge2Pt2
|
Ge-La-Pt
|
Ge40La20Pt40
|
I 4/m m m
|
tetragonal
| 4.458128
| 4.458128
| 5.960432
|
data/final/MP/cifs/Ge2.2La1Pt1.8-MP-mp-21057-synth_doped.cif
|
data/source/MP/raw/cifs/mp-21057.cif
|
mp-21057
| 0
| null |
2014-02-21 09:25:11
| 11.137877
|
10.17188/1196317
|
@misc{osti_1196317,
author = "Persson, Kristin",
title = "Materials Data on La(GePt)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 = "10.17188/1196317",
place = "United States",
year = "2014",
month = "11",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1704515'}}
| 0.097341
| 6.859377
| 520
| -30.677544
| -6.135509
|
{'tags': ['Lanthanum platinum germanide (1/2/2)']}
| -30.677544
| -6.135509
| -0.870733
|
['xas', 'bandstructure']
| true
|
[53665]
| true
|
2021-05-12 10:56:57.051000
|
NM
| 5
| 8
|
mp-21057
| null |
La(GePt)2
|
{'functional': 'PBE', 'labels': ['La', 'Ge_d', 'Pt'], 'pot_type': 'paw'}
|
{'La': 1.0, 'Ge': 2.0, 'Pt': 2.0}
|
GGA
|
mp-21057
|
['mp-993642', 'mp-991893', 'mp-21057', 'mp-1429115', 'mp-1704515', 'mp-1783057', 'mp-994947', 'mp-1591906']
| 0.003651
|
{'La': 1.0, 'Ge': 2.0, 'Pt': 2.0}
| 100.538937
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0]
| 0.000036
| 0.003651
| 0
| 0.003651
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-21057.cif
| true
| null |
data/final/MP/graphs/Ge2.2La1Pt1.8-MP-mp-21057-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Bi2Pd1
| 1
| 0
| 2
| false
|
Bi4Pd2
|
Bi4Pd2
| 3.823333
|
Other
| true
|
Bi66.667Pd33.333
|
Bi-Pd
| 2
|
Supercon
|
Bi2Pd1
|
MP-mp-568746
|
Bi4Pd2
|
Bi-Pd
|
Bi66.667Pd33.333
|
C 1 2/m 1
|
monoclinic
| 4.340166
| 5.728344
| 6.823328
|
data/final/MP/cifs/Bi2Pd1-MP-mp-568746.cif
|
data/source/MP/raw/cifs/mp-568746.cif
|
mp-568746
| 0
| null |
2014-02-16 12:26:53
| 11.096922
|
10.17188/1274673
|
@misc{osti_1274673,
author = "Persson, Kristin",
title = "Materials Data on Bi2Pd (SG:12) 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 = "10.17188/1274673",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1705121'}}
| 0
| 6.179046
| 520
| -27.358006
| -4.559668
|
{'tags': ['Froodite', 'Bismuth palladium (2/1)', 'Palladium bismuthide (1/2)']}
| -27.358006
| -4.559668
| -0.239684
|
['xas', 'elasticity', 'bandstructure']
| true
|
[42565, 616946]
| true
|
2021-05-12 10:56:22.739000
|
NM
| 6
| 9
|
mp-568746
| null |
Bi2Pd
|
{'functional': 'PBE', 'labels': ['Bi', 'Pd'], 'pot_type': 'paw'}
|
{'Bi': 2.0, 'Pd': 1.0}
|
GGA
|
mp-568746
|
['mp-924877', 'mp-925451', 'mp-909850', 'mp-568746', 'mp-1077114', 'mp-1415370', 'mp-1705121', 'mp-1779403', 'mp-1588082']
| 0.000373
|
{'Bi': 4.0, 'Pd': 2.0}
| 156.936281
|
[]
|
NM
| false
| 12
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000005
| 0.000373
| 0
| 0.000745
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-568746.cif
| false
| null |
data/final/MP/graphs/Bi2Pd1-MP-mp-568746.json
| 0
| true
|
2/m
| 0
| 0
| 3
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Ir2Lu1
| 1
| 0
| 2
| false
|
Ir4Lu2
|
Ir4Lu2
| 2.47
|
Other
| true
|
Ir66.667Lu33.333
|
Ir-Lu
| 2
|
Supercon
|
Ir2Lu1
|
MP-mp-1761
|
Lu2Ir4
|
Ir-Lu
|
Ir66.667Lu33.333
|
F d -3 m
|
cubic
| 5.31576
| 5.31576
| 5.31576
|
data/final/MP/cifs/Ir2Lu1-MP-mp-1761.cif
|
data/source/MP/raw/cifs/mp-1761.cif
|
mp-1761
| 0
| null |
2011-05-13 05:05:15
| 17.491265
|
10.17188/1192590
|
@misc{osti_1192590,
author = "Persson, Kristin",
title = "Materials Data on LuIr2 (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 = "10.17188/1192590",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1702250'}}
| 0
| 6.82956
| 520
| -49.459782
| -8.243297
|
{'tags': ['Iridium lutetium (2/1)']}
| -49.459782
| -8.243297
| -0.844027
|
['xas', 'elasticity', 'bandstructure']
| true
|
[104491, 640781, 640782, 104492]
| true
|
2021-05-12 10:56:14.760000
|
NM
| 6
| 7
|
mp-1761
| null |
LuIr2
|
{'functional': 'PBE', 'labels': ['Lu_3', 'Ir'], 'pot_type': 'paw'}
|
{'Lu': 1.0, 'Ir': 2.0}
|
GGA
|
mp-1761
|
['mp-930555', 'mp-913757', 'mp-930053', 'mp-1761', 'mp-1441292', 'mp-1702250', 'mp-1597027']
| 0.013273
|
{'Lu': 2.0, 'Ir': 4.0}
| 106.213841
|
[]
|
NM
| false
| 227
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.00025
| 0.013273
| 0
| 0.026546
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1761.cif
| false
| null |
data/final/MP/graphs/Ir2Lu1-MP-mp-1761.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
