| import matplotlib.pyplot as plt
|
| import numpy as np
|
| import torch
|
| from ase import Atoms
|
| from ase.calculators.calculator import Calculator, all_changes
|
| from ase.geometry.analysis import Analysis
|
| from ase.optimize import FIRE
|
| from matsciml.datasets.trajectory_lmdb import data_list_collater
|
| from matsciml.datasets.transforms import (
|
| FrameAveraging,
|
| PeriodicPropertiesTransform,
|
| PointCloudToGraphTransform,
|
| )
|
| from matsciml.preprocessing.atoms_to_graphs import AtomsToGraphs
|
|
|
| a2g = AtomsToGraphs(
|
| max_neigh=200,
|
| radius=6,
|
| r_energy=False,
|
| r_forces=False,
|
| r_distances=False,
|
| r_edges=True,
|
| r_fixed=True,
|
| )
|
| f_avg = FrameAveraging(frame_averaging="3D", fa_method="stochastic")
|
| PBCTransform = PeriodicPropertiesTransform(cutoff_radius=6.0, adaptive_cutoff=True)
|
| GTransform = PointCloudToGraphTransform(
|
| "dgl",
|
| node_keys=["pos", "atomic_numbers"],
|
| )
|
|
|
|
|
| def convAtomstoBatchmace(atoms):
|
| data_obj = a2g.convert(atoms)
|
| Reformatted_batch = {
|
| "cell": data_obj.cell,
|
| "natoms": torch.Tensor([data_obj.natoms]).unsqueeze(0),
|
| "edge_index": [data_obj.edge_index.shape],
|
| "cell_offsets": data_obj.cell_offsets,
|
| "atomic_numbers": data_obj.atomic_numbers,
|
| "pos": data_obj.pos,
|
| "y": None,
|
| "force": None,
|
| "fixed": [data_obj.fixed],
|
| "tags": None,
|
| "sid": None,
|
| "fid": None,
|
| "dataset": "S2EFDataset",
|
| "graph": data_list_collater([data_obj]),
|
| }
|
|
|
| Reformatted_batch = PBCTransform(Reformatted_batch)
|
|
|
| return Reformatted_batch
|
|
|
|
|
| def convAtomstoBatchtensornet(atoms):
|
| data_obj = a2g.convert(atoms)
|
| Reformatted_batch = {
|
| "cell": data_obj.cell,
|
| "natoms": torch.Tensor([data_obj.natoms]).unsqueeze(0),
|
| "edge_index": [data_obj.edge_index.shape],
|
| "cell_offsets": data_obj.cell_offsets,
|
| "atomic_numbers": data_obj.atomic_numbers,
|
| "pos": data_obj.pos,
|
| "y": None,
|
| "force": None,
|
| "fixed": [data_obj.fixed],
|
| "tags": None,
|
| "sid": None,
|
| "fid": None,
|
| "dataset": "S2EFDataset",
|
|
|
| }
|
| Reformatted_batch = PBCTransform(Reformatted_batch)
|
| Reformatted_batch = GTransform(Reformatted_batch)
|
| return Reformatted_batch
|
|
|
|
|
| def convAtomstoBatchfaenet(atoms):
|
| data_obj = a2g.convert(atoms)
|
| Reformatted_batch = {
|
| "cell": data_obj.cell,
|
| "natoms": torch.Tensor([data_obj.natoms]).unsqueeze(0),
|
| "edge_index": [data_obj.edge_index.shape],
|
| "cell_offsets": data_obj.cell_offsets,
|
| "atomic_numbers": data_obj.atomic_numbers,
|
| "pos": data_obj.pos,
|
| "y": None,
|
| "force": None,
|
| "fixed": [data_obj.fixed],
|
| "tags": None,
|
| "sid": None,
|
| "fid": None,
|
| "dataset": "S2EFDataset",
|
| "graph": data_list_collater([data_obj]),
|
| }
|
| Reformatted_batch = f_avg(Reformatted_batch)
|
| Reformatted_batch = PBCTransform(Reformatted_batch)
|
|
|
| return Reformatted_batch
|
|
|
|
|
| def convBatchtoAtoms(batch):
|
|
|
| curr_atoms = Atoms(
|
| positions=batch["graph"].pos,
|
| cell=batch["cell"][0],
|
| numbers=batch["graph"].atomic_numbers,
|
| pbc=True,
|
| )
|
|
|
| return curr_atoms
|
|
|
|
|
| def minimize_structure(atoms, fmax=0.05, steps=50):
|
| """
|
| Perform energy minimization on the given ASE Atoms object using the FIRE optimizer.
