def calculate_eos(atoms, npoints=5, eps=0.04, trajectory=None, callback=None):
"""Calculate equation-of-state.
atoms: Atoms object
System to calculate EOS for. Must have a calculator attached.
npoints: int
Number of points.
eps: float
Variation in volume from v0*(1-eps) to v0*(1+eps).
trajectory: Trjectory object or str
Write configurations to a trajectory file.
callback: function
Called after every energy calculation.
>>> from ase.build import bulk
>>> from ase.calculators.emt import EMT
>>> a = bulk('Cu', 'fcc', a=3.6)
>>> a.calc = EMT()
>>> eos = calculate_eos(a, trajectory='Cu.traj')
>>> v, e, B = eos.fit()
>>> a = (4 * v)**(1 / 3.0)
>>> print('{0:.6f}'.format(a))
3.589825
"""
# Save original positions and cell:
p0 = atoms.get_positions()
c0 = atoms.get_cell()
if isinstance(trajectory, basestring):
from ase.io import Trajectory
trajectory = Trajectory(trajectory, 'w', atoms)
if trajectory is not None:
trajectory.set_description({'type': 'eos',
'npoints': npoints,
'eps': eps})
try:
energies = []
volumes = []
for x in np.linspace(1 - eps, 1 + eps, npoints)**(1 / 3):
atoms.set_cell(x * c0, scale_atoms=True)
volumes.append(atoms.get_volume())
energies.append(atoms.get_potential_energy())
if callback:
callback()
if trajectory is not None:
trajectory.write()
return EquationOfState(volumes, energies)
finally:
atoms.cell = c0
atoms.positions = p0
if trajectory is not None:
trajectory.close()
import sys
from ase.test import NotAvailable, must_raise
if sys.platform in ['win32']:
raise NotAvailable('Fails on Windows '
'https://trac.fysik.dtu.dk/projects/ase/ticket/62')
import os
from ase import Atom, Atoms
from ase.io import Trajectory, read
from ase.constraints import FixBondLength
co = Atoms([Atom('C', (0, 0, 0)),
Atom('O', (0, 0, 1.2))])
traj = Trajectory('1.traj', 'w', co)
for i in range(5):
co.positions[:, 2] += 0.1
traj.write()
traj = Trajectory('1.traj', 'a')
co = read('1.traj')
print(co.positions)
co.positions[:] += 1
traj.write(co)
for a in Trajectory('1.traj'):
print(1, a.positions[-1, 2])
co.positions[:] += 1
t = Trajectory('1.traj', 'a')
t.write(co)
N = len(initial) # number of atoms
# Make a mask of zeros and ones that select fixed atoms - the two
# bottom layers:
mask = initial.positions[:, 2] - min(initial.positions[:, 2]) < 1.5 * h
constraint = FixAtoms(mask=mask)
initial.set_constraint(constraint)
# Calculate using EMT:
initial.set_calculator(EMT())
# Relax the initial state:
QuasiNewton(initial).run(fmax=0.05)
e0 = initial.get_potential_energy()
traj = Trajectory('dimer_along.traj', 'w', initial)
traj.write()
# Making dimer mask list:
d_mask = [False] * (N - 1) + [True]
# Set up the dimer:
d_control = DimerControl(initial_eigenmode_method='displacement',
displacement_method='vector',
logfile=None,
mask=d_mask)
d_atoms = MinModeAtoms(initial, d_control)
# Displacement settings:
displacement_vector = np.zeros((N, 3))
# Strength of displacement along y axis = along row:
# creates: lattice_constant.csv
import numpy as np
a0 = 3.52 / np.sqrt(2)
c0 = np.sqrt(8 / 3.0) * a0
from ase.io import Trajectory
traj = Trajectory('Ni.traj', 'w')
from ase.lattice import bulk
from ase.calculators.emt import EMT
eps = 0.01
for a in a0 * np.linspace(1 - eps, 1 + eps, 3):
for c in c0 * np.linspace(1 - eps, 1 + eps, 3):
ni = bulk('Ni', 'hcp', a=a, c=c)
ni.set_calculator(EMT())
ni.get_potential_energy()
traj.write(ni)
from ase.io import read
configs = read('Ni.traj@:')
energies = [config.get_potential_energy() for config in configs]
a = np.array([config.cell[0, 0] for config in configs])
c = np.array([config.cell[2, 2] for config in configs])
functions = np.array([a**0, a, c, a**2, a * c, c**2])
p = np.linalg.lstsq(functions.T, energies)[0]
p0 = p[0]
p1 = p[1:3]
p2 = np.array([(2 * p[3], p[4]),
linspace = (1.0, 1.0, 1) # eos numpy's linspace
linspacestr = ''.join([str(t) + 'x' for t in linspace])[:-1]
code = category + '_gpaw' + '-' + mode + str(e) + '_c' + str(constant_basis)
code = code + '_e' + linspacestr
code = code + '_k' + str(kptdensity) + '_w' + str(width)
code = code + '_r' + str(relativistic)
for name in names:
