import contextlib
import os
import warnings
from pathlib import Path
from typing import List, Optional, Tuple, Union
import numpy as np
from ase import Atoms
import _nepy
from calorine.nep.model import _get_nep_contents
def _get_atomic_properties(
structure: Atoms,
) -> Tuple[List[float], List[str], List[float]]:
"""Fetches cell, symbols and positions for a structure. Since NEP_CPU requires a cell, if the
structure has no cell a default cubic cell with a side of 100 Å will be used.
Parameters
----------
structure
Atoms object representing the structure.
Returns
-------
List[float]
Cell vectors
List[str]
Atomic species
List[float]
Atom positions
List[float]
Atom masses
"""
if structure.cell.rank == 0:
warnings.warn('Using default unit cell (cubic with side 100 Å).')
set_default_cell(structure)
c = structure.get_cell(complete=True).flatten()
cell = [c[0], c[3], c[6], c[1], c[4], c[7], c[2], c[5], c[8]]
symbols = structure.get_chemical_symbols()
positions = list(
structure.get_positions().T.flatten()
) # [x1, ..., xN, y1, ... yN,...]
masses = structure.get_masses()
return cell, symbols, positions, masses
def _setup_nepy(
model_filename: str,
natoms: int,
cell: List[float],
symbols: List[str],
positions: List[float],
masses: List[float],
debug: bool,
) -> _nepy.NEPY:
"""Sets up an instance of the NEPY pybind11 interface to NEP_CPU.
Parameters
----------
model_filename
Path to model.
natoms:
Number of atoms in the structure.
cell:
Cell vectors.
symbols:
Atom species.
positions:
Atom positions.
masses:
Atom masses.
debug:
Flag to control if the output from NEP_CPU will be printed.
Returns
-------
NEPY
NEPY interface
"""
# Ensure that `model_filename` exists to avoid segfault in pybind11 code
if not os.path.isfile(model_filename):
raise ValueError(f'{Path(model_filename)} does not exist')
# Disable output from C++ code by default
if debug:
nepy = _nepy.NEPY(model_filename, natoms, cell, symbols, positions, masses)
else:
with open(os.devnull, 'w') as f:
with contextlib.redirect_stdout(f):
with contextlib.redirect_stderr(f):
nepy = _nepy.NEPY(
model_filename, natoms, cell, symbols, positions, masses
)
return nepy
def set_default_cell(structure: Atoms, box_length: float = 100):
"""Adds a cubic box to an Atoms object. Atoms object is edited in-place.
Parameters
----------
structure
Structure to add box to
box_length
Cubic box side length in Å, by default 100
"""
structure.set_cell([[box_length, 0, 0], [0, box_length, 0], [0, 0, box_length]])
structure.center()
[docs]
def get_descriptors(
structure: Atoms, model_filename: Optional[str] = None, debug: bool = False
) -> np.ndarray:
"""Calculates the NEP descriptors for a given structure. A NEP model defined by a nep.txt
can additionally be provided to get the NEP3 model specific descriptors.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format. Defaults to ``None``.
debug
Flag to toggle debug mode. Makes the generated dummy NEP2 model available
in a local tmp directory, as well as prints GPUMD output. Defaults to ``False``.
Returns
-------
Descriptors for the supplied structure, with shape (natoms, descriptor components)
"""
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
all_descriptors = nepy.get_descriptors()
descriptors_per_atom = np.array(all_descriptors).reshape(-1, natoms).T
return descriptors_per_atom
[docs]
def get_latent_space(
structure: Atoms, model_filename: Union[str, None] = None, debug: bool = False
) -> np.ndarray:
"""Calculates the latent space representation of a structure, i.e, the activiations in
the hidden layer. A NEP model defined by a `nep.txt` file needs to be provided.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model. Defaults to None.
debug
Flag to toggle debug mode. Prints GPUMD output. Defaults to False.
Returns
-------
Activation with shape `(natoms, N_neurons)`
"""
if model_filename is None:
raise ValueError('Model is undefined')
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
latent = nepy.get_latent_space()
latent = np.array(latent).reshape(-1, natoms).T
return latent
[docs]
def get_potential_forces_and_virials(
structure: Atoms, model_filename: Optional[str] = None, debug: bool = False
) -> Tuple[np.ndarray, np.ndarray, np.ndarray]:
"""Calculates the per-atom potential, forces and virials for a given structure.