|
|
|
| Parameters:
|
| atoms (ase.Atoms): The Atoms object to be minimized.
|
| fmax (float): The maximum force tolerance for the optimization (default: 0.01 eV/Å).
|
| steps (int): The maximum number of optimization steps (default: 1000).
|
|
|
| Returns:
|
| ase.Atoms: The minimized Atoms object.
|
| """
|
| dyn = FIRE(atoms, trajectory=None)
|
| dyn.run(fmax=fmax, steps=steps)
|
| return atoms
|
|
|
|
|
| def to(data, device):
|
| """Simple utility function to move things to correct device"""
|
| new_dict = {}
|
| for key, value in data.items():
|
| if hasattr(value, "to"):
|
| new_dict[key] = value.to(device)
|
| else:
|
| new_dict[key] = value
|
| return new_dict
|
|
|
|
|
| def min_height(cell_matrix):
|
| """
|
| Calculate the perpendicular heights in three directions given a 3x3 cell matrix.
|
| """
|
| a, b, c = cell_matrix[:, 0], cell_matrix[:, 1], cell_matrix[:, 2]
|
| volume = abs(np.dot(a, np.cross(b, c)))
|
|
|
| a_cross_b, b_cross_c, c_cross_a = (
|
| np.linalg.norm(np.cross(a, b)),
|
| np.linalg.norm(np.cross(b, c)),
|
| np.linalg.norm(np.cross(c, a)),
|
| )
|
|
|
| height_a, height_b, height_c = (
|
| abs(volume / a_cross_b),
|
| abs(volume / b_cross_c),
|
| abs(volume / c_cross_a),
|
| )
|
| return min(height_a, height_b, height_c)
|
|
|
|
|
| def perturb_config(atoms, displacement_std=0.01):
|
|
|
| positions = atoms.get_positions()
|
| displacements = np.random.normal(scale=displacement_std, size=positions.shape)
|
| new_positions = positions + displacements
|
| new_perturbed_atoms = atoms.copy()
|
| new_perturbed_atoms.set_positions(new_positions)
|
| return new_perturbed_atoms
|
|
|
|
|
| def plot_pair_rdfs(Pair_rdfs, shift=0):
|
| counter = 0
|
| plt.figure()
|
| for key in Pair_rdfs.keys():
|
| plt.plot(Pair_rdfs[key][0], Pair_rdfs[key][1] + shift * counter, label=key)
|
| counter += 1
|
| plt.legend(loc=(1.2, 0))
|
| plt.xlabel("r (Angstrom)")
|
| plt.ylabel("g(r)")
|
| plt.show()
|
|
|
|
|
| def replicate_system(atoms, replicate_factors):
|
| """
|
| Replicates the given ASE Atoms object according to the specified replication factors.
|
| """
|
| nx, ny, nz = replicate_factors
|
| original_cell = atoms.get_cell()
|
| original_positions = atoms.get_positions()
|
| original_numbers = atoms.get_atomic_numbers()
|
| x_cell, y_cell, z_cell = original_cell[0], original_cell[1], original_cell[2]
|
| new_numbers = []
|
| for i in range(nx):
|
| for j in range(ny):
|
| for k in range(nz):
|
| new_numbers += [original_numbers]
|
| pos_after_x = np.concatenate([original_positions + i * x_cell for i in range(nx)])
|
| pos_after_y = np.concatenate([pos_after_x + i * y_cell for i in range(ny)])
|
| pos_after_z = np.concatenate([pos_after_y + i * z_cell for i in range(nz)])
|
| new_cell = [nx * original_cell[0], ny * original_cell[1], nz * original_cell[2]]
|
| new_atoms = Atoms(
|
| numbers=np.concatenate(new_numbers),
|
| positions=pos_after_z,
|
| cell=new_cell,
|
| pbc=atoms.get_pbc(),
|
| )
|
| return new_atoms
|
|
|
|
|
| def write_xyz(Filepath, atoms):
|
| """Writes ovito xyz file"""