B2C1Rh2Th1
| 1
| 0
| 1
| true
|
B2C1Rh2Th1
|
B2C1Rh2Th1
| 0
|
Other
| true
|
B33.333C16.667Rh33.333Th16.667
|
B-C-Rh-Th
| 4
|
Supercon
|
Th1Rh2B2C1
|
MP-mp-1080399
|
Th1B2Rh2C1
|
B-C-Rh-Th
|
B33.333C16.667Rh33.333Th16.667
|
I 4/m m m
|
tetragonal
| 3.893554
| 3.893554
| 5.807689
|
data/final/MP/cifs/B2C1Rh2Th1-MP-mp-1080399.cif
|
data/source/MP/raw/cifs/mp-1080399.cif
|
mp-1080399
| 0
| null |
2018-04-23 16:41:56
| 10.099294
| null | null |
{'GGA': {'task_id': 'mp-1688256'}}
| 0
| 7.688597
| 520
| -48.754372
| -8.125729
|
{'tags': ['Thorium rhodium boride carbide (1/2/2/1)', 'LuNi2B2C', 'ThRh2B2C']}
| -48.754372
| -8.125729
| -0.671056
|
['bandstructure']
| true
|
[659010]
| true
|
2021-05-12 10:58:16.596000
|
NM
| 6
| 5
|
mp-1080399
| null |
ThB2Rh2C
|
{'functional': 'PBE', 'labels': ['Th', 'B', 'Rh_pv', 'C'], 'pot_type': 'paw'}
|
{'Th': 1.0, 'B': 2.0, 'Rh': 2.0, 'C': 1.0}
|
GGA
|
mp-1080399
|
['mp-1080399', 'mp-1300113', 'mp-1688256', 'mp-1799448', 'mp-1594399']
| 0.000012
|
{'Th': 1.0, 'B': 2.0, 'Rh': 2.0, 'C': 1.0}
| 77.521645
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0, 0]
| 0
| 0.000012
| 0
| 0.000012
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1080399.cif
| false
| null |
data/final/MP/graphs/B2C1Rh2Th1-MP-mp-1080399.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
B0.08C0.92Cu1Sr2O5
| 2
| 0.017778
| 4
| false
|
B0.32C3.68Cu4Sr8O20
|
C4Cu4Sr8O20
| 25
|
Cuprate
| true
|
B0.889C10.222Cu11.111Sr22.222O55.55555555555556
|
B-C-Cu-Sr-O
| 5
|
Supercon
|
Sr2Cu1C0.92B0.08O5
|
MP-mp-1198030
|
Sr8Cu4C4O20
|
C-Cu-Sr-O
|
C11.111Cu11.111Sr22.222O55.55555555555556
|
I -4
|
tetragonal
| 7.877744
| 7.877744
| 9.467551
|
data/final/MP/cifs/B0.08C0.92Cu1Sr2O5-MP-mp-1198030-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1198030.cif
|
mp-1198030
| 0
| null |
2019-01-12 02:53:33.853000
| 4.624821
| null | null |
{'GGA': {'task_id': 'mp-1742814'}}
| 0.038619
| 3.478895
| 520
| -237.901634
| -6.608379
|
{'tags': ['Distrontium copper dioxide carbonate - LT', 'Distrontium copper dioxide carbonate']}
| -237.901634
| -6.608379
| -2.38507
|
['bandstructure']
| true
|
[78650, 83095]
| true
|
2021-05-12 10:58:37.524000
|
NM
| 36
| 6
|
mp-1198030
|
oxide
|
Sr2CuCO5
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Cu_pv', 'C', 'O'], 'pot_type': 'paw'}
|
{'Sr': 2.0, 'Cu': 1.0, 'C': 1.0, 'O': 5.0}
|
GGA
|
mp-1198030
|
['mp-1198030', 'mp-1200477', 'mp-1399692', 'mp-1742814', 'mp-1929945', 'mp-1655225']
| 0.000744
|
{'Sr': 8.0, 'Cu': 4.0, 'C': 4.0, 'O': 20.0}
| 475.085076
|
[]
|
NM
| false
| 82
| 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]
| 0.000006
| 0.000744
| 0
| 0.002976
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1198030.cif
| true
| null |
data/final/MP/graphs/B0.08C0.92Cu1Sr2O5-MP-mp-1198030-synth_doped.json
| 0
| true
|
-4
| 0
| 0
| 0
| 0
| 2
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Cr1Cu4Sr8Tl3O20
| 1
| 0
| 1
| true
|
Cr1Cu4Sr8Tl3O20
|
Cr1Cu4Sr8Tl3O20
| 25
|
Cuprate
| true
|
Cr2.778Cu11.111Sr22.222Tl8.333O55.55555555555556
|
Cr-Cu-Sr-Tl-O
| 5
|
Supercon
|
Tl3Cr1Sr8Cu4O20
|
MP-mp-559339
|
Sr8Tl3Cr1Cu4O20
|
Cr-Cu-Sr-Tl-O
|
Cr2.778Cu11.111Sr22.222Tl8.333O55.55555555555556
|
C m m m
|
orthorhombic
| 3.702758
| 11.790784
| 11.790784
|
data/final/MP/cifs/Cr1Cu4Sr8Tl3O20-MP-mp-559339.cif
|
data/source/MP/raw/cifs/mp-559339.cif
|
mp-559339
| 0
| null |
2014-03-04 11:49:15
| 6.344914
| null | null |
{'GGA+U': {'task_id': 'mp-1742799'}}
| 0.062621
| 3.360823
| 520
| -203.711973
| -5.658666
|
{'tags': ['Thallium chromate strontium coppper oxide (3/1/8/4/16)']}
| -203.711973
| -5.658666
| -2.051056
|
['xas']
| false
|
[81375]
| true
|
2021-05-12 10:57:23.123000
|
FM
| 36
| 5
|
mp-559339
|
oxide
|
Sr8Tl3Cr(CuO5)4
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Tl_d', 'Cr_pv', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'Sr': 8.0, 'Tl': 3.0, 'Cr': 1.0, 'Cu': 4.0, 'O': 20.0}
|
GGA+U
|
mp-559339
|
['mp-565938', 'mp-559339', 'mp-1446056', 'mp-1742799', 'mp-1825288']
| 1.047642
|
{'Sr': 8.0, 'Tl': 3.0, 'Cr': 1.0, 'Cu': 4.0, 'O': 20.0}
| 507.793723
|
[]
|
FM
| true
| 65
| 1
|
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.8, 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, 0.0]
| 0.002063
| 1.047642
| 1
| 1.047642
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-559339.cif
