sync code from github@2603923ed5412e943ea2128d491e9c54f907332f
Browse files- magnet/inference.py +127 -50
- magnet/pyproject.toml +1 -1
- magnet/run_magnet.py +6 -8
- tests/test_magnet.py +72 -0
magnet/inference.py
CHANGED
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@@ -138,29 +138,35 @@ def _predict_once(model_H, model_C, solute_atomic_numbers, geometry, atomic_numb
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return y_pred_combined
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def _predict_batch(model_H, model_C,
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"""
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n = len(
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combined = [None] * n
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for atom_type in ['H', 'C']:
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data_list = []
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for
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data = yield_data(
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solute_atomic_numbers = solute_atomic_numbers,
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geometries =
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atomic_numbers = atomic_numbers,
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shieldings = None,
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N_atoms_per_solvent =
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solvent_distance_threshold =
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atom_type = atom_type,
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)
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# PyG owns `batch` on a Batch, and the model rebuilds `natoms` from it; keeping the
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@@ -191,8 +197,37 @@ def _predict_batch(model_H, model_C, solute_atomic_numbers, geometries, atomic_n
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return combined
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def predict_shieldings(model_H, model_C, solute_atomic_numbers, geometry, atomic_numbers = None, N_atoms_per_solvent = None, solvent_distance_threshold = None, device = 'cpu', n_passes = 1, mirror_average = False, symmetrize = None, max_batch_graphs = MAX_BATCH_GRAPHS):
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-
"""Predict 1H/13C shieldings for the solute atoms.
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A single forward pass is NOT deterministic: each edge picks a random local
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reference frame (eqV2/edge_rot_mat.py), so with a finite spherical-harmonic grid
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@@ -206,47 +241,89 @@ def predict_shieldings(model_H, model_C, solute_atomic_numbers, geometry, atomic
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spurious error.
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The passes are independent of one another, so they are run as one batch per head rather than
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one forward pass each
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solvated system at a high n_passes does not have to fit in memory all at once. The answer does
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not depend on it.
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`symmetrize` is the old name for `mirror_average` and still works, with a DeprecationWarning.
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"""
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mirror_average = resolve_mirror_average(mirror_average, symmetrize, "predict_shieldings")
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solute_atomic_numbers = np.asarray(solute_atomic_numbers)
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if atomic_numbers is None:
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atomic_numbers = solute_atomic_numbers
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else:
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# coerce so the element comparisons in yield_data (atomic_numbers == 1) stay array-wise;
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# a bare Python list would compare to a scalar False and silently mis-mask
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atomic_numbers = np.asarray(atomic_numbers)
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# system, which for MagNET-x includes the solvent atoms).
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unsupported = sorted(set(np.unique(atomic_numbers).tolist()) - SUPPORTED_ELEMENTS)
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if unsupported:
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raise ValueError(
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f"MagNET supports only the elements {sorted(SUPPORTED_ELEMENTS)} "
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f"(H, C, N, O, F, S, Cl); the input contains unsupported atomic numbers {unsupported}. "
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f"Exclude molecules with these elements before predicting.")
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# atleast_1d keeps a one-atom solute a (1,) array instead of a 0-d scalar after the per-pass squeeze
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return np.atleast_1d(np.mean(
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return y_pred_combined
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def _predict_batch(model_H, model_C, graphs, device):
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"""Run every graph in `graphs` through both heads, one forward pass per head.
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Each entry of `graphs` is one geometry to predict for, as
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`(solute_atomic_numbers, geometry, atomic_numbers, N_atoms_per_solvent,
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solvent_distance_threshold)`. They need not be the same molecule: the graphs are concatenated
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into a single torch_geometric Batch, and the answers are split apart again by which graph each
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atom came from, so molecules of different sizes batch together as readily as repeated passes
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of one.
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The model recomputes `natoms` from `batch.batch`, so the per-graph `batch` and `natoms` that
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yield_data writes are dropped before concatenating and PyG assigns its own.
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`unique_molecule_batch` rides along unread: yield_data consumes it for solvent filtering
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before this point, and no model looks at it, so nothing has to be offset across graphs.
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Returns one (n_solute,) array per entry, in the order given.
