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import warnings
from math import sqrt
import numpy as np
from ase import Atoms
from ase.calculators.singlepoint import SinglePointCalculator
from ase.constraints import FixAtoms
from ase.data import covalent_radii
from ase.geometry import find_mic
from ase.gui.defaults import read_defaults
from ase.gui.i18n import _
from ase.io import read, string2index, write
class Images:
def __init__(self, images=None):
self.covalent_radii = covalent_radii.copy()
self.config = read_defaults()
self.atom_scale = self.config['radii_scale']
if images is None:
images = [Atoms()]
self.initialize(images)
def __len__(self):
return len(self._images)
def __getitem__(self, index):
return self._images[index]
def __iter__(self):
return iter(self._images)
# XXXXXXX hack
# compatibility hacks while allowing variable number of atoms
def get_dynamic(self, atoms: Atoms) -> np.ndarray:
dynamic = np.ones(len(atoms), bool)
for constraint in atoms.constraints:
if isinstance(constraint, FixAtoms):
dynamic[constraint.index] = False
return dynamic
def set_dynamic(self, mask, value):
# Does not make much sense if different images have different
# atom counts. Attempts to apply mask to all images,
# to the extent possible.
for atoms in self:
dynamic = self.get_dynamic(atoms)
dynamic[mask[:len(atoms)]] = value
atoms.constraints = [c for c in atoms.constraints
if not isinstance(c, FixAtoms)]
atoms.constraints.append(FixAtoms(mask=~dynamic))
def scale_radii(self, scaling_factor):
self.covalent_radii *= scaling_factor
def get_energy(self, atoms: Atoms) -> np.float64:
try:
return atoms.get_potential_energy()
except RuntimeError:
return np.nan # type: ignore[return-value]
def get_forces(self, atoms: Atoms):
try:
return atoms.get_forces(apply_constraint=False)
except RuntimeError:
return None
def initialize(self, images, filenames=None):
nimages = len(images)
if filenames is None:
filenames = [None] * nimages
self.filenames = filenames
warning = False
self._images = []
# Whether length or chemical composition changes:
self.have_varying_species = False
for i, atoms in enumerate(images):
# copy atoms or not? Not copying allows back-editing,
# but copying actually forgets things like the attached
# calculator (might have forces/energies
self._images.append(atoms)
self.have_varying_species |= not np.array_equal(self[0].numbers,
atoms.numbers)
if hasattr(self, 'Q'):
assert False # XXX askhl fix quaternions
self.Q[i] = atoms.get_quaternions()
if (atoms.pbc != self[0].pbc).any():
warning = True
if warning:
import warnings
warnings.warn('Not all images have the same boundary conditions!')
self.maxnatoms = max(len(atoms) for atoms in self)
self.selected = np.zeros(self.maxnatoms, bool)
self.selected_ordered = []
self.visible = np.ones(self.maxnatoms, bool)
self.repeat = np.ones(3, int)
def get_radii(self, atoms: Atoms) -> np.ndarray:
radii = np.array([self.covalent_radii[z] for z in atoms.numbers])
radii *= self.atom_scale
return radii
def read(self, filenames, default_index=':', filetype=None):
if isinstance(default_index, str):
default_index = string2index(default_index)
images = []
names = []
for filename in filenames:
from ase.io.formats import parse_filename
if '@' in filename and 'postgres' not in filename or \
'postgres' in filename and filename.count('@') == 2:
actual_filename, index = parse_filename(filename, None)
else:
actual_filename, index = parse_filename(filename,
default_index)
# Read from stdin:
if filename == '-':
import sys
from io import BytesIO
buf = BytesIO(sys.stdin.buffer.read())
buf.seek(0)
filename = buf
filetype = 'traj'
imgs = read(filename, index, filetype)
if hasattr(imgs, 'iterimages'):
imgs = list(imgs.iterimages())
images.extend(imgs)
# Name each file as filename@index:
if isinstance(index, slice):
start = index.start or 0
step = index.step or 1
else:
start = index
step = 1
for i, img in enumerate(imgs):
if isinstance(start, int):
names.append('{}@{}'.format(
actual_filename, start + i * step))
else:
names.append(f'{actual_filename}@{start}')
self.initialize(images, names)
def repeat_results(self, atoms: Atoms, repeat=None, oldprod=None):
"""Return a dictionary which updates the magmoms, energy and forces
to the repeated amount of atoms.
"""
def getresult(name, get_quantity):