|
| R = atoms.get_position()
|
| species = atoms.get_atomic_numbers()
|
| cell = atoms.get_cell()
|
| f = open(Filepath, "w")
|
| f.write(str(R.shape[0]) + "\n")
|
| flat_cell = cell.flatten()
|
| f.write(
|
| f'Lattice="{flat_cell[0]} {flat_cell[1]} {flat_cell[2]} {flat_cell[3]} {flat_cell[4]} {flat_cell[5]} {flat_cell[6]} {flat_cell[7]} {flat_cell[8]}" Properties=species:S:1:pos:R:3 Time=0.0'
|
| )
|
| for i in range(R.shape[0]):
|
| f.write(
|
| "\n"
|
| + str(species[i])
|
| + "\t"
|
| + str(R[i, 0])
|
| + "\t"
|
| + str(R[i, 1])
|
| + "\t"
|
| + str(R[i, 2])
|
| )
|
|
|
|
|
| def symmetricize_replicate(curr_atoms, max_atoms, box_lengths):
|
| replication = [1, 1, 1]
|
| atom_count = curr_atoms
|
| lengths = box_lengths
|
| while atom_count < (max_atoms // 2):
|
| direction = np.argmin(box_lengths)
|
| replication[direction] += 1
|
| lengths[direction] = box_lengths[direction] * replication[direction]
|
| atom_count = curr_atoms * replication[0] * replication[1] * replication[2]
|
| return replication, atom_count
|
|
|
|
|
| def get_pairs(atoms):
|
| Atom_types = np.unique(atoms.get_chemical_symbols())
|
| Pairs = []
|
| for i in range(len(Atom_types)):
|
| for j in range(i, len(Atom_types)):
|
| Pairs += [[Atom_types[i], Atom_types[j]]]
|
| return Pairs
|
|
|
|
|
| def getfirstpeaklength(r, rdf, r_max=6.0):
|
| bin_size = (r[-1] - r[0]) / len(r)
|
| cut_index = int(r_max / bin_size)
|
| cut_index = min(cut_index, len(r))
|
| Peak_index = np.argmax(rdf[:cut_index])
|
|
|
| return Peak_index, r[Peak_index]
|
|
|
|
|
| def get_partial_rdfs(Traj, r_max=6.0, dr=0.01):
|
| rmax = min(r_max, min_height(Traj[0].get_cell()) / 2.7)
|
| analysis = Analysis(Traj)
|
| dr = dr
|
| nbins = int(rmax / dr)
|
| pairs_list = get_pairs(Traj[0])
|
| Pair_rdfs = dict()
|
| for pair in pairs_list:
|
| rdf = analysis.get_rdf(
|
| rmax=rmax, nbins=nbins, imageIdx=None, elements=pair, return_dists=True
|
| )
|
| x = rdf[0][1]
|
| y = np.array([rdf[k][0] for k in range(len(rdf))]).mean(axis=0)
|
| Pair_rdfs["-".join(pair)] = [x, y]
|
| return Pair_rdfs
|
|
|
|
|
| def get_partial_rdfs_smoothened(
|
| inp_atoms, perturb=10, noise_std=0.01, max_atoms=300, r_max=6.0, dr=0.01
|
| ):
|
| atoms = inp_atoms.copy()
|
| replication_factors, _ = symmetricize_replicate(
|
| len(atoms),
|
| max_atoms=max_atoms,
|
| box_lengths=atoms.get_cell_lengths_and_angles()[:3],
|
| )
|
| atoms = replicate_system(atoms, replication_factors)
|
| Traj = [perturb_config(atoms, noise_std) for k in range(perturb)]
|
| return get_partial_rdfs(Traj, r_max=r_max, dr=dr)
|
|
|
|
|
| def get_bond_lengths_noise(
|
| inp_atoms, perturb=10, noise_std=0.01, max_atoms=300, r_max=6.0, dr=0.01
|
| ):
|
| Pair_rdfs = get_partial_rdfs_smoothened(
|
| inp_atoms,
|
| perturb=perturb,
|
| noise_std=noise_std,
|
| max_atoms=max_atoms,
|
| r_max=r_max,
|
| dr=dr,
|
| )
|
| Bond_lengths = dict()
|
| for key in Pair_rdfs:
|
| r, rdf = Pair_rdfs[key]
|
| Bond_lengths[key] = getfirstpeaklength(r, rdf)[1]
|
| return Bond_lengths, Pair_rdfs
|
|
|
|
|