| false
| null |
data/final/MP/graphs/Cr1Cu4Sr8Tl3O20-MP-mp-559339.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Ir0.32Ru0.68
| 3
| 0.14
| 8
| false
|
Ir2.56Ru5.44
|
Ir2Ru6
| 0.18
|
Other
| true
|
Ir32Ru68
|
Ir-Ru
| 2
|
Supercon
|
Ir0.32Ru0.68
|
MP-mp-862620
|
Ir2Ru6
|
Ir-Ru
|
Ir25Ru75
|
P 63/m m c
|
hexagonal
| 4.324858
| 5.47935
| 5.47935
|
data/final/MP/cifs/Ir0.32Ru0.68-MP-mp-862620-synth_doped.cif
|
data/source/MP/raw/cifs/mp-862620.cif
|
mp-862620
| 0
| null |
2014-08-23 01:08:58
| 14.631816
|
10.17188/1309490
|
@misc{osti_1309490,
author = "Persson, Kristin",
title = "Materials Data on Ru3Ir (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 = "10.17188/1309490",
place = "United States",
year = "2016",
month = "8",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1754749'}}
| 0
| 8.78966
| 520
| -73.744761
| -9.218095
|
{'tags': []}
| -73.744761
| -9.218095
| -0.052695
|
['xas', 'elasticity', 'bandstructure']
| true
|
[]
| true
|
2021-05-12 10:56:31.128000
|
NM
| 8
| 11
|
mp-862620
| null |
IrRu3
|
{'functional': 'PBE', 'labels': ['Ir', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Ir': 1.0, 'Ru': 3.0}
|
GGA
|
mp-862620
|
['mp-862620', 'mp-1002464', 'mp-1004058', 'mp-1050147', 'mp-1050219', 'mp-1385810', 'mp-1754749', 'mp-1804901', 'mp-1009375', 'mp-1619818', 'mp-1050210']
| 0.000759
|
{'Ir': 2.0, 'Ru': 6.0}
| 112.45028
|
[]
|
NM
| false
| 194
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0]
| 0.000014
| 0.000759
| 0
| 0.001519
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-862620.cif
| true
| null |
data/final/MP/graphs/Ir0.32Ru0.68-MP-mp-862620-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ca0.16Cu1La1.84O4
| 3
| 0.045714
| 1
| true
|
Ca0.16Cu1La1.84O4
|
Cu1La2O4
| 34
|
Cuprate
| true
|
Ca2.286Cu14.286La26.286O57.142857142857146
|
Ca-Cu-La-O
| 4
|
Supercon
|
La1.84Ca0.16Cu1O4
|
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/Ca0.16Cu1La1.84O4-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/Ca0.16Cu1La1.84O4-MP-mp-1077929-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
B2C1Dy0.2Ho0.8Ni2
| 3
| 0.066667
| 1
| true
|
B2C1Dy0.2Ho0.8Ni2
|
B2C1Ho1Ni2
| 6.61
|
Other
| true
|
B33.333C16.667Dy3.333Ho13.333Ni33.333
|
B-C-Dy-Ho-Ni
| 5
|
Supercon
|
Ho0.8Dy0.2Ni2B2C1
|
MP-mp-6646
|
Ho1Ni2B2C1
|
B-C-Ho-Ni
|
B33.333C16.667Ho16.667Ni33.333
|
I 4/m m m
|
tetragonal
| 3.529864
| 3.529864
| 5.760322
|
data/final/MP/cifs/B2C1Dy0.2Ho0.8Ni2-MP-mp-6646-synth_doped.cif
|
data/source/MP/raw/cifs/mp-6646.cif
|
mp-6646
| 0
| null |
2011-05-13 04:24:09
| 8.110751
|
10.17188/1281460
|
@misc{osti_1281460,
author = "Persson, Kristin",
title = "Materials Data on HoNi2B2C (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 = "10.17188/1281460",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1670774'}}
| 0
| 6.709814
| 520
| -41.843646
| -6.973941
|
{'tags': ['Holmium dinickel diboride carbide']}
| -41.843646
| -6.973941
| -0.519233
|
['xas', 'elasticity', 'bandstructure']
| true
|
[79064, 56650, 79065, 79062, 79063, 79575]
| true
|
2021-05-12 10:56:27.046000
|
NM
| 6
| 8
|
mp-6646
| null |
HoNi2B2C
|
{'functional': 'PBE', 'labels': ['Ho_3', 'Ni_pv', 'B', 'C'], 'pot_type': 'paw'}
|
{'Ho': 1.0, 'Ni': 2.0, 'B': 2.0, 'C': 1.0}
|
GGA
|
mp-6646
|
['mp-1007146', 'mp-6646', 'mp-1000682', 'mp-1439301', 'mp-1670774', 'mp-1782657', 'mp-1011887', 'mp-1589032']
| 0.003246
|
{'Ho': 1.0, 'Ni': 2.0, 'B': 2.0, 'C': 1.0}
| 64.685379
|
[]
|
NM
| false
| 139
| 0
|
[0.0, -0.0, -0.0, 0.0, 0.0, 0.0]
| 0.00005
| 0.003246
| 0
| 0.003246
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-6646.cif
| true
| null |
data/final/MP/graphs/B2C1Dy0.2Ho0.8Ni2-MP-mp-6646-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
As2Ba0.84Fe2K0.16
| 3
| 0.069333
| 3
| false
|
As6Ba2.52Fe6K0.48
|
As6Ba2Fe6K1
| 6.42
|
Ferrite
| true
|
As40Ba16.8Fe40K3.2
|
As-Ba-Fe-K
| 4
|
Supercon
|
Ba0.84K0.16Fe2As2
|
MP-mp-1223567
|
K1Ba2Fe6As6
|
As-Ba-Fe-K
|
As40Ba13.333Fe40K6.667
|
C 1 2/m 1
|
monoclinic
| 5.480608
| 7.1028
| 8.784942
|
data/final/MP/cifs/As2Ba0.84Fe2K0.16-MP-mp-1223567-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1223567.cif
|
mp-1223567
| 0
| null |
2019-01-12 23:56:38.667000
| 6.101417
| null | null | null | 0.018688
| 4.380144
| 520
| -90.515093
| -6.03434
|
{'tags': []}