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"""
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n = len(graphs)
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combined = [None] * n
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for atom_type in ['H', 'C']:
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data_list = []
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for solute_atomic_numbers, geometry, atomic_numbers, per_solvent, threshold in graphs:
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data = yield_data(
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solute_atomic_numbers = solute_atomic_numbers,
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geometries = geometry,
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atomic_numbers = atomic_numbers,
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shieldings = None,
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N_atoms_per_solvent = per_solvent if per_solvent is not None else 3,
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solvent_distance_threshold = threshold,
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atom_type = atom_type,
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)
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# PyG owns `batch` on a Batch, and the model rebuilds `natoms` from it; keeping the
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return combined
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def _check_elements(atomic_numbers):
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"""Refuse a system holding an element MagNET was never trained on.
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MagNET was only ever trained on SUPPORTED_ELEMENTS. On anything else it would emit a confident
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but meaningless prediction, so refuse it rather than let bad numbers through (validate the full
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system, which for MagNET-x includes the solvent atoms).
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Raises:
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ValueError: naming every atomic number that is not supported.
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"""
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unsupported = sorted(set(np.unique(atomic_numbers).tolist()) - SUPPORTED_ELEMENTS)
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if unsupported:
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raise ValueError(
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f"MagNET supports only the elements {sorted(SUPPORTED_ELEMENTS)} "
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f"(H, C, N, O, F, S, Cl); the input contains unsupported atomic numbers {unsupported}. "
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f"Exclude molecules with these elements before predicting.")
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def _geometries_of(geometry, mirror_average, n_passes):
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"""Say which geometries one prediction runs over, the mirror image and the passes included."""
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geometry = np.asarray(geometry, dtype=float)
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geometries = [geometry]
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if mirror_average:
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reflected = geometry.copy()
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reflected[..., 0] = -reflected[..., 0] # mirror across the yz-plane (an improper rotation)
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geometries.append(reflected)
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return [geom for geom in geometries for _ in range(n_passes)]
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def predict_shieldings(model_H, model_C, solute_atomic_numbers, geometry, atomic_numbers = None, N_atoms_per_solvent = None, solvent_distance_threshold = None, device = 'cpu', n_passes = 1, mirror_average = False, symmetrize = None, max_batch_graphs = MAX_BATCH_GRAPHS):
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"""Predict 1H/13C shieldings for the solute atoms of one molecule.
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A single forward pass is NOT deterministic: each edge picks a random local
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reference frame (eqV2/edge_rot_mat.py), so with a finite spherical-harmonic grid
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spurious error.
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The passes are independent of one another, so they are run as one batch per head rather than
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one forward pass each. `predict_shieldings_batch` batches whole molecules together as well,
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and is what to call for more than one.
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`symmetrize` is the old name for `mirror_average` and still works, with a DeprecationWarning.
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"""
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mirror_average = resolve_mirror_average(mirror_average, symmetrize, "predict_shieldings")
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return predict_shieldings_batch(
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model_H, model_C, [solute_atomic_numbers], [geometry],
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atomic_numbers_list = None if atomic_numbers is None else [atomic_numbers],
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N_atoms_per_solvent = N_atoms_per_solvent,
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solvent_distance_threshold = solvent_distance_threshold, device = device,
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n_passes = n_passes, mirror_average = mirror_average,
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max_batch_graphs = max_batch_graphs)[0]
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def predict_shieldings_batch(model_H, model_C, solute_atomic_numbers_list, geometries_list, atomic_numbers_list = None, N_atoms_per_solvent = None, solvent_distance_threshold = None, device = 'cpu', n_passes = 1, mirror_average = False, symmetrize = None, max_batch_graphs = MAX_BATCH_GRAPHS):
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"""Predict 1H/13C shieldings for many molecules at once.
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Every molecule's passes, and its mirror image where `mirror_average` is set, go through as one
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batch rather than one forward pass each, and molecules share those batches with one another.
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A 31-atom graph occupies very little of a GPU, so what costs the time is the number of forward
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passes and not the size of any one of them: batching across molecules is what fills the card.
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The molecules need not be the same size or the same shape. Each answer is split out by which
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graph its atoms came from, so a list of molecules comes back as a list of per-atom arrays in
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the order given, exactly as calling `predict_shieldings` on each would have.
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Args:
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model_H, model_C: the 1H and 13C models to run.