| def get_bond_lengths_TrajAvg(Traj, r_max=6.0, dr=0.01):
|
| Pair_rdfs = get_partial_rdfs(Traj, r_max=r_max, dr=dr)
|
| Bond_lengths = dict()
|
| for key in Pair_rdfs:
|
| r, rdf = Pair_rdfs[key]
|
| Bond_lengths[key] = getfirstpeaklength(r, rdf)[1]
|
| return Bond_lengths, Pair_rdfs
|
|
|
|
|
| def get_initial_rdf(
|
| inp_atoms,
|
| perturb=10,
|
| noise_std=0.01,
|
| max_atoms=300,
|
| replicate=False,
|
| Structid=0,
|
| r_max=6.0,
|
| dr=0.01,
|
| ):
|
| atoms = inp_atoms.copy()
|
|
|
| if replicate:
|
| replication_factors, size = symmetricize_replicate(
|
| len(atoms),
|
| max_atoms=max_atoms,
|
| box_lengths=atoms.get_cell_lengths_and_angles()[:3],
|
| )
|
| atoms = replicate_system(atoms, replication_factors)
|
| rmax = min(r_max, min_height(atoms.get_cell()) / 2.7)
|
|
|
| analysis = Analysis([perturb_config(atoms, noise_std) for k in range(perturb)])
|
|
|
| dr = dr
|
| nbins = int(rmax / dr)
|
| rdf = analysis.get_rdf(
|
| rmax=rmax, nbins=nbins, imageIdx=None, elements=None, return_dists=True
|
| )
|
| x = rdf[0][1]
|
| y = np.array([rdf[k][0] for k in range(len(rdf))]).mean(axis=0)
|
| return x, y
|
|
|
|
|
| def get_rdf(Traj, r_max=6.0, dr=0.01):
|
| rmax = min(r_max, min_height(Traj[0].get_cell()) / 2.7)
|
| analysis = Analysis(Traj)
|
| dr = dr
|
| nbins = int(rmax / dr)
|
| rdf = analysis.get_rdf(
|
| rmax=rmax, nbins=nbins, imageIdx=None, elements=None, return_dists=True
|
| )
|
| x = rdf[0][1]
|
| y = np.array([rdf[k][0] for k in range(len(rdf))]).mean(axis=0)
|
| return x, y
|
|
|
|
|
|
|
| class ASEcalculator(Calculator):
|
| """Simulation ASE Calculator"""
|
|
|
| implemented_properties = ["energy", "forces", "stress"]
|
|
|
| def __init__(self, model, model_name, **kwargs):
|
| Calculator.__init__(self, **kwargs)
|
| self.results = {}
|
|
|
| self.model = model
|
| if model_name == "mace":
|
| self.convAtomstoBatch = convAtomstoBatchmace
|
|
|
| elif model_name == "faenet":
|
| self.convAtomstoBatch = convAtomstoBatchfaenet
|
|
|
| elif model_name == "tensornet":
|
| self.convAtomstoBatch = convAtomstoBatchtensornet
|
|
|
| else:
|
| print("Wrong Model Name")
|
|
|
|
|
| def calculate(self, atoms=None, properties=None, system_changes=all_changes):
|
| """
|
| Calculate properties.
|
| :param atoms: ase.Atoms object
|
| :param properties: [str], properties to be computed, used by ASE internally
|
| :param system_changes: [str], system changes since last calculation, used by ASE internally
|
| :return:
|
| """
|
|
|
| Calculator.calculate(self, atoms)
|
|
|
|
|
| batch = self.convAtomstoBatch(atoms)
|
|
|
|
|
| out = self.model.predict(to(batch,self.model.device))
|
|
|
| energy = out['energy'].detach().cpu().item()
|
| forces = out["force"].detach().cpu().numpy()
|
| stress = out["stress"].squeeze(0).detach().cpu().numpy()
|
|
|
| E = energy
|
| stress = np.array(
|
| [
|
| stress[0, 0],
|
| stress[1, 1],
|
| stress[2, 2],
|
| stress[1, 2],
|
| stress[0, 2],
|
| stress[0, 1],
|
| ]
|
| )
|
| self.results = {
|
| "energy": E,
|
|
|
| "forces": forces,
|
| "stress": stress,
|
| }
|
|
|