A NEP model defined by a `nep.txt` file needs to be provided.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model. Defaults to None.
debug
Flag to toggle debug mode. Prints GPUMD output. Defaults to False.
Returns
-------
potential with shape `(natoms,)`
forces with shape `(natoms, 3)`
virials with shape `(natoms, 9)`
"""
if model_filename is None:
raise ValueError('Model is undefined')
model_type = _get_nep_contents(model_filename)[0]['model_type']
if model_type != 'potential':
raise ValueError(
'A NEP model trained for predicting energies and forces must be used.'
)
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
energies, forces, virials = nepy.get_potential_forces_and_virials()
forces_per_atom = np.array(forces).reshape(-1, natoms).T
virials_per_atom = np.array(virials).reshape(-1, natoms).T
return np.array(energies), forces_per_atom, virials_per_atom
[docs]
def get_polarizability(
structure: Atoms,
model_filename: Optional[str] = None,
debug: bool = False,
) -> np.ndarray:
"""Calculates the polarizability tensor for a given structure. A NEP model defined
by a ``nep.txt`` file needs to be provided. The model must be trained to predict the
polarizability.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format. Defaults to ``None``.
debug
Flag to toggle debug mode. Prints GPUMD output. Defaults to ``False``.
Returns
-------
polarizability with shape ``(3, 3)``
"""
if model_filename is None:
raise ValueError('Model is undefined')
model_type = _get_nep_contents(model_filename)[0]['model_type']
if model_type != 'polarizability':
raise ValueError(
'A NEP model trained for predicting polarizability must be used.'
)
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
# Components are in order xx yy zz xy yz zx.
pol = nepy.get_polarizability()
polarizability = np.array([
[pol[0], pol[3], pol[5]],
[pol[3], pol[1], pol[4]],
[pol[5], pol[4], pol[2]]
])
return polarizability
[docs]
def get_dipole(
structure: Atoms,
model_filename: Optional[str] = None,
debug: bool = False,
) -> np.ndarray:
"""Calculates the dipole for a given structure. A NEP model defined by a
``nep.txt`` file needs to be provided.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format. Defaults to ``None``.
debug
Flag to toggle debug mode. Prints GPUMD output. Defaults to ``False``.
Returns
-------
dipole with shape ``(3,)``
"""
if model_filename is None:
raise ValueError('Model is undefined')
model_type = _get_nep_contents(model_filename)[0]['model_type']
if model_type != 'dipole':
raise ValueError('A NEP model trained for predicting dipoles must be used.')
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
dipole = np.array(nepy.get_dipole())
return dipole
[docs]
def get_dipole_gradient(
structure: Atoms,
model_filename: Optional[str] = None,
backend: str = 'c++',
method: str = 'central difference',
displacement: float = 0.01,
charge: float = 1.0,
nep_command: str = 'nep',
debug: bool = False,
) -> np.ndarray:
"""Calculates the dipole gradient for a given structure using finite differences.
A NEP model defined by a `nep.txt` file needs to be provided.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format. Defaults to ``None``.
backend
Backend to use for computing dipole gradient with finite differences.
One of ``'c++'`` (CPU), ``'python'`` (CPU) and ``'nep'`` (GPU).
Defaults to ``'c++'``.
method
Method for computing gradient with finite differences.
One of 'forward difference' and 'central difference'.
Defaults to 'central difference'
displacement
Displacement in Å to use for finite differences. Defaults to ``0.01``.
charge
System charge in units of the elemental charge.
Used for correcting the dipoles before computing the gradient.
Defaults to ``1.0``.
nep_command
Command for running the NEP executable. Defaults to ``'nep'``.
debug
Flag to toggle debug mode. Prints GPUMD output (if applicable). Defaults to ``False``.