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solute_atomic_numbers_list: one array of solute atomic numbers per molecule.
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geometries_list: one (n, 3) coordinate array per molecule, in the same order.
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atomic_numbers_list: the whole system per molecule where it differs from the solute (the
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explicit-solvent path), or None where every system is its own solute.
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N_atoms_per_solvent, solvent_distance_threshold: the explicit-solvent options, applied to
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every molecule.
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device: where to run.
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n_passes: how many forward passes to average per geometry.
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mirror_average: whether to average over the mirror image as well.
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symmetrize: the old name for `mirror_average`, which still works and warns.
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max_batch_graphs: how many graphs go through one forward pass at most. It bounds memory
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and changes no answer.
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Returns:
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One (n_solute,) array per molecule, in the order given.
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Raises:
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ValueError: a molecule holds an element MagNET was not trained on, or the lists differ in
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length.
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"""
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mirror_average = resolve_mirror_average(mirror_average, symmetrize, "predict_shieldings_batch")
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if len(solute_atomic_numbers_list) != len(geometries_list):
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raise ValueError(
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f"got {len(solute_atomic_numbers_list)} solutes and {len(geometries_list)} geometries; "
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f"they name the same molecules and must be the same length")
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if atomic_numbers_list is not None and len(atomic_numbers_list) != len(geometries_list):
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raise ValueError(
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f"got {len(atomic_numbers_list)} systems and {len(geometries_list)} geometries; "
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f"they name the same molecules and must be the same length")
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# every graph to run, and which molecule each one belongs to
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graphs, molecule_of_graph = [], []
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for i, (solute, geometry) in enumerate(zip(solute_atomic_numbers_list, geometries_list)):
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solute = np.asarray(solute)
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if atomic_numbers_list is None:
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whole = solute
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else:
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# coerce so the element comparisons in yield_data (atomic_numbers == 1) stay array-wise;
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# a bare Python list would compare to a scalar False and silently mis-mask
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whole = np.asarray(atomic_numbers_list[i])
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_check_elements(whole)
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for geom in _geometries_of(geometry, mirror_average, n_passes):
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graphs.append((solute, geom, whole, N_atoms_per_solvent, solvent_distance_threshold))
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molecule_of_graph.append(i)
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per_graph = []
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for start in range(0, len(graphs), max_batch_graphs):
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per_graph.extend(_predict_batch(model_H, model_C, graphs[start:start + max_batch_graphs],
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device))
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# average each molecule's own passes, and nothing else's
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gathered = [[] for _ in geometries_list]
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for prediction, molecule in zip(per_graph, molecule_of_graph):
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gathered[molecule].append(prediction)
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# atleast_1d keeps a one-atom solute a (1,) array instead of a 0-d scalar after the per-pass squeeze
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return [np.atleast_1d(np.mean(passes, axis=0)) for passes in gathered]
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magnet/pyproject.toml
CHANGED
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[project]
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name = "magnet-nmr"
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version = "0.2.
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description = "MagNET: equivariant neural networks for NMR chemical-shift (shielding) prediction"
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readme = {text = "MagNET: equivariant neural networks for NMR chemical-shift (shielding) prediction. Models, datasets, install instructions, and usage examples are at https://github.com/ekwan/MagNET", content-type = "text/markdown"}
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requires-python = ">=3.9"
