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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,
}