Returns
-------
dipole gradient with shape ``(N, 3, 3)``
"""
if model_filename is None:
raise ValueError('Model is undefined')
model_type = _get_nep_contents(model_filename)[0]['model_type']
if model_type != 'dipole':
raise ValueError('A NEP model trained for predicting dipoles must be used.')
local_structure = structure.copy()
if backend == 'c++':
dipole_gradient = _dipole_gradient_cpp(
local_structure,
model_filename,
displacement=displacement,
method=method,
charge=charge,
debug=debug,
)
elif backend == 'python':
dipole_gradient = _dipole_gradient_python(
local_structure,
model_filename,
displacement=displacement,
charge=charge,
method=method,
)
elif backend == 'nep':
dipole_gradient = _dipole_gradient_nep(
local_structure,
model_filename,
displacement=displacement,
method=method,
charge=charge,
nep_command=nep_command,
)
else:
raise ValueError(f'Invalid backend {backend}')
return dipole_gradient
def _dipole_gradient_cpp(
structure: Atoms,
model_filename: str,
method: str = 'central difference',
displacement: float = 0.01,
charge: float = 1.0,
debug: bool = False,
) -> np.ndarray:
"""Calculates the dipole gradient with finite differences, using NEP_CPU.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format.
method
Method for computing gradient with finite differences.
One of ``'forward difference'`` and ``'central difference'``.
Defaults to ``'central difference'``
displacement
Displacement in Å to use for finite differences. Defaults to ``0.01``.
charge
System charge in units of the elemental charge.
Used for correcting the dipoles before computing the gradient.
Defaults to ``1.0``.
Returns
-------
dipole gradient with shape ``(N, 3, 3)``
"""
if displacement <= 0:
raise ValueError('Displacement must be > 0 Å')
implemented_methods = {
'forward difference': 0,
'central difference': 1,
'second order central difference': 2,
}
if method not in implemented_methods.keys():
raise ValueError(f'Invalid method {method} for calculating gradient')
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
dipole_gradient = np.array(
nepy.get_dipole_gradient(displacement, implemented_methods[method], charge)
).reshape(natoms, 3, 3)
return dipole_gradient
def _dipole_gradient_python(
structure: Atoms,
model_filename: str,
method: str = 'central difference',
displacement: float = 0.01,
charge: float = 1.0,
) -> np.ndarray:
"""Calculates the dipole gradient with finite differences, using the Python and get_dipole().
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format.
method
Method for computing gradient with finite differences.
One of ``'forward difference'`` and ``'central difference'``.
Defaults to ``'central difference'``
displacement
Displacement in Å to use for finite differences. Defaults to ``0.01``.
charge
System charge in units of the elemental charge.
Used for correcting the dipoles before computing the gradient.
Defaults to ``1.0``.
Returns
-------
dipole gradient with shape ``(N, 3, 3)``
"""
if displacement <= 0:
raise ValueError('Displacement must be > 0 Å')
N = len(structure)
if method == 'forward difference':
# Correct all dipole by the permanent dipole, charge * center of mass
d = (
get_dipole(structure, model_filename)
+ charge * structure.get_center_of_mass()
)
d_forward = np.zeros((N, 3, 3))
for atom in range(N):
for cartesian in range(3):
copy = structure.copy()
positions = copy.get_positions()
positions[atom, cartesian] += displacement
copy.set_positions(positions)
d_forward[atom, cartesian, :] = (
get_dipole(copy, model_filename)
+ charge * copy.get_center_of_mass()
)
