entry_id int64 1.6k 2.2M | calculation_id int64 2.45k 5.82M | structure_id int64 40.9k 10.7M |
|---|---|---|
1,603 | 1,332,179 | 2,010,321 |
1,604 | 1,332,180 | 2,010,323 |
1,605 | 1,228,803 | 1,771,058 |
1,606 | 1,292,017 | 1,926,947 |
1,607 | 1,341,376 | 2,010,502 |
1,608 | 1,341,365 | 2,010,485 |
1,609 | 27,588 | 59,945 |
1,610 | 1,230,677 | 1,772,750 |
1,611 | 1,341,653 | 2,010,921 |
1,612 | 1,332,133 | 2,010,325 |
1,613 | 1,289,735 | 1,925,231 |
1,614 | 681,121 | 1,077,303 |
1,615 | 1,341,418 | 2,010,723 |
1,616 | 27,664 | 59,925 |
1,617 | 1,284,699 | 1,921,707 |
1,618 | 379,412 | 693,180 |
1,619 | 146,094 | 181,465 |
1,620 | 143,821 | 180,233 |
1,621 | 1,341,906 | 2,011,030 |
1,622 | 146,033 | 181,312 |
1,623 | 1,226,714 | 1,769,171 |
1,624 | 28,566 | 56,345 |
1,626 | 1,227,972 | 1,769,638 |
1,627 | 1,293,990 | 1,928,782 |
1,628 | 1,341,196 | 2,010,344 |
1,629 | 1,341,459 | 2,010,706 |
1,630 | 32,568 | 63,018 |
1,631 | 1,227,916 | 1,771,439 |
1,632 | 1,335,471 | 2,010,347 |
1,633 | 28,598 | 56,377 |
1,634 | 149,650 | 184,564 |
1,635 | 1,301,229 | 1,967,349 |
1,636 | 1,341,530 | 2,010,794 |
1,637 | 1,341,385 | 2,010,505 |
1,638 | 846,043 | 1,284,883 |
1,639 | 1,292,062 | 1,926,978 |
1,640 | 1,341,315 | 2,010,438 |
1,641 | 19,886 | 49,149 |
1,642 | 1,230,737 | 1,775,639 |
1,643 | 1,341,290 | 2,010,421 |
1,644 | 1,342,024 | 2,011,637 |
1,645 | 1,341,336 | 2,010,461 |
1,646 | 143,848 | 180,205 |
1,647 | 1,320,840 | 1,987,797 |
1,648 | 1,301,206 | 1,967,326 |
1,649 | 1,230,424 | 1,919,375 |
1,650 | 1,341,342 | 2,010,474 |
1,651 | 1,301,230 | 1,967,350 |
1,652 | 800,498 | 1,229,253 |
1,653 | 27,649 | 60,686 |
1,654 | 5,199,811 | 9,749,233 |
1,655 | 149,693 | 184,601 |
1,656 | 1,294,146 | 1,928,657 |
1,657 | 1,294,944 | 1,929,112 |
1,658 | 20,086 | 178,486 |
1,659 | 143,671 | 180,207 |
1,660 | 18,905 | 48,697 |
1,661 | 149,665 | 184,421 |
1,662 | 1,342,705 | 2,032,491 |
1,663 | 27,648 | 59,922 |
1,664 | 1,292,079 | 1,926,985 |
1,665 | 1,301,207 | 1,967,327 |
1,666 | 1,280,431 | 1,921,171 |
1,667 | 1,341,735 | 2,010,865 |
1,668 | 149,682 | 184,716 |
1,669 | 143,720 | 180,260 |
1,670 | 20,069 | 48,920 |
1,671 | 1,342,329 | 2,011,428 |
1,672 | 682,637 | 1,113,065 |
1,673 | 1,341,744 | 2,010,905 |
1,674 | 1,341,402 | 2,010,515 |
1,675 | 28,811 | 56,613 |
1,676 | 149,666 | 184,319 |
1,677 | 1,341,828 | 2,011,026 |
1,678 | 28,827 | 56,627 |
1,679 | 1,350,356 | 2,026,136 |
1,680 | 1,342,140 | 2,011,473 |
1,681 | 1,341,476 | 2,010,598 |
1,682 | 1,151,642 | 1,769,243 |
1,683 | 146,777 | 183,483 |
1,684 | 1,332,114 | 2,010,576 |
1,685 | 1,332,145 | 2,010,577 |
1,686 | 149,632 | 184,565 |
1,687 | 5,199,481 | 9,749,520 |
1,688 | 1,332,159 | 2,010,578 |
1,689 | 1,341,656 | 2,010,754 |
1,690 | 1,342,038 | 2,011,127 |
1,691 | 147,816 | 182,119 |
1,692 | 1,341,781 | 2,010,943 |
1,693 | 1,341,531 | 2,010,660 |
1,694 | 1,341,532 | 2,010,665 |
1,695 | 1,341,492 | 2,010,609 |
1,696 | 18,904 | 49,106 |
1,697 | 20,331 | 49,220 |
1,698 | 1,332,184 | 2,010,603 |
1,699 | 34,759 | 65,376 |
1,700 | 16,587 | 47,224 |
1,701 | 1,341,831 | 2,010,937 |
1,702 | 1,341,635 | 2,010,770 |
1,703 | 1,278,253 | 1,909,512 |
OQMD
Structures and energies of the Open Quantum Materials Database, preprocessed for machine learning.