| -90.515093
| -6.03434
| -0.452799
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:52.054000
|
FM
| 15
| 4
|
mp-1223567
| null |
KBa2(FeAs)6
|
{'functional': 'PBE', 'labels': ['K_sv', 'Ba_sv', 'Fe_pv', 'As'], 'pot_type': 'paw'}
|
{'K': 1.0, 'Ba': 2.0, 'Fe': 6.0, 'As': 6.0}
|
GGA
|
mp-1223567
|
['mp-1223567', 'mp-1374097', 'mp-1656306', 'mp-1808539']
| 1.332645
|
{'K': 1.0, 'Ba': 2.0, 'Fe': 6.0, 'As': 6.0}
| 298.923365
|
[]
|
FM
| true
| 12
| 2
|
[0.0, 0.0, 0.0, 0.3, 0.3, 0.1, 0.3, 0.1, 0.3, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.004458
| 1.332645
| 6
| 1.332645
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1223567.cif
| true
| null |
data/final/MP/graphs/As2Ba0.84Fe2K0.16-MP-mp-1223567-synth_doped.json
| 0
| true
|
2/m
| 0
| 0
| 3
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
B2C1Ni2Pr0.05Y0.95
| 2
| 0.016667
| 1
| true
|
B2C1Ni2Pr0.05Y0.95
|
B2C1Ni2Y1
| 14.05
|
Other
| true
|
B33.333C16.667Ni33.333Pr0.833Y15.833
|
B-C-Ni-Pr-Y
| 5
|
Supercon
|
Y0.95Pr0.05Ni2B2C1
|
MP-mp-6576
|
Y1Ni2B2C1
|
B-C-Ni-Y
|
B33.333C16.667Ni33.333Y16.667
|
I 4/m m m
|
tetragonal
| 3.54879
| 3.54879
| 5.761441
|
data/final/MP/cifs/B2C1Ni2Pr0.05Y0.95-MP-mp-6576-synth_doped.cif
|
data/source/MP/raw/cifs/mp-6576.cif
|
mp-6576
| 0
| null |
2011-05-13 05:21:43
| 6.099731
|
10.17188/1281366
|
@misc{osti_1281366,
author = "Persson, Kristin",
title = "Materials Data on YNi2B2C (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 = "10.17188/1281366",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1688230'}}
| 0
| 6.81083
| 520
| -43.677878
| -7.279646
|
{'tags': []}
| -43.677878
| -7.279646
| -0.510928
|
['xas', 'bandstructure']
| true
|
[75816, 89142, 83231, 79574, 41549]
| true
|
2021-05-12 10:57:32.679000
|
NM
| 6
| 8
|
mp-6576
| null |
YNi2B2C
|
{'functional': 'PBE', 'labels': ['Y_sv', 'Ni_pv', 'B', 'C'], 'pot_type': 'paw'}
|
{'Y': 1.0, 'Ni': 2.0, 'B': 2.0, 'C': 1.0}
|
GGA
|
mp-6576
|
['mp-6576', 'mp-1007054', 'mp-1000583', 'mp-1439516', 'mp-1688230', 'mp-1794280', 'mp-1011792', 'mp-1597064']
| 0.00066
|
{'Y': 1.0, 'Ni': 2.0, 'B': 2.0, 'C': 1.0}
| 65.315244
|
[]
|
NM
| false
| 139
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.00001
| 0.00066
| 0
| 0.00066
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-6576.cif
| true
| null |
data/final/MP/graphs/B2C1Ni2Pr0.05Y0.95-MP-mp-6576-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Re3W1
| 1
| 0
| 1
| true
|
Re3W1
|
Re3W1
| 8.733333
|
Other
| true
|
Re75W25
|
Re-W
| 2
|
Supercon
|
Re3W1
|
MP-mp-974416
|
Re3W1
|
Re-W
|
Re75W25
|
I 4/m m m
|
tetragonal
| 3.957486
| 3.957486
| 4.831944
|
data/final/MP/cifs/Re3W1-MP-mp-974416.cif
|
data/source/MP/raw/cifs/mp-974416.cif
|
mp-974416
| 0
| null |
2015-09-16 23:33:34
| 19.984001
|
10.17188/1314486
|
@misc{osti_1314486,
author = "Persson, Kristin",
title = "Materials Data on Re3W (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 = "10.17188/1314486",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1765313'}}
| 0.127501
| 7.231799
| 520
| -49.781703
| -12.445426
|
{'tags': []}
| -49.781703
| -12.445426
| 0.127501
|
['xas', 'elasticity', 'bandstructure']
| true
|
[]
| true
|
2021-05-12 10:56:35.166000
|
NM
| 4
| 8
|
mp-974416
| null |
Re3W
|
{'functional': 'PBE', 'labels': ['Re_pv', 'W_pv'], 'pot_type': 'paw'}
|
{'Re': 3.0, 'W': 1.0}
|
GGA
|
mp-974416
|
['mp-974416', 'mp-974475', 'mp-974524', 'mp-1417436', 'mp-1765313', 'mp-1783614', 'mp-974552', 'mp-1613935']
| 0.003286
|
{'Re': 3.0, 'W': 1.0}
| 61.693627
|
[]
|
NM
| false
| 139
| 0
|
[0.0, 0.0, 0.0, 0.0]
| 0.000053
| 0.003286
| 0
| 0.003286
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-974416.cif
| false
| null |
data/final/MP/graphs/Re3W1-MP-mp-974416.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
Gd0.08Ru2Y0.92
| 3
| 0.053333
| 4
| false
|
Gd0.32Ru8Y3.68
|
Ru8Y4
| 2.2
|
Other
| true
|
Gd2.667Ru66.667Y30.667
|
Gd-Ru-Y
| 3
|
Supercon
|
Y0.92Gd0.08Ru2
|
MP-mp-568186
|
Y4Ru8
|
Ru-Y
|
Ru66.667Y33.333
|
P 63/m m c
|
hexagonal
| 5.276516
| 5.276516
| 8.969022
|
data/final/MP/cifs/Gd0.08Ru2Y0.92-MP-mp-568186-synth_doped.cif
|
data/source/MP/raw/cifs/mp-568186.cif
|
mp-568186
| 0
| null |
2014-02-24 13:08:31
| 8.939233
|
10.17188/1272553
|
@misc{osti_1272553,
author = "Persson, Kristin",
title = "Materials Data on YRu2 (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 = "10.17188/1272553",
