Atomistic workflows

An atomistic number is defined only together with its code, units, convergence parameters and stopping criteria; a "DFT energy" without k-mesh and cutoff cannot be reproduced.

ASE

1. Atoms(symbols, positions, cell, pbc); ase.io.read and write convert between formats (read("traj.xyz", index=":") for all frames). Internal units are eV and angstrom; ase.units supplies fs, kB, Hartree and Bohr for conversion (the native time unit is about 10.18 fs, so always multiply by units.fs). Attach a calculator with atoms.calc = ... (EMT, ase.calculators.vasp.Vasp, espresso.Espresso, lammpslib.LAMMPSlib, a machine-learned potential), then get_potential_energy(), get_forces(), get_stress() (eV per cubic angstrom).
2. Relaxation: from ase.optimize import BFGS, LBFGS, FIRE, then opt = BFGS(atoms, trajectory="opt.traj", logfile="opt.log") and opt.run(fmax=0.01, steps=500). fmax is the largest force on any atom in eV per angstrom: 0.05 is loose, 0.01 standard, 0.001 for phonons. Relax the cell with FrechetCellFilter from ase.filters wrapped around the atoms; fix atoms with FixAtoms. Check that opt.run returned converged rather than exhausting steps.
3. MD: MaxwellBoltzmannDistribution(atoms, temperature_K=300) and Stationary(atoms), then Langevin(atoms, 1.0 * units.fs, temperature_K=300, friction=0.01 / units.fs) or NVTBerendsen, NPT; dyn.run(steps) with a trajectory attached; record the seed.

pymatgen

4. Structure.from_file("POSCAR") or a CIF; structure.to(filename="out.cif"). Symmetry via SpacegroupAnalyzer(structure, symprec=0.01, angle_tolerance=5) with get_space_group_symbol() and get_conventional_standard_structure(); symprec changes the answer (0.01 angstrom strict, 0.1 loose), so report it. Kpoints.automatic_density(structure, kppa=1000) sets k-mesh density per reciprocal atom. Vasprun("vasprun.xml") exposes final_energy, converged_electronic and converged_ionic; read both flags. AseAtomsAdaptor bridges to ASE.
5. Materials Project: from mp_api.client import MPRester, then mpr.materials.summary.search(formula="Fe2O3", fields=[...]) with fields such as material_id, structure, energy_above_hull and band_gap. Database energies carry their own functional and correction scheme; never mix them with raw energies from your own runs without applying the same corrections. Record the database release and the material_id.

Convergence

6. Plane-wave DFT: converge the quantity you report (total energy per atom, an energy difference, forces, stress) against cutoff (VASP ENCUT in eV, at least 1.3 x ENMAX for stress and cell relaxation; Quantum ESPRESSO ecutwfc in Ry with ecutrho 4 to 12 times larger) and against k-mesh (Monkhorst-Pack or Gamma-centred, density stated), to a criterion such as 1 meV per atom. Metals need smearing (ISMEAR, SIGMA; occupations="smearing", degauss) and denser meshes. Record pseudopotential or PAW set and version, functional, DFT+U values, dispersion correction, spin initialization, electronic (EDIFF, conv_thr) and ionic (EDIFFG, forc_conv_thr) thresholds. Slabs need at least 10 to 15 angstrom of vacuum and a dipole correction; defects need a supercell-size test.
7. MD: timestep at most 1 fs with explicit hydrogens, 2 fs with bond constraints, 0.5 fs for high temperatures or very light atoms; validate by energy drift in NVE. Equilibrate NVT then NPT before production; check the observable against run length (block averaging or autocorrelation) and against system size.

LAMMPS and GROMACS

8. LAMMPS: the units command (metal, real, lj, si) fixes every other unit in the input, so state it first. Skeleton: atom_style, boundary p p p, read_data, pair_style and pair_coeff, timestep 0.001 (in the chosen time unit), velocity all create 300 4928459 dist gaussian (the seed is part of the record), fix 1 all nvt temp 300 300 0.1, thermo_style custom step temp pe etotal press vol, dump, run. minimize 1e-8 1e-10 10000 100000 gives energy tolerance, force tolerance, max iterations and max force evaluations; report which criterion stopped it. write_restart and read_restart continue a run; log.lammps is the evidence.
9. GROMACS (nm, ps, kJ/mol, bar): gmx pdb2gmx -ff amber99sb-ildn -water tip3p, gmx editconf -c -d 1.0 -bt dodecahedron, gmx solvate, gmx grompp, gmx genion -neutral -conc 0.15. Minimization .mdp: integrator = steep, emtol = 1000.0 (kJ mol^-1 nm^-1). Production: integrator = md, dt = 0.002, constraints = h-bonds, cutoff-scheme = Verlet, coulombtype = PME, rcoulomb = 1.0, rvdw = 1.0, tcoupl = V-rescale, tau_t = 0.1, ref_t = 300, pcoupl = C-rescale, ref_p = 1.0, compressibility = 4.5e-5. Restart with gmx mdrun -cpi state.cpt; analyze with gmx energy, gmx rms, gmx trjconv.

Units per code

Reproducible inputs

• Archive the exact inputs (INCAR, KPOINTS, POSCAR, POTCAR titles and hashes; in.lammps and data files; every .mdp and topol.top), seeds, a run.sh, code versions (lmp -h, gmx --version, ase.__version__) and the raw outputs the numbers came from (OUTCAR, vasprun.xml, log.lammps, .edr).
• After any format conversion, check that atom counts, cell and composition survived.
• State functional, pseudopotentials, cutoffs, k-mesh, smearing, thresholds, force field, water model, timestep, ensemble, T and P, run length and equilibration discarded.

Sources

• ASE documentation (units, optimizers, molecular dynamics): https://ase-lib.org/
• pymatgen documentation: https://pymatgen.org/
• Materials Project API documentation: https://docs.materialsproject.org/
• LAMMPS manual (units, minimize, fix nvt): https://docs.lammps.org/
• GROMACS reference manual and .mdp options: https://manual.gromacs.org/current/
• VASP wiki (ENCUT, KPOINTS, EDIFFG): https://www.vasp.at/wiki/
• Quantum ESPRESSO pw.x input description: https://www.quantum-espresso.org/Doc/INPUT_PW.html
• Lejaeghere et al. (2016), Reproducibility in density functional theory calculations of solids, Science 351, aad3000: https://doi.org/10.1126/science.aad3000