# save all steps in one traj file in addition to the database
# we should only used the database c.reserve, but here
# traj file is used as another lock ...
fd = opencew(name + '_' + code + '.traj')
if fd is None:
continue
traj = Trajectory(name + '_' + code + '.traj', 'w')
atoms = collection[name]
cell = atoms.get_cell()
kpts = tuple(kpts2mp(atoms, kptdensity, even=True))
kwargs = {}
if mode == 'fd':
if constant_basis:
# gives more smooth EOS in fd mode
kwargs.update({'gpts': h2gpts(e, cell)})
else:
kwargs.update({'h': e})
elif mode == 'pw':
if constant_basis:
kwargs.update({'mode': PW(e, cell=cell)})
else:
kwargs.update({'mode': PW(e)})
import numpy as np
from ase import Atoms
from ase.calculators.emt import EMT
from ase.io import Trajectory
Cu = Atoms('Cu', pbc=(1, 0, 0), calculator=EMT())
traj = Trajectory('Cu.traj', 'w')
for a in np.linspace(2.0, 4.0, 20):
Cu.set_cell([a, 1, 1], scale_atoms=True)
traj.write(Cu)
from ase.calculators.emt import EMT
from ase.collections import dcdft
from ase.io import Trajectory
for symbol in ['Al', 'Ni', 'Cu', 'Pd', 'Ag', 'Pt', 'Au']:
traj = Trajectory('{}.traj'.format(symbol), 'w')
for s in range(94, 108, 2):
atoms = dcdft[symbol]
atoms.set_cell(atoms.cell * (s / 100)**(1 / 3), scale_atoms=True)
atoms.calc = EMT()
atoms.get_potential_energy()
traj.write(atoms)
def execute_one_neb(self, n_cur, to_run, climb=False, many_steps=False):
'''Internal method which executes one NEB optimization.'''
self.iteration += 1
# First we copy around all the images we are not using in this
# neb (for reproducability purposes)
if self.world.rank == 0:
for i in range(n_cur):
if i not in to_run[1:-1]:
filename = '%s%03d.traj' % (self.prefix, i)
t = Trajectory(filename,
mode='w',
atoms=self.all_images[i])
t.write()
filename_ref = self.iter_folder + \
'/%s%03diter%03d.traj' % (self.prefix, i,
self.iteration)
if os.path.isfile(filename):
shutil.copy2(filename, filename_ref)
if self.world.rank == 0:
print('Now starting iteration %d on ' % self.iteration, to_run)
# Attach calculators to all the images we will include in the NEB
self.attach_calculators([self.all_images[i] for i in to_run[1:-1]])
neb = NEB([self.all_images[i] for i in to_run],
k=[self.k[i] for i in to_run[0:-1]],
method=self.method,
parallel=self.parallel,
remove_rotation_and_translation=self.