place = "United States",
year = "2016",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1697189'}}
| 0
| 5.963037
| 520
| -103.834048
| -8.652837
|
{'tags': ['Yttrium ruthenium (1/2)', 'Ruthenium yttrium (2/1)']}
| -103.834048
| -8.652837
| -0.314421
|
['xas', 'elasticity', 'bandstructure']
| true
|
[150516, 650775, 650778]
| true
|
2021-05-12 10:56:22.739000
|
NM
| 12
| 10
|
mp-568186
| null |
YRu2
|
{'functional': 'PBE', 'labels': ['Y_sv', 'Ru_pv'], 'pot_type': 'paw'}
|
{'Y': 1.0, 'Ru': 2.0}
|
GGA
|
mp-568186
|
['mp-1001392', 'mp-914500', 'mp-568186', 'mp-1102880', 'mp-1103240', 'mp-1432386', 'mp-1697189', 'mp-1829069', 'mp-1007832', 'mp-1599952']
| 0.006527
|
{'Y': 4.0, 'Ru': 8.0}
| 216.257038
|
[]
|
NM
| false
| 194
| 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]
| 0.000121
| 0.006527
| 0
| 0.026106
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-568186.cif
| true
| null |
data/final/MP/graphs/Gd0.08Ru2Y0.92-MP-mp-568186-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ba2Cu3La0.8Pr0.2O7
| 3
| 0.030769
| 1
| true
|
Ba2Cu3La0.8Pr0.2O7
|
Ba2Cu3La1O7
| 59.8
|
Cuprate
| true
|
Ba15.385Cu23.077La6.154Pr1.538O53.84615384615385
|
Ba-Cu-La-Pr-O
| 5
|
Supercon
|
La0.8Pr0.2Ba2Cu3O7
|
MP-mp-622210
|
Ba2La1Cu3O7
|
Ba-Cu-La-O
|
Ba15.385Cu23.077La7.692O53.84615384615385
|
P m m m
|
orthorhombic
| 3.912033
| 3.978575
| 11.900925
|
data/final/MP/cifs/Ba2Cu3La0.8Pr0.2O7-MP-mp-622210-synth_doped.cif
|
data/source/MP/raw/cifs/mp-622210.cif
|
mp-622210
| 0
| null |
2014-02-16 07:47:08
| 6.420496
|
10.17188/1278110
|
@misc{osti_1278110,
author = "Persson, Kristin",
title = "Materials Data on Ba2LaCu3O7 (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 = "10.17188/1278110",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1676618'}}
| 0.020601
| 3.942262
| 520
| -79.094448
| -6.084188
|
{'tags': ['Lanthanum dibarium tricopper heptaoxide']}
| -79.094448
| -6.084188
| -2.168935
|
['bandstructure']
| true
|
[81167]
| true
|
2021-05-12 10:58:51.532000
|
NM
| 13
| 10
|
mp-622210
|
oxide
|
Ba2LaCu3O7
|
{'functional': 'PBE', 'labels': ['Ba_sv', 'La', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'Ba': 2.0, 'La': 1.0, 'Cu': 3.0, 'O': 7.0}
|
GGA
|
mp-622210
|
['mp-932742', 'mp-931665', 'mp-916330', 'mp-622210', 'mp-1228591', 'mp-1236979', 'mp-1381031', 'mp-1676618', 'mp-1832760', 'mp-1598015']
| 0.000006
|
{'Ba': 2.0, 'La': 1.0, 'Cu': 3.0, 'O': 7.0}
| 185.229766
|
[]
|
NM
| false
| 47
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0
| 0.000006
| 0
| 0.000006
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-622210.cif
| true
| null |
data/final/MP/graphs/Ba2Cu3La0.8Pr0.2O7-MP-mp-622210-synth_doped.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B2Li0.05Mg0.95
| 2
| 0.033333
| 1
| true
|
B2Li0.05Mg0.95
|
B2Mg1
| 38.25
|
Other
| true
|
B66.667Li1.667Mg31.667
|
B-Li-Mg
| 3
|
Supercon
|
Mg0.95Li0.05B2
|
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/B2Li0.05Mg0.95-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/B2Li0.05Mg0.95-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
B2Mo1
| 1
| 0
| 2
| false
|
B4Mo2
|
B4Mo2
| 0
|
Other
| true
|
B66.667Mo33.333
|
B-Mo
| 2
|
Supercon
|
B2Mo1
|
MP-mp-2331
|
B4Mo2
|
B-Mo
|
B66.667Mo33.333
|
R -3 m
|
trigonal
| 3.027959
| 3.027959
| 7.203934
|
data/final/MP/cifs/B2Mo1-MP-mp-2331.cif
|
data/source/MP/raw/cifs/mp-2331.cif
|
mp-2331
| 0
| null |
2011-05-12 22:01:57
| 7.035996
|
10.17188/1199416
|
@misc{osti_1199416,
author = "Persson, Kristin",
title = "Materials Data on B2Mo (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 = "10.17188/1199416",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1686405'}}
| 0
| 8.848587
| 520
| -50.999193
| -8.499866
|
{'tags': ['Molybdenum boride (1/2)', 'Molybdenum diboride', 'Molybdenum boride (2/4)', 'Molybdenum boride (1/2) - beta', 'Molybdenum boride', 'Dimolybdenium tetraboride']}
| -50.999193
| -8.499866
| -0.431723
|
['xas', 'elasticity', 'bandstructure']
| true
|
[252125, 40907, 418397, 418398, 39554, 167732, 44451, 191908]
| true
|
2021-05-12 10:56:16.728000
|
NM
| 6
| 13
|
mp-2331
| null |
B2Mo
|
{'functional': 'PBE', 'labels': ['B', 'Mo_pv'], 'pot_type': 'paw'}
|
{'B': 2.0, 'Mo': 1.0}
|
GGA
|
mp-2331
|