gradient = (d_forward - d[None, None, :]) / displacement
elif method == 'central difference':
d_forward = np.zeros((N, 3, 3))
d_backward = np.zeros((N, 3, 3))
for atom in range(N):
for cartesian in range(3):
# Forward displacements
copy_forward = structure.copy()
positions_forward = copy_forward.get_positions()
positions_forward[atom, cartesian] += displacement
copy_forward.set_positions(positions_forward)
d_forward[atom, cartesian, :] = (
get_dipole(copy_forward, model_filename)
+ charge * copy_forward.get_center_of_mass()
)
# Backwards displacement
copy_backward = structure.copy()
positions_backward = copy_backward.get_positions()
positions_backward[atom, cartesian] -= displacement
copy_backward.set_positions(positions_backward)
d_backward[atom, cartesian, :] = (
get_dipole(copy_backward, model_filename)
+ charge * copy_backward.get_center_of_mass()
)
gradient = (d_forward - d_backward) / (2 * displacement)
elif method == 'second order central difference':
# Coefficients from
# https://en.wikipedia.org/wiki/Finite_difference_coefficient#Central_finite_difference
d_forward_one_h = np.zeros((N, 3, 3))
d_forward_two_h = np.zeros((N, 3, 3))
d_backward_one_h = np.zeros((N, 3, 3))
d_backward_two_h = np.zeros((N, 3, 3))
for atom in range(N):
for cartesian in range(3):
copy = structure.copy()
positions = copy.get_positions()
# Forward displacements
positions[atom, cartesian] += displacement # + h
copy.set_positions(positions)
d_forward_one_h[atom, cartesian, :] = (
get_dipole(copy, model_filename)
+ charge * copy.get_center_of_mass()
)
positions[atom, cartesian] += displacement # + 2h total
copy.set_positions(positions)
d_forward_two_h[atom, cartesian, :] = (
get_dipole(copy, model_filename)
+ charge * copy.get_center_of_mass()
)
# Backwards displacement
positions[atom, cartesian] -= 3 * displacement # 2h - 3h = -h
copy.set_positions(positions)
d_backward_one_h[atom, cartesian, :] = (
get_dipole(copy, model_filename)
+ charge * copy.get_center_of_mass()
)
positions[atom, cartesian] -= displacement # - 2h total
copy.set_positions(positions)
d_backward_two_h[atom, cartesian, :] = (
get_dipole(copy, model_filename)
+ charge * copy.get_center_of_mass()
)
c0 = -1.0 / 12.0
c1 = 2.0 / 3.0
gradient = (
c0 * d_forward_two_h
+ c1 * d_forward_one_h
- c1 * d_backward_one_h
- c0 * d_backward_two_h
) / displacement
else:
raise ValueError(f'Invalid method {method} for calculating gradient')
return gradient
def _dipole_gradient_nep(
structure: Atoms,
model_filename: str,
method: str = 'central difference',
displacement: float = 0.01,
charge: float = 1.0,
nep_command: str = 'nep',
) -> np.ndarray:
"""Calculates the dipole gradient with finite differences, using the NEP executable.
Parameters
----------
structure
Input structure
model_filename
Path to NEP model in ``nep.txt`` format.
method
Method for computing gradient with finite differences.
One of ``'forward difference'`` and ``'central difference'``.
Defaults to ``'central difference'``
displacement
Displacement in Å to use for finite differences. Defaults to 0.01 Å.
Note that results are possibly unreliable for displacemen < 0.01,
which might be due to rounding errors.
charge
System charge in units of the elemental charge.
Used for correcting the dipoles before computing the gradient.
Defaults to 1.0.
nep_command
Command for running the NEP executable. Defaults to ``'nep'``.
Returns
-------
dipole gradient with shape ``(N, 3, 3)``
"""
if displacement <= 0:
raise ValueError('Displacement must be > 0 Å')
if displacement < 1e-2:
warnings.warn(
'Dipole gradients with nep are unstable for displacements < 0.01 Å.'