remove_rotation_and_translation,
climb=climb)
# Do the actual NEB calculation
qn = self.optimizer(neb,
logfile=self.iter_folder + '/%s_log_iter%03d.log' %
(self.prefix, self.iteration))
# Find the ranks which are masters for each their calculation
if self.parallel:
nneb = to_run[0]
nim = len(to_run) - 2
n = self.world.size // nim # number of cpu's per image
j = 1 + self.world.rank // n # my image number
assert nim * n == self.world.size
traj = Trajectory('%s%03d.traj' % (self.prefix, j + nneb),
'w',
self.all_images[j + nneb],
master=(self.world.rank % n == 0))
filename_ref = self.iter_folder + \
'/%s%03diter%03d.traj' % (self.prefix,
j + nneb, self.iteration)
trajhist = Trajectory(filename_ref,
'w',
self.all_images[j + nneb],
master=(self.world.rank % n == 0))
qn.attach(traj)
qn.attach(trajhist)
else:
num = 1
for i, j in enumerate(to_run[1:-1]):
filename_ref = self.iter_folder + \
'/%s%03diter%03d.traj' % (self.prefix, j, self.iteration)
trajhist = Trajectory(filename_ref, 'w', self.all_images[j])
qn.attach(seriel_writer(trajhist, i, num).write)
traj = Trajectory('%s%03d.traj' % (self.prefix, j), 'w',
self.all_images[j])
qn.attach(seriel_writer(traj, i, num).write)
num += 1
if isinstance(self.maxsteps, (list, tuple)) and many_steps:
steps = self.maxsteps[1]
elif isinstance(self.maxsteps, (list, tuple)) and not many_steps:
steps = self.maxsteps[0]
else:
steps = self.maxsteps
if isinstance(self.fmax, (list, tuple)) and many_steps:
fmax = self.fmax[1]
elif isinstance(self.fmax, (list, tuple)) and not many_steps:
fmax = self.fmax[0]
else:
fmax = self.fmax
qn.run(fmax=fmax, steps=steps)
# Remove the calculators and replace them with single
# point calculators and update all the nodes for
# preperration for next iteration
neb.distribute = types.MethodType(store_E_and_F_in_spc, neb)
neb.distribute()
# Set calculator
# loop a number of times to capture if minimization stops with high force
# due to the VariansBreak calls
niter = 0
# If the structure is already fully relaxed just return it
traj = Trajectory(label + '_lcao.traj', 'w', structure)
while (structure.get_forces()**
2).sum(axis=1).max()**0.5 > forcemax and niter < niter_max:
dyn = BFGS(structure, logfile=label + '.log')
vb = VariansBreak(structure, dyn, min_stdev=0.01, N=15)
dyn.attach(traj)
dyn.attach(vb)
dyn.run(fmax=forcemax, steps=steps)
niter += 1
#print('relaxgpaw over',flush=True)
return structure
calc = GPAW(mode=PW(500), xc='PBE', basis='dzp', kpts=(3, 3, 1))
traj = Trajectory('V2O5_2H2OTiO2_101_DFTrelaxed.traj', 'w')
name = 'V2O5_2H2OTiO2_101surface_gm'
data = read('V2O5_2H2O_TiO2_I3s.traj@:')
for i in range(0, len(data)):
name = 'V2O5_2H2OTiO2_101surface_isomer_{}'.format(i)
a = data[i]
a.set_calculator(calc)
a_relaxed = relaxGPAW(a, name, forcemax=0.01, niter_max=2, steps=100)
traj.write(a_relaxed)
def polyfit(x, y, order=3):
"""Fit polynomium at points in x to values in y.
With D dimensions and N points, x must have shape (N, D) and y
must have length N."""
p = NDPoly(len(x[0]), order)
p.fit(x, y)
return p
a0 = 3.52 / np.sqrt(2)
c0 = np.sqrt(8 / 3.0) * a0
print('%.4f %.3f' % (a0, c0 / a0))
for i in range(3):
traj = Trajectory('Ni.traj', 'w')
eps = 0.01
for a in a0 * np.linspace(1 - eps, 1 + eps, 4):
for c in c0 * np.linspace(1 - eps, 1 + eps, 4):
ni = bulk('Ni', 'hcp', a=a, covera=c / a)
ni.set_calculator(EMT())
ni.get_potential_energy()
traj.write(ni)
traj.close()
configs = read('Ni.traj@:')
energies = [config.get_potential_energy() for config in configs]
ac = [(config.cell[0, 0], config.cell[2, 2]) for config in configs]
p = polyfit(ac, energies, 2)
from scipy.optimize import fmin_bfgs
a0, c0 = fmin_bfgs(p, (a0, c0))
import sys
from ase.test import NotAvailable, must_raise
if sys.platform in ['win32']:
raise NotAvailable('Fails on Windows '
'https://trac.fysik.dtu.dk/projects/ase/ticket/62')
import os
from ase import Atom, Atoms
from ase.io import Trajectory, read
co = Atoms([Atom('C', (0, 0, 0)),
Atom('O', (0, 0, 1.2))])
traj = Trajectory('1.traj', 'w', co)
for i in range(5):
co.positions[:, 2] += 0.1
traj.write()
traj = Trajectory('1.traj', 'a')
co = read('1.traj')
print(co.positions)
co.positions[:] += 1
traj.write(co)
for a in Trajectory('1.traj'):
print(1, a.positions[-1, 2])
co.positions[:] += 1
t = Trajectory('1.traj', 'a')
t.write(co)
assert len(t) == 7