['mp-920254', 'mp-921267', 'mp-906549', 'mp-2331', 'mp-1070862', 'mp-1070903', 'mp-1070939', 'mp-1077759', 'mp-1440002', 'mp-1686405', 'mp-1793532', 'mp-1588848', 'mp-1070920']
| 0.000616
|
{'B': 4.0, 'Mo': 2.0}
| 55.490733
|
[]
|
NM
| false
| 166
| 0
|
[0, 0, 0, 0, 0, 0]
| 0.000022
| 0.000616
| 0
| 0.001232
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-2331.cif
| false
| null |
data/final/MP/graphs/B2Mo1-MP-mp-2331.json
| 0
| true
|
-3m
| 0
| 0
| 0
| 0
| 0
| 0
| 6
| 1
| 0
| 0
| 0
| 1
| false
|
B1.84C0.16Mg1
| 3
| 0.106667
| 1
| true
|
B1.84C0.16Mg1
|
B2Mg1
| 33
|
Other
| true
|
B61.333C5.333Mg33.333
|
B-C-Mg
| 3
|
Supercon
|
Mg1B1.84C0.16
|
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/B1.84C0.16Mg1-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/B1.84C0.16Mg1-MP-mp-763-synth_doped.json
| 0
| true
|
6/mmm
| 0
| 7
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Mo6Se6Tl2
| 1
| 0
| 1
| true
|
Mo6Se6Tl2
|
Mo6Se6Tl2
| 2.2875
|
Chevrel
| true
|
Mo42.857Se42.857Tl14.286
|
Mo-Se-Tl
| 3
|
Supercon
|
Tl2Mo6Se6
|
MP-mp-3411
|
Tl2Mo6Se6
|
Mo-Se-Tl
|
Mo42.857Se42.857Tl14.286
|
P 63/m
|
hexagonal
| 4.528686
| 9.236128
| 9.236128
|
data/final/MP/cifs/Mo6Se6Tl2-MP-mp-3411.cif
|
data/source/MP/raw/cifs/mp-3411.cif
|
mp-3411
| 0.3883
| null |
2011-05-15 16:41:52
| 7.237249
|
10.17188/1206717
|
@misc{osti_1206717,
author = "Persson, Kristin",
title = "Materials Data on Tl(MoSe)3 (SG:176) 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 = "10.17188/1206717",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1704781'}}
| 0
| 5.083103
| 520
| -97.577307
| -6.969808
|
{'tags': ['Thallium molybdenum selenide (1/3/3)', 'Thallium molybdenum(I/II) selenide (1/3/3)', 'Dithallium octahedro-hexakis(selenomolybdate)', 'Dithallium hexaseleno-octahedro-hexamolybdenum']}
| -97.577307
| -6.969808
| -0.688192
|
['xas', 'bandstructure']
| true
|
[53119, 644382, 603627, 23301, 644383, 644381, 604524]
| true
|
2021-05-12 10:57:06.958000
|
NM
| 14
| 10
|
mp-3411
| null |
Tl(MoSe)3
|
{'functional': 'PBE', 'labels': ['Tl_d', 'Mo_pv', 'Se'], 'pot_type': 'paw'}
|
{'Tl': 1.0, 'Mo': 3.0, 'Se': 3.0}
|
GGA
|
mp-3411
|
['mp-926439', 'mp-910675', 'mp-926951', 'mp-3411', 'mp-1103582', 'mp-1105103', 'mp-1416373', 'mp-1704781', 'mp-1806018', 'mp-1601950']
| 0.00009
|
{'Tl': 2.0, 'Mo': 6.0, 'Se': 6.0}
| 334.566733
|
[]
|
NM
| false
| 176
| 0
|
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
| 0.000001
| 0.00009
| 0
| 0.000179
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-3411.cif
| false
| null |
data/final/MP/graphs/Mo6Se6Tl2-MP-mp-3411.json
| 0
| true
|
6/m
| 0
| 3
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ce3Ge2Rh2
| 1
| 0
| 4
| false
|
Ce12Ge8Rh8
|
Ce12Ge8Rh8
| 0
|
Heavy_fermion
| true
|
Ce42.857Ge28.571Rh28.571
|
Ce-Ge-Rh
| 3
|
Supercon
|
Ce3Rh2Ge2
|
MP-mp-21597
|
Ce12Ge8Rh8
|
Ce-Ge-Rh
|
Ce42.857Ge28.571Rh28.571
|
P b c m
|
orthorhombic
| 5.608529
| 8.081324
| 13.309131
|
data/final/MP/cifs/Ce3Ge2Rh2-MP-mp-21597.cif
|
data/source/MP/raw/cifs/mp-21597.cif
|
mp-21597
| 0
| null |
2014-02-15 07:04:21
| 8.494337
|
10.17188/1197023
|
@misc{osti_1197023,
author = "Persson, Kristin",
title = "Materials Data on Ce3(GeRh)2 (SG:57) 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 = "10.17188/1197023",
place = "United States",
year = "2016",
month = "2",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1752907'}}
| 0
| 7.934614
| 520
| -191.004174
| -6.821578
|
{'tags': ['Cerium rhodium germanide (3/2/2)']}
| -191.004174
| -6.821578
| -0.853872
|
['xas']
| false
|
[76352]
| true
|
2021-05-12 10:56:59.077000
|
FM
| 28
| 7
|
mp-21597
| null |
Ce3(GeRh)2
|
{'functional': 'PBE', 'labels': ['Ce', 'Ge_d', 'Rh_pv'], 'pot_type': 'paw'}
|
{'Ce': 3.0, 'Ge': 2.0, 'Rh': 2.0}
|
GGA
|
mp-21597
|
['mp-922122', 'mp-940019', 'mp-940486', 'mp-21597', 'mp-1383857', 'mp-1752907', 'mp-1936964']
| 1.981192
|
{'Ce': 12.0, 'Ge': 8.0, 'Rh': 8.0}
| 603.227579
|
[]
|
FM
| true
| 57
| 2
|
[0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 0.6, 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]
| 0.013137
| 1.981192
| 12
| 7.924769
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-21597.cif
| false
| null |
data/final/MP/graphs/Ce3Ge2Rh2-MP-mp-21597.json
| 0
| true
|
mmm
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Ce0.15Cu1Nd1.85O4
| 2
| 0.042857
| 1
| true
|