)
N = len(structure)
if method == 'forward difference':
structure = _set_dummy_energy_forces(structure)
structures = [structure] # will hold 3N+1 structures
# Correct for the constant dipole, by adding charge * center of mass
corrections = np.zeros((3 * N + 1, 3))
corrections[0] = charge * structure.get_center_of_mass()
for atom in range(N):
for cartesian in range(3):
copy = structure.copy()
positions = copy.get_positions()
positions[atom, cartesian] += displacement
copy.set_positions(positions)
copy = _set_dummy_energy_forces(copy)
structures.append(copy)
corrections[1 + atom * 3 + cartesian] = (
charge * copy.get_center_of_mass()
)
dipoles = (
_predict_dipole_batch(structures, model_filename, nep_command) * N
) # dipole/atom, shape (3N+1, 3)
dipoles += corrections
d = dipoles[0, :]
d_forward = dipoles[1:].reshape(N, 3, 3)
gradient = (d_forward - d[None, None, :]) / displacement
elif method == 'central difference':
structures_forward = [] # will hold 3N structures
structures_backward = [] # will hold 3N structures
# Correct for the constant dipole, by adding charge * center of mass
corrections_forward = np.zeros((3 * N, 3))
corrections_backward = np.zeros((3 * N, 3))
for atom in range(N):
for cartesian in range(3):
# Forward displacements
copy_forward = structure.copy()
positions_forward = copy_forward.get_positions()
positions_forward[atom, cartesian] += displacement
copy_forward.set_positions(positions_forward)
copy_forward = _set_dummy_energy_forces(copy_forward)
structures_forward.append(copy_forward)
corrections_forward[atom * 3 + cartesian] = (
charge * copy_forward.get_center_of_mass()
)
# Backwards displacement
copy_backward = structure.copy()
positions_backward = copy_backward.get_positions()
positions_backward[atom, cartesian] -= displacement
copy_backward.set_positions(positions_backward)
copy_backward = _set_dummy_energy_forces(copy_backward)
structures_backward.append(copy_backward)
corrections_backward[atom * 3 + cartesian] = (
charge * copy_backward.get_center_of_mass()
)
structures = structures_forward + structures_backward
dipoles = (
_predict_dipole_batch(structures, model_filename, nep_command) * N
) # dipole/atom, shape (6N, 3)
d_forward = dipoles[: 3 * N, :]
d_backward = dipoles[3 * N :, :]
d_forward += corrections_forward
d_backward += corrections_backward
d_forward = d_forward.reshape(N, 3, 3)
d_backward = d_backward.reshape(N, 3, 3)
gradient = (d_forward - d_backward) / (2 * displacement)
else:
raise ValueError(f'Invalid method {method} for calculating gradient')
return gradient
def _set_dummy_energy_forces(structure: Atoms) -> Atoms:
"""Sets the energies and forces of structure to zero.
Parameters
----------
structure
Input structure
Returns
------- Copy of structure, with SinglePointCalculator with zero energy and force.
"""
from ase.calculators.singlepoint import SinglePointCalculator
copy = structure.copy()
N = len(copy)
energy = 0
forces = np.zeros((N, 3))
dummy = SinglePointCalculator(copy, **{'energy': energy, 'forces': forces})
copy.calc = dummy
return copy
def _predict_dipole_batch(
structures: List[Atoms], model_filename: str, nep_command: str = 'nep'
) -> np.ndarray:
"""Predicts dipoles for a set of structures using the NEP executable
Note that the units are in (dipole units)/atom.
Parameters
----------
structure
Input structures
model_filename
Path to NEP model in ``nep.txt`` format.
nep_command
Command for running the NEP executable. Defaults to ``'nep'``.
Returns
------- Predicted dipoles, with shape (len(structures), 3).
"""
import shutil
from os.path import join as join_path
from subprocess import run
from tempfile import TemporaryDirectory
from calorine.nep import read_model, write_nepfile, write_structures
with TemporaryDirectory() as directory:
shutil.copy2(model_filename, join_path(directory, 'nep.txt'))
model = read_model(model_filename)
parameters = dict(
prediction=1,
mode=1,
version=model.version,
n_max=[model.n_max_radial, model.n_max_angular],
cutoff=[model.radial_cutoff, model.angular_cutoff],
basis_size=[model.n_basis_radial, model.n_basis_radial],
l_max=[model.l_max_3b, model.l_max_4b, model.l_max_5b],
neuron=model.n_neuron,
type=[len(model.types), *model.types],
)
write_nepfile(parameters, directory)
file = join_path(directory, 'train.xyz')
write_structures(file, structures)
# Execute nep
completed = run([nep_command], cwd=directory, capture_output=True)
completed.check_returncode()
# Read results
dipoles = np.loadtxt(join_path(directory, 'dipole_train.out'))
if len(dipoles.shape) == 1:
dipoles = dipoles.reshape(1, -1)
return dipoles[:, :3]
def _check_components_polarizability_gradient(component: Union[str, List[str]]) -> List[int]:
"""
Verifies that the selected components are ok.
