History#
- 2026.10.3.1 – The finite-difference Hessian as separate calculations, on this machine or a cluster
When the job’s calculations go to a cluster queue and the program can run separate calculations (ORCA, MOPAC), the Hessian is the finite difference of the gradients, run there as 6N calculations; nothing is started on the job’s own machine, where the program may not be installed.
Otherwise the analytic Hessian is used when the program’s MDI engine has one, and ORCA’s model chemistry now says so without ORCA being started to ask. Failing that, ORCA’s finite-difference calculations run several at a time on this machine; MOPAC, xTB and MLFFs use the warm MDI engine as before.
Rerunning the job reuses finished finite-difference calculations.
If the program is not installed on this machine, the separate calculations are used and the output says so; other failures to start the engine stop the step with the reason rather than quietly switching method.
Requires seamm-exec 2026.10.3 or later.
- 2026.10.3 – Bugfix: the Hessian used the program’s method name and default basis
The MDI engine for the Hessian was launched with the model chemistry’s method name alone, so ORCA ran def2-SVP whatever basis was chosen, and a functional whose name the Model Chemistry step had to alter was not recognized. It now gets the program’s own keyword and the chosen basis (with model_chemistry_step 2026.10.3).
The shared CI now runs on uv:
devtools/conda-envs/test_env.yamlis removed, sorequirements.txtis the one dependency list.
- 2026.7.15 – Initial release
Generates an ensemble of displaced structures by normal-mode sampling of a molecule’s Hessian, for building machine-learned-force-field training sets and similar uses.
Amplitudes follow the quantum (Wigner) distribution by default, so stiff modes such as O-H stretches get the real zero-point spread that classical 300 K sampling misses; classical-thermal and ground-state (0 K) distributions are also available.
The Hessian is obtained from the Model Chemistry defined earlier in the flowchart, over MDI: the analytic Hessian when the engine provides one, otherwise a finite-difference of the forces over the resident engine.
A temperature, per-mode selection, amplitude cap, and harmonic-energy outlier rejection are all controllable, and the random seed can be fixed for reproducible ensembles.
Off-minimum geometries are allowed with a warning, so a transition state is sampled along its real modes while its imaginary reaction coordinate is left alone.
Each generated structure records its predicted harmonic energy and the per-mode normal-coordinate displacement as properties, for downstream filtering and analysis.