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[project]
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name = "magnet-nmr"
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version = "0.2.1"
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description = "MagNET: equivariant neural networks for NMR chemical-shift (shielding) prediction"
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readme = {text = "MagNET: equivariant neural networks for NMR chemical-shift (shielding) prediction. Models, datasets, install instructions, and usage examples are at https://github.com/ekwan/MagNET", content-type = "text/markdown"}
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requires-python = ">=3.9"
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magnet/run_magnet.py
CHANGED
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import torch
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from magnet.model import MagNET_Lightning
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from magnet.inference import predict_shieldings,
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MODEL_CHECKPOINTS = {
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# foundation model (predicts the gas-phase shielding the rovibrational/QCD analysis builds on)
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device = _default_device()
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model_H = load_model_to_device(MODEL_CHECKPOINTS[key_H], device, checkpoints_dir=checkpoints_dir)
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model_C = load_model_to_device(MODEL_CHECKPOINTS[key_C], device, checkpoints_dir=checkpoints_dir)
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for
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model_H, model_C, solute_atomic_numbers=atomic_numbers, geometry=geometry,
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device=device, n_passes=n_passes, mirror_average=mirror_average, **predict_kwargs).squeeze()))
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return out
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def compute_MagNET_foundation_shieldings(atomic_numbers_list, geometries_list,
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import torch
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from magnet.model import MagNET_Lightning
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from magnet.inference import (predict_shieldings, predict_shieldings_batch,
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resolve_mirror_average)
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MODEL_CHECKPOINTS = {
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# foundation model (predicts the gas-phase shielding the rovibrational/QCD analysis builds on)
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device = _default_device()
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model_H = load_model_to_device(MODEL_CHECKPOINTS[key_H], device, checkpoints_dir=checkpoints_dir)
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model_C = load_model_to_device(MODEL_CHECKPOINTS[key_C], device, checkpoints_dir=checkpoints_dir)
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# one batch across the molecules as well as their passes, rather than a call per molecule
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return [np.atleast_1d(one.squeeze()) for one in predict_shieldings_batch(
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model_H, model_C, list(atomic_numbers_list), list(geometries_list),
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| 105 |
+
device=device, n_passes=n_passes, mirror_average=mirror_average, **predict_kwargs)]
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| 106 |
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| 107 |
|
| 108 |
def compute_MagNET_foundation_shieldings(atomic_numbers_list, geometries_list,
|
tests/test_magnet.py
CHANGED
|
@@ -345,3 +345,75 @@ def test_one_atom_solute_stays_one_dimensional():
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|
| 345 |
[-0.629, 0.629, -0.629], [0.629, -0.629, -0.629]])
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| 346 |
out = predict_shieldings(mH, mC, solute_atomic_numbers=z, geometry=xyz, device=dev, n_passes=2)
|
| 347 |
assert out.ndim == 1 and out.shape == (5,)
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| 345 |
[-0.629, 0.629, -0.629], [0.629, -0.629, -0.629]])
|
| 346 |
out = predict_shieldings(mH, mC, solute_atomic_numbers=z, geometry=xyz, device=dev, n_passes=2)
|
| 347 |
assert out.ndim == 1 and out.shape == (5,)
|
| 348 |
+
|
| 349 |
+
|
| 350 |
+
# =====================================================================
|
| 351 |
+
# batching across molecules
|
| 352 |
+
# =====================================================================
|
| 353 |
+
|
| 354 |
+
def test_batch_refuses_mismatched_lists():
|
| 355 |
+
"""Two lists naming the same molecules have to be the same length."""
|
| 356 |
+
from magnet.inference import predict_shieldings_batch
|
| 357 |
+
z = np.array([6, 1, 1, 1, 1])
|
| 358 |
+
xyz = np.zeros((5, 3))
|
| 359 |
+
with pytest.raises(ValueError, match="same length"):
|
| 360 |
+
predict_shieldings_batch(None, None, [z, z], [xyz])
|
| 361 |
+
with pytest.raises(ValueError, match="same length"):
|
| 362 |
+
predict_shieldings_batch(None, None, [z], [xyz], atomic_numbers_list=[z, z])
|
| 363 |
+
|
| 364 |
+
|
| 365 |
+
def test_batch_refuses_unsupported_element():
|
| 366 |
+
"""A molecule out of vocabulary is refused before any model runs, as the single path does."""
|
| 367 |
+
from magnet.inference import predict_shieldings_batch
|
| 368 |
+
good = np.array([6, 1, 1, 1, 1])
|
| 369 |
+
bad = np.array([15, 1, 1, 1]) # phosphorus
|
| 370 |
+
with pytest.raises(ValueError, match="unsupported atomic numbers"):
|
| 371 |
+
predict_shieldings_batch(None, None, [good, bad], [np.zeros((5, 3)), np.zeros((4, 3))])
|
| 372 |
+
|
| 373 |
+
|
| 374 |
+
@pytest.mark.skipif(not os.path.exists(CKPT), reason="released MagNET-Zero checkpoints not present")
|
| 375 |
+
def test_batch_matches_one_at_a_time():
|
| 376 |
+
"""Molecules batched together answer as they do apart, whatever their sizes.