| File | Structures | Atoms | Content |
|---|---|---|---|
all.hdf5 |
1,407,269 | 14,266,404 | one structure per entry of OQMD v1.8 |
unique.hdf5 |
1,259,553 | 13,089,068 | same, without the entries marked as duplicates in OQMD |
all_index.parquet, unique_index.parquet |
OQMD entry_id, calculation_id and structure_id of each row of the file above |
||
oqmd.tar.gz, dump.py |
1,021,320 | 7,117,087 | older export (2024) in another layout, kept unchanged, see the end of this page |
Structures have 1 to 312 atoms (median 6).
How structures are selected
Source: the SQL dump of OQMD v1.8 (qmdb__v1_8__022026.sql.gz, February 2026), 1,407,285 entries.
For each entry, one calculation is selected:
- its output structure must be consistent: the number of atoms declared for the structure
equals its number of rows in the
atomstable (47,859 of 8,374,305 structures are not); - the calculation is converged, its label starts with
staticorstandard, and does not end withlda; - among those, the one with the lowest energy per atom is kept (lowest calculation id when equal).
1,407,269 entries have such a calculation. Nothing else is filtered in all.hdf5.
unique.hdf5 groups each entry with the entry it duplicates according to OQMD
(entries.duplicate_of_id) and keeps the entry with the lowest energy per atom of each group;
when energies are exactly equal the original entry is kept. 147,716 entries are removed this
way. Duplicates that OQMD does not mark are not removed.
Labels
| Field | Source | Meaning |
|---|---|---|
total_energy |
calculations.energy_pa × number of atoms |
DFT total energy of the cell in eV |
formation_energy_per_atom |
formation_energies.delta_e (fit standard) |
formation energy in eV/atom |
energy_above_hull |
formation_energies.stability (fit standard) |
distance to the convex hull in eV/atom, stored as in OQMD: negative for phases below the hull |
band_gap |
calculations.band_gap |
band gap in eV, NaN for 3,155 structures of all.hdf5 |
Labels are not cleaned. all.hdf5 contains unphysical values from failed calculations: 559
structures with a positive total energy (up to +704 eV/atom), 668 with a stability above
5 eV/atom, and one negative band gap. Filter them for training.
all.hdf5 |
unique.hdf5 |
|
|---|---|---|
| stability ≤ 0 | 97,228 | 96,246 |
| stability ≤ 0.1 eV/atom | 458,906 | 402,102 |
Format
Flat concatenated arrays:
| Dataset | Shape | Type | Content |
|---|---|---|---|
lattice |
(n_struct, 3, 3) | float32 | lattice vectors as rows, in angstrom |
num_atoms |
(n_struct,) | int64 | number of atoms of each structure |
ptr |
(n_struct,) | int64 | index of the first atom of each structure in x and z |
x |
(n_atoms, 3) | float32 | fractional coordinates in [0, 1) |
z |
(n_atoms,) | int64 | atomic numbers |
total_energy, formation_energy_per_atom, energy_above_hull, band_gap |
(n_struct,) | float32 | labels, NaN when unknown |
The lattice is rebuilt from cell lengths and angles, so it is in the standard orientation
(first vector along x). Fractional coordinates are wrapped into the cell. The batch array is
an artefact of the writer and is not used when reading. Structures are ordered by OQMD entry
id; row i of an index file describes structure i.
Usage
from pycrystalgen.data import HDF5Dataset
dataset = HDF5Dataset.from_hub("materials-toolkits/oqmd", "unique.hdf5")
structures = dataset[:32] # batched Structures
Processing and checks
Built with pycrystalgen (scripts/build_oqmd.py): the dump is read as a stream without a MySQL
server, the tables are extracted, structures are written to CIF then preprocessed to HDF5.
Every structure of both files was compared with the tables of the dump: number of atoms, elements, fractional coordinates, lattice and the four labels.
Older export (oqmd.tar.gz)
oqmd.tar.gz holds a 2024 export produced by dump.py from an earlier version of the database,
in the layout of materials-toolkit (data.hdf5, batching.json). It contains 1,021,320
structures with an energy per atom and an energy above the hull recomputed by materials-toolkit
(not OQMD's stability). The selection rules above follow the ones of dump.py. 1,007,099 of its
entries are also in all.hdf5; 1,005,090 of them have the same selected structure.
References
- J. E. Saal, S. Kirklin, M. Aykol, B. Meredig and C. Wolverton, Materials Design and Discovery with High-Throughput Density Functional Theory: The Open Quantum Materials Database (OQMD), JOM 65, 1501 (2013).
- S. Kirklin et al., The Open Quantum Materials Database (OQMD): assessing the accuracy of DFT formation energies, npj Computational Materials 1, 15010 (2015).
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