Ce0.15Cu1Nd1.85O4
|
Cu1Nd2O4
| 21.2325
|
Cuprate
| true
|
Ce2.143Cu14.286Nd26.429O57.142857142857146
|
Ce-Cu-Nd-O
| 4
|
Supercon
|
Nd1.85Ce0.15Cu1O4
|
MP-mp-4158
|
Nd2Cu1O4
|
Cu-Nd-O
|
Cu14.286Nd28.571O57.142857142857146
|
I 4/m m m
|
tetragonal
| 3.973854
| 3.973854
| 6.782969
|
data/final/MP/cifs/Ce0.15Cu1Nd1.85O4-MP-mp-4158-synth_doped.cif
|
data/source/MP/raw/cifs/mp-4158.cif
|
mp-4158
| 0
| null |
2011-05-13 10:19:33
| 7.086167
|
10.17188/1207899
|
@misc{osti_1207899,
author = "Persson, Kristin",
title = "Materials Data on Nd2CuO4 (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 = "10.17188/1207899",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-670050'}}
| 0.00095
| 3.165109
| 520
| -51.480915
| -7.354416
|
{'tags': ['Dineodymium copper tetraoxide', 'Dineodymium copper oxide', 'Dineodymium cuprate', 'High pressure experimental phase']}
| -51.480915
| -7.354416
| -2.971654
|
['xas', 'elasticity', 'bandstructure']
| true
|
[261376, 203228, 160629, 261375, 69479, 186590, 4203, 75830, 75825, 202885, 203229, 71181, 82067, 75828, 69886, 75826, 75829, 75824, 75827, 69482, 86752]
| true
|
2021-05-12 10:56:20.740000
|
NM
| 7
| 11
|
mp-4158
|
oxide
|
Nd2CuO4
|
{'functional': 'PBE', 'labels': ['Nd_3', 'Cu_pv', 'O'], 'pot_type': 'paw'}
|
{'Nd': 2.0, 'Cu': 1.0, 'O': 4.0}
|
GGA
|
mp-4158
|
['mp-670050', 'mp-660368', 'mp-4158', 'mp-1078016', 'mp-1173374', 'mp-1440751', 'mp-1668619', 'mp-1797319', 'mp-1588086', 'mp-1590518', 'mp-688505']
| 0.00849
|
{'Nd': 2.0, 'Cu': 1.0, 'O': 4.0}
| 97.489948
|
[]
|
NM
| false
| 139
| 0
|
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.000087
| 0.00849
| 0
| 0.00849
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-4158.cif
| true
| null |
data/final/MP/graphs/Ce0.15Cu1Nd1.85O4-MP-mp-4158-synth_doped.json
| 0
| true
|
4/mmm
| 0
| 0
| 0
| 0
| 7
| 0
| 0
| 0
| 0
| 1
| 0
| 1
| false
|
N0.84Ti1
| 3
| 0.086957
| 1
| true
|
N0.84Ti1
|
N1Ti1
| 0
|
Other
| true
|
N45.652Ti54.348
|
N-Ti
| 2
|
Supercon
|
N0.84Ti1
|
MP-mp-492
|
Ti1N1
|
N-Ti
|
N50Ti50
|
F m -3 m
|
cubic
| 3.007703
| 3.007703
| 3.007703
|
data/final/MP/cifs/N0.84Ti1-MP-mp-492-synth_doped.cif
|
data/source/MP/raw/cifs/mp-492.cif
|
mp-492
| 0
| null |
2011-05-12 17:28:04
| 5.340297
|
10.17188/1208488
|
@misc{osti_1208488,
author = "Persson, Kristin",
title = "Materials Data on TiN (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 = "10.17188/1208488",
place = "United States",
year = "2014",
month = "7",
note = "An optional note"
}
|
{'GGA': {'task_id': 'mp-1674200'}}
| 0
| 9.097731
| 520
| -19.664995
| -9.832498
|
{'tags': ['Titanium nitride', 'Titanium nitride (1/1)', 'Titanium(III) nitride', 'Titanium nitride - B1', 'Osbornite']}
| -19.664995
| -9.832498
| -1.897004
|
['xas', 'elasticity', 'bandstructure']
| true
|
[26947, 192040, 181787, 644778, 64905, 64909, 183415, 236802, 105128, 184916, 644774, 644770, 644780, 644768, 644783, 186008, 152807, 187188, 644777, 644772, 644781, 64904, 656836, 604220, 236801, 644769, 644775, 644776, 186382, 658338, 601248, 644779, 64908, 64907]
| true
|
2021-05-12 10:56:20.740000
|
NM
| 2
| 42
|
mp-492
| null |
TiN
|
{'functional': 'PBE', 'labels': ['Ti_pv', 'N'], 'pot_type': 'paw'}
|
{'Ti': 1.0, 'N': 1.0}
|
GGA
|
mp-492
|
['mp-1000437', 'mp-1006912', 'mvc-13876', 'mp-492', 'mp-1057172', 'mp-1057185', 'mp-1057208', 'mp-1058302', 'mp-1058334', 'mp-1058311', 'mp-1058844', 'mp-1058812', 'mp-1058719', 'mp-1058731', 'mp-1058768', 'mp-1058795', 'mp-1059321', 'mp-1059405', 'mp-1059335', 'mp-1059364', 'mp-1059371', 'mp-1059381', 'mp-1060451', 'mp-1060512', 'mp-1060469', 'mp-1061088', 'mp-1061064', 'mp-1061129', 'mp-1440637', 'mp-1674200', 'mp-1793307', 'mp-1011627', 'mp-1595453', 'mp-1594449', 'mp-1058832', 'mp-1061120', 'mp-1057200', 'mp-1058325', 'mp-1059400', 'mp-1058755', 'mp-1060496', 'mp-1059351']
| 0.00026
|
{'Ti': 1.0, 'N': 1.0}
| 19.239321
|
[]
|
NM
| false
| 225
| 0
|
[0, 0]
| 0.000013
| 0.00026
| 0
| 0.00026
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-492.cif
| true
| null |
data/final/MP/graphs/N0.84Ti1-MP-mp-492-synth_doped.json
| 0
| true
|
m-3m
| 6
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 0
| 1
| 1
| false
|
H0.965Pd1
| 2
| 0.017812
| 2
| false
|
H1.93Pd2
|
H2Pd2
| 6.45
|
Other
| true
|
H49.109Pd50.891
|
H-Pd
| 2
|
Supercon
|
H0.965Pd1
|
MP-mp-1184548
|
H2Pd2
|