|
| 377 |
+
|
| 378 |
+
The molecules are deliberately of two different atom counts, since what splits the answers
|
| 379 |
+
apart is which graph each atom came from and not any assumption that they match.
|
| 380 |
+
"""
|
| 381 |
+
from magnet.inference import predict_shieldings_batch
|
| 382 |
+
dev = "cpu"
|
| 383 |
+
mH = MagNET_Lightning.load_from_checkpoint(os.path.join(CKPT, "MagNET-Zero_1H.ckpt"), map_location=dev).eval()
|
| 384 |
+
mC = MagNET_Lightning.load_from_checkpoint(os.path.join(CKPT, "MagNET-Zero_13C.ckpt"), map_location=dev).eval()
|
| 385 |
+
methane_z = np.array([6, 1, 1, 1, 1])
|
| 386 |
+
methane_xyz = np.array([[0., 0., 0.], [0.629, 0.629, 0.629], [-0.629, -0.629, 0.629],
|
| 387 |
+
[-0.629, 0.629, -0.629], [0.629, -0.629, -0.629]])
|
| 388 |
+
ethanol_z = np.array([6, 6, 8, 1, 1, 1, 1, 1, 1])
|
| 389 |
+
ethanol_xyz = np.array([[1.17, -0.24, 0.], [0., 0.55, 0.], [-1.16, -0.25, 0.],
|
| 390 |
+
[2.08, 0.37, 0.], [1.17, -0.87, 0.89], [1.17, -0.87, -0.89],
|
| 391 |
+
[0.01, 1.19, 0.88], [0.01, 1.19, -0.88], [-1.90, 0.35, 0.]])
|
| 392 |
+
zs, xyzs = [methane_z, ethanol_z], [methane_xyz, ethanol_xyz]
|
| 393 |
+
kw = dict(device=dev, n_passes=30, mirror_average=True)
|
| 394 |
+
apart = [predict_shieldings(mH, mC, solute_atomic_numbers=z, geometry=x, **kw)
|
| 395 |
+
for z, x in zip(zs, xyzs)]
|
| 396 |
+
together = predict_shieldings_batch(mH, mC, zs, xyzs, **kw)
|
| 397 |
+
assert [one.shape for one in together] == [one.shape for one in apart]
|
| 398 |
+
for a, b in zip(apart, together):
|
| 399 |
+
# both average the same frame noise away, so they agree to well inside it
|
| 400 |
+
assert np.max(np.abs(a - b)) < 0.05
|
| 401 |
+
|
| 402 |
+
|
| 403 |
+
@pytest.mark.skipif(not os.path.exists(CKPT), reason="released MagNET-Zero checkpoints not present")
|
| 404 |
+
def test_batch_chunking_does_not_change_the_answer():
|
| 405 |
+
"""max_batch_graphs splits the work and nothing else, across molecules as within one."""
|
| 406 |
+
from magnet.inference import predict_shieldings_batch
|
| 407 |
+
dev = "cpu"
|
| 408 |
+
mH = MagNET_Lightning.load_from_checkpoint(os.path.join(CKPT, "MagNET-Zero_1H.ckpt"), map_location=dev).eval()
|
| 409 |
+
mC = MagNET_Lightning.load_from_checkpoint(os.path.join(CKPT, "MagNET-Zero_13C.ckpt"), map_location=dev).eval()
|
| 410 |
+
z = np.array([6, 1, 1, 1, 1])
|
| 411 |
+
xyz = np.array([[0., 0., 0.], [0.629, 0.629, 0.629], [-0.629, -0.629, 0.629],
|
| 412 |
+
[-0.629, 0.629, -0.629], [0.629, -0.629, -0.629]])
|
| 413 |
+
kw = dict(device=dev, n_passes=20, mirror_average=True)
|
| 414 |
+
whole = predict_shieldings_batch(mH, mC, [z, z, z], [xyz, xyz + 0.01, xyz - 0.01],
|
| 415 |
+
max_batch_graphs=1000, **kw)
|
| 416 |
+
chunked = predict_shieldings_batch(mH, mC, [z, z, z], [xyz, xyz + 0.01, xyz - 0.01],
|
| 417 |
+
max_batch_graphs=3, **kw)
|
| 418 |
+
for a, b in zip(whole, chunked):
|
| 419 |
+
assert np.max(np.abs(a - b)) < 0.05
|