"""
allowed_components = {
'x': 0,
'y': 1,
'z': 2,
}
# Check if chosen components are ok
if component == 'full':
components_to_compute = [0, 1, 2]
else:
components_list = [component] if isinstance(component, str) else component
components_to_compute = []
for c in components_list:
if c in allowed_components.keys():
components_to_compute.append(allowed_components[c])
elif c == 'full':
raise ValueError('Write ``component="full"`` to get all components.')
else:
raise ValueError(f'Invalid component {c}')
assert len(components_list) == len(components_to_compute), \
'Number of components to compute does not match.'
return components_to_compute
[docs]
def get_polarizability_gradient(
structure: Atoms,
model_filename: Optional[str] = None,
displacement: float = 0.01,
component: Union[str, List[str]] = 'full',
debug: bool = False,
) -> np.ndarray:
"""Calculates the dipole gradient for a given structure using finite differences.
A NEP model defined by a ``nep.txt`` file needs to be provided.
This function computes the derivatives using the second-order central difference
method with a C++ backend.
Parameters
----------
structure
Input structure.
model_filename
Path to NEP model in ``nep.txt`` format. Defaults to ``None``.
displacement
Displacement in Å to use for finite differences. Defaults to ``0.01``.
component
Component or components of the polarizability tensor that the gradient
should be computed for.
The following components are available: ``x`, ``y``, ``z``, ``full``.
Option ``full`` computes the derivative whilst moving the atoms in each Cartesian
direction, which yields a tensor of shape ``(N, 3, 6)``.
Multiple components may be specified.
Defaults to ``full``.
debug
Flag to toggle debug mode. Prints GPUMD output (if applicable). Defaults to ``False``.
Returns
-------
polarizability gradient with shape ``(N, C, 6)`` where ``C``
is the number of components chosen.
"""
if model_filename is None:
raise ValueError('Model is undefined')
model_type = _get_nep_contents(model_filename)[0]['model_type']
if model_type != 'polarizability':
raise ValueError('A NEP model trained for predicting polarizability must be used.')
components_to_compute = _check_components_polarizability_gradient(component)
local_structure = structure.copy()
polarizability_gradient = _polarizability_gradient_cpp(
local_structure,
model_filename,
displacement=displacement,
components=components_to_compute,
debug=debug,
)
return polarizability_gradient
def _polarizability_gradient_to_3x3(natoms, pg):
"""
Converts a polarizability gradient tensor with
shape (Natoms, 3, 6) to (Natoms, 3, 3, 3).
The 6 items in the polarizability gradient have
the following order from GPUMD: xx, yy, zz, xy, yz, zx.
"""
gpumd_to_3x3_indices = np.array([
[0, 3, 5],
[3, 1, 4],
[5, 4, 2]
])
polgrad_3x3 = np.zeros((natoms, 3, 3, 3))
for i in range(3):
for j in range(3):
index = gpumd_to_3x3_indices[i, j]
polgrad_3x3[:, :, i, j] = pg[:, :, index]
return polgrad_3x3
def _polarizability_gradient_cpp(
structure: Atoms,
model_filename: str,
displacement: float,
components: List[int],
debug: bool = False,
) -> np.ndarray:
"""Calculates the polarizability gradient with finite differences, using NEP_CPU.
Parameters
----------
structure
Input structure.
model_filename
Path to NEP model in ``nep.txt`` format.
displacement
Displacement in Å to use for finite differences. Defaults to ``0.01``.
components
List of components to compute. Integer values from 0 to 2 that corresponds
to indices in the ordered list [x, y, z]. Index 1 corresponds to the
derivative with regards to only the y positions of the atoms, and so forth.
Returns
-------
dipole gradient with shape ``(N, len(components), 3, 3)``
"""
if displacement <= 0:
raise ValueError('Displacement must be > 0 Å')
# TODO possibly use components later to only move atoms in one cartesian direction
local_structure = structure.copy()
natoms = len(local_structure)
cell, symbols, positions, masses = _get_atomic_properties(local_structure)
nepy = _setup_nepy(
model_filename, natoms, cell, symbols, positions, masses, debug
)
pg = np.array(
nepy.get_polarizability_gradient(displacement, components)
).reshape(natoms, 3, 6)
# Convert to 3x3
polarizability_gradient = _polarizability_gradient_to_3x3(natoms, pg)
return polarizability_gradient[:, components, :, :] # Only return the relevant components