# ase/io/trajectory.py line 170 does this by using
# the get_property(prop, atoms, allow_calculation=False)
# so that is an alternative option.
try:
if (not atoms.calc or
atoms.calc.calculation_required(atoms, [name])):
quantity = None
else:
quantity = get_quantity()
except Exception as err:
quantity = None
errmsg = ('An error occurred while retrieving {} '
'from the calculator: {}'.format(name, err))
warnings.warn(errmsg)
return quantity
if repeat is None:
repeat = self.repeat.prod()
if oldprod is None:
oldprod = self.repeat.prod()
results = {}
original_length = len(atoms) // oldprod
newprod = repeat.prod()
# Read the old properties
magmoms = getresult('magmoms', atoms.get_magnetic_moments)
magmom = getresult('magmom', atoms.get_magnetic_moment)
energy = getresult('energy', atoms.get_potential_energy)
forces = getresult('forces', atoms.get_forces)
# Update old properties to the repeated image
if magmoms is not None:
magmoms = np.tile(magmoms[:original_length], newprod)
results['magmoms'] = magmoms
if magmom is not None:
magmom = magmom * newprod / oldprod
results['magmom'] = magmom
if forces is not None:
forces = np.tile(forces[:original_length].T, newprod).T
results['forces'] = forces
if energy is not None:
energy = energy * newprod / oldprod
results['energy'] = energy
return results
def repeat_unit_cell(self):
for atoms in self:
# Get quantities taking into account current repeat():'
results = self.repeat_results(atoms, self.repeat.prod(),
oldprod=self.repeat.prod())
atoms.cell *= self.repeat.reshape((3, 1))
atoms.calc = SinglePointCalculator(atoms, **results)
self.repeat = np.ones(3, int)
def repeat_images(self, repeat):
from ase.constraints import FixAtoms
repeat = np.array(repeat)
oldprod = self.repeat.prod()
images = []
constraints_removed = False
for i, atoms in enumerate(self):
refcell = atoms.get_cell()
fa = []
for c in atoms._constraints:
if isinstance(c, FixAtoms):
fa.append(c)
else:
constraints_removed = True
atoms.set_constraint(fa)
# Update results dictionary to repeated atoms
results = self.repeat_results(atoms, repeat, oldprod)
del atoms[len(atoms) // oldprod:] # Original atoms
atoms *= repeat
atoms.cell = refcell
atoms.calc = SinglePointCalculator(atoms, **results)
images.append(atoms)
if constraints_removed:
from ase.gui.ui import showwarning, tk
# We must be able to show warning before the main GUI
# has been created. So we create a new window,
# then show the warning, then destroy the window.
tmpwindow = tk.Tk()
tmpwindow.withdraw() # Host window will never be shown
showwarning(_('Constraints discarded'),
_('Constraints other than FixAtoms '
'have been discarded.'))
tmpwindow.destroy()
self.initialize(images, filenames=self.filenames)
self.repeat = repeat
def center(self):
"""Center each image in the existing unit cell, keeping the
cell constant."""
for atoms in self:
atoms.center()
def graph(self, expr: str) -> np.ndarray:
"""Routine to create the data in graphs, defined by the
string expr."""
import ase.units as units
code = compile(expr + ',', '<input>', 'eval')
nimages = len(self)
def d(n1, n2):
return sqrt(((R[n1] - R[n2])**2).sum())
def a(n1, n2, n3):
v1 = R[n1] - R[n2]
v2 = R[n3] - R[n2]
arg = np.vdot(v1, v2) / (sqrt((v1**2).sum() * (v2**2).sum()))
if arg > 1.0:
arg = 1.0
if arg < -1.0:
arg = -1.0
return 180.0 * np.arccos(arg) / np.pi
def dih(n1, n2, n3, n4):
# vector 0->1, 1->2, 2->3 and their normalized cross products:
a = R[n2] - R[n1]
b = R[n3] - R[n2]
c = R[n4] - R[n3]
bxa = np.cross(b, a)
bxa /= np.sqrt(np.vdot(bxa, bxa))
cxb = np.cross(c, b)
cxb /= np.sqrt(np.vdot(cxb, cxb))
angle = np.vdot(bxa, cxb)
# check for numerical trouble due to finite precision:
if angle < -1:
angle = -1
if angle > 1:
angle = 1
angle = np.arccos(angle)
if np.vdot(bxa, c) > 0:
angle = 2 * np.pi - angle
return angle * 180.0 / np.pi
# get number of mobile atoms for temperature calculation
E = np.array([self.get_energy(atoms) for atoms in self])
s = 0.0
# Namespace for eval:
ns = {'E': E,
'd': d, 'a': a, 'dih': dih}
data = []
for i in range(nimages):
ns['i'] = i
ns['s'] = s
ns['R'] = R = self[i].get_positions()
ns['V'] = self[i].get_velocities()
F = self.get_forces(self[i])
if F is not None:
ns['F'] = F
ns['A'] = self[i].get_cell()
ns['M'] = self[i].get_masses()
# XXX askhl verify:
dynamic = self.get_dynamic(self[i])
if F is not None:
ns['f'] = f = ((F * dynamic[:, None])**2).sum(1)**.5
ns['fmax'] = max(f)
ns['fave'] = f.mean()
ns['epot'] = epot = E[i]
ns['ekin'] = ekin = self[i].get_kinetic_energy()
ns['e'] = epot + ekin
ndynamic = dynamic.sum()
if ndynamic > 0:
ns['T'] = 2.0 * ekin / (3.0 * ndynamic * units.kB)
data = eval(code, ns)
if i == 0:
nvariables = len(data)
xy = np.empty((nvariables, nimages))
xy[:, i] = data
if i + 1 < nimages and not self.have_varying_species:
dR = find_mic(self[i + 1].positions - R, self[i].get_cell(),
self[i].get_pbc())[0]
s += sqrt((dR**2).sum())
return xy
def write(self, filename, rotations='', bbox=None,
**kwargs):
# XXX We should show the unit cell whenever there is one
indices = range(len(self))
p = filename.rfind('@')
if p != -1:
try:
slice = string2index(filename[p + 1:])
except ValueError:
pass
else:
indices = indices[slice]
filename = filename[:p]
if isinstance(indices, int):
indices = [indices]
images = [self.get_atoms(i) for i in indices]
if len(filename) > 4 and filename[-4:] in ['.eps', '.png', '.pov']:
write(filename, images,
rotation=rotations,
bbox=bbox, **kwargs)
else:
write(filename, images, **kwargs)
def get_atoms(self, frame, remove_hidden=False):
atoms = self[frame]
try:
E = atoms.get_potential_energy()
except RuntimeError:
E = None
try:
F = atoms.get_forces()
except RuntimeError:
F = None
# Remove hidden atoms if applicable
if remove_hidden:
atoms = atoms[self.visible]
if F is not None:
F = F[self.visible]
atoms.calc = SinglePointCalculator(atoms, energy=E, forces=F)
return atoms
def delete(self, i):
self._images.pop(i)
self.filenames.pop(i)
self.initialize(self._images, self.filenames)
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