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