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", # 'graph' : data_list_collater([data_obj]), } 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): # data_obj=a2g.convert(atoms) curr_atoms = Atoms( positions=batch["graph"].pos, cell=batch["cell"][0], numbers=batch["graph"].atomic_numbers, pbc=True, ) # True or false 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))) # Calculate the cross products 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)), ) # Calculate the perpendicular heights 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): # Create a new Atoms object with the perturbed positions 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_cell # Scaled or Unscaled ? 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]) # Returns : Peak index and Bond length 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() # write_xyz(f"StabilityXYZData2/{Structid}.xyz",atoms.get_positions(),atoms.get_chemical_symbols(),atoms.get_cell()) 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) # atoms.rattle(0.01) analysis = Analysis([perturb_config(atoms, noise_std) for k in range(perturb)]) # write_xyz(f"StabilityXYZDataReplicated2/{Structid}.xyz",atoms.get_positions(),atoms.get_chemical_symbols(),atoms.get_cell()) 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 ## MAce Calculator 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") # pylint: disable=dangerous-default-value 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: """ # call to base-class to set atoms attribute Calculator.calculate(self, atoms) # prepare data batch = self.convAtomstoBatch(atoms) # predict + extract data out = self.model.predict(to(batch,self.model.device)) #out = self.model.forward(batch) energy = out['energy'].detach().cpu().item() forces = out["force"].detach().cpu().numpy() stress = out["stress"].squeeze(0).detach().cpu().numpy() # store results 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, # force has units eng / len: "forces": forces, "stress": stress, }