H-Pd
|
H50Pd50
|
P 63 m c
|
hexagonal
| 2.968136
| 2.968136
| 5.040799
|
data/final/MP/cifs/H0.965Pd1-MP-mp-1184548-synth_doped.cif
|
data/source/MP/raw/cifs/mp-1184548.cif
|
mp-1184548
| 0
| null |
2019-01-11 12:52:40.348000
| 9.276812
| null | null |
{'GGA': {'task_id': 'mp-1734957'}}
| 0
| 3.521133
| 520
| -17.477448
| -4.369362
|
{'tags': []}
| -17.477448
| -4.369362
| -0.083058
|
['bandstructure']
| true
|
[]
| true
|
2021-05-12 10:58:27.755000
|
NM
| 4
| 5
|
mp-1184548
| null |
HPd
|
{'functional': 'PBE', 'labels': ['H', 'Pd'], 'pot_type': 'paw'}
|
{'H': 1.0, 'Pd': 1.0}
|
GGA
|
mp-1184548
|
['mp-1184548', 'mp-1426775', 'mp-1734957', 'mp-1792734', 'mp-1612181']
| 0.000037
|
{'H': 2.0, 'Pd': 2.0}
| 38.458963
|
[]
|
NM
| false
| 186
| 0
|
[0, 0, 0, 0]
| 0.000002
| 0.000037
| 0
| 0.000074
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1184548.cif
| true
| null |
data/final/MP/graphs/H0.965Pd1-MP-mp-1184548-synth_doped.json
| 0
| true
|
6mm
| 0
| 5
| 0
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
Bi2Ca1Cu2Sr2O8
| 1
| 0
| 2
| false
|
Bi4Ca2Cu4Sr4O16
|
Bi4Ca2Cu4Sr4O16
| 88.25
|
Cuprate
| true
|
Bi13.333Ca6.667Cu13.333Sr13.333O53.333333333333336
|
Bi-Ca-Cu-Sr-O
| 5
|
Supercon
|
Bi2Ca1Sr2Cu2O8
|
MP-mp-1218930
|
Sr4Ca2Cu4Bi4O16
|
Bi-Ca-Cu-Sr-O
|
Bi13.333Ca6.667Cu13.333Sr13.333O53.333333333333336
|
C c c 2
|
orthorhombic
| 5.417115
| 5.472898
| 16.113989
|
data/final/MP/cifs/Bi2Ca1Cu2Sr2O8-MP-mp-1218930.cif
|
data/source/MP/raw/cifs/mp-1218930.cif
|
mp-1218930
| 0
| null |
2019-01-12 20:01:06.544000
| 6.266669
| null | null | null | 0.039252
| 4.517683
| 520
| -173.15021
| -5.771674
|
{'tags': []}
| -173.15021
| -5.771674
| -2.074957
|
[]
| false
|
[]
| true
|
2021-05-12 11:00:42.526000
|
NM
| 30
| 3
|
mp-1218930
|
oxide
|
Sr2CaCu2(BiO4)2
|
{'functional': 'PBE', 'labels': ['Sr_sv', 'Ca_sv', 'Cu_pv', 'Bi', 'O'], 'pot_type': 'paw'}
|
{'Sr': 2.0, 'Ca': 1.0, 'Cu': 2.0, 'Bi': 2.0, 'O': 8.0}
|
GGA
|
mp-1218930
|
['mp-1218930', 'mp-1359698', 'mp-1817714']
| 0.000112
|
{'Sr': 4.0, 'Ca': 2.0, 'Cu': 4.0, 'Bi': 4.0, 'O': 16.0}
| 470.797629
|
[]
|
NM
| false
| 37
| 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
| 0.000112
| 0
| 0.000223
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-1218930.cif
| false
| null |
data/final/MP/graphs/Bi2Ca1Cu2Sr2O8-MP-mp-1218930.json
| 0
| true
|
mm2
| 0
| 0
| 0
| 6
| 0
| 0
| 0
| 0
| 1
| 0
| 0
| 1
| false
|
Ca0.4La0.6Mn1O3
| 2
| 0.04
| 4
| false
|
Ca1.6La2.4Mn4O12
|
Ca2La2Mn4O12
| 0
|
Oxide
| true
|
Ca8La12Mn20O60
|
Ca-La-Mn-O
| 4
|
Supercon
|
La0.6Ca0.4Mn1O3
|
MP-mp-39689
|
Ca2La2Mn4O12
|
Ca-La-Mn-O
|
Ca10La10Mn20O60
|
P m n 21
|
orthorhombic
| 5.479104
| 5.528867
| 7.700679
|
data/final/MP/cifs/Ca0.4La0.6Mn1O3-MP-mp-39689-synth_doped.cif
|
data/source/MP/raw/cifs/mp-39689.cif
|
mp-39689
| 0
| null |
2013-11-18 12:40:04
| 5.479017
|
10.17188/1207686
|
@misc{osti_1207686,
author = "Persson, Kristin",
title = "Materials Data on CaLaMn2O6 (SG:31) 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 = "10.17188/1207686",
place = "United States",
year = "2016",
month = "4",
note = "An optional note"
}
|
{'GGA+U': {'task_id': 'mp-1683310'}}
| 0.105089
| 5.235727
| 520
| -150.490769
| -7.524538
|
{'tags': ['Lanthanum calcium manganate (III/IV)']}
| -150.490769
| -7.524538
| -2.774998
|
['xas', 'elasticity', 'bandstructure']
| true
|
[246478]
| true
|
2021-05-12 10:56:37.246000
|
FM
| 20
| 18
|
mp-39689
|
oxide
|
CaLaMn2O6
|
{'functional': 'PBE', 'labels': ['Ca_sv', 'La', 'Mn_pv', 'O'], 'pot_type': 'paw'}
|
{'Ca': 1.0, 'La': 1.0, 'Mn': 2.0, 'O': 6.0}
|
GGA+U
|
mp-39689
|
['mp-915443', 'mp-931300', 'mp-932172', 'mp-646643', 'mvc-11813', 'mp-41744', 'mp-41893', 'mp-39689', 'mp-40316', 'mp-1182471', 'mp-1182841', 'mp-1237098', 'mp-1293799', 'mp-1284909', 'mp-1281712', 'mp-1279698', 'mp-1369165', 'mp-1683310']
| 7.00051
|
{'Ca': 2.0, 'La': 2.0, 'Mn': 4.0, 'O': 12.0}
| 233.278464
|
[]
|
FM
| true
| 31
| 2
|
[0.0, 0.0, 0.0, 0.0, 3.6, 3.6, 3.6, 3.6, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0]
| 0.060018
| 7.00051
| 4
| 14.00102
|
MP
|
data/source/MP/cleaned/cifs/MP-mp-39689.cif
| true
| null |
data/final/MP/graphs/Ca0.4La0.6Mn1O3-MP-mp-39689-synth_doped.json
| 0
| true
|
mm2
| 0
| 0
| 0
| 6
| 0
| 0
| 0
| 1
| 0
| 0
| 0
| 1
| false
|
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