def interp_by_neb(initial, final, n_images, interp='idpp',
calculator=None, constraint=None, fmax=0.5, steps=10,
**kwargs):
"""Interpolate between the initial and final points by NEB method.
:param initial: The initial image.
:param final: The final image.
:param int n_images: The number of image between the initial and final
images.
:param string interp: The interpolation method.
:param Callable calculator: The callable to generate calculators for the
images. It can be set to None if no real optimization is intended.
:param constraint: The constraint for the images.
:param fmax: The maximal force to stop the optimization.
:param steps: The number of optimization steps allowed.
:param kwargs: All other keyword arguments are forwarded to the
initializer of the ASE NEB class.
:return: The list of images between the points.
"""
# To circumvent the error from interpolation when we have no middle images.
if n_images == 0:
return [initial, final]
images = [initial]
for _ in range(n_images):
image = initial.copy()
images.append(image)
if calculator is not None:
image.set_calculator(calculator())
if constraint is not None:
image.set_constraint(constraint)
continue
images.append(final)
neb = NEB(images, **kwargs)
neb.interpolate(method=interp)
if calculator is not None:
dyn = MDMin(neb)
dyn.run(fmax=fmax, steps=steps)
return neb.images
def test_unitcellfilter_hcp(asap3, testdir):
cu = bulk('Cu', 'hcp', a=3.6 / 2.0**0.5)
cu.cell[1, 0] -= 0.05
cu *= (6, 6, 3)
cu.calc = asap3.EMT()
print(cu.get_forces())
print(cu.get_stress())
f = UnitCellFilter(cu)
opt = MDMin(f, dt=0.01)
with Trajectory('Cu-hcp.traj', 'w', cu) as t:
opt.attach(t)
opt.run(0.2)
xc=xc,
kpts=kpts,
parallel={'band': 1},
txt='neb{}.txt'.format(j),
communicator=ranks)
image.set_calculator(calc_ase)
images_ase.append(image)
images_ase.append(final_ase)
neb_ase = NEB(images_ase, parallel=True, climb=True)
neb_ase.interpolate(method='idpp')
qn_ase = MDMin(neb_ase, logfile='neb_ase.log', trajectory='neb_ase.traj')
itime = time.default_timer()
qn_ase.run(fmax=0.05)
logging.warning('ase = %s', time.default_timer() - itime)
# 2.B. NEB using CatLearn
neb_catlearn = MLNEB(start=slab_initial,
end=slab_final,
ase_calc=calc,
n_images=n_images + 2,
interpolation='idpp',
restart=False)
itime = time.default_timer()
neb_catlearn.run(fmax=0.05, trajectory='ML-NEB.traj')
# 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)
print(mask)
for image in images:
# Let all images use an EMT calculator:
image.set_calculator(EMT())
image.set_constraint(constraint)
# Relax the initial and final states:
QuasiNewton(initial).run(fmax=0.05)
QuasiNewton(final).run(fmax=0.05)
# Create a Nudged Elastic Band:
neb = NEB(images)
# Make a starting guess for the minimum energy path (a straight line
# from the initial to the final state):
neb.interpolate()
# Relax the NEB path:
minimizer = MDMin(neb)
minimizer.run(fmax=0.05)
# Write the path to a trajectory:
view(images) # 126 meV
write('jump1.traj', images)
print 'Starting NEB run with %d images' % len(neb.images)
if not os.path.exists('%s-initial.xyz' % basename):
neb.write('%s-initial.xyz' % basename)
if opt.eval:
# actually evaluate end forces as well
neb.get_forces(all=True)
neb.write('%s-eval.xyz' % basename)
elif not opt.dry_run:
# Optimize:
if opt.optimizer == 'FIRE':
from ase.optimize.fire import FIRE
optimizer = FIRE(neb)
elif opt.optimizer == 'MDMin':
from ase.optimize import MDMin
optimizer = MDMin(neb)
else:
p.error('Unknown optimizer %s' % opt.optimizer)
if opt.write_traj is not None:
def write_traj():
global neb
n = 0
while os.path.exists('%s-band-%d.xyz' % (basename, n)):
n += 1
neb.write('%s-band-%d.xyz' % (basename, n))
optimizer.attach(write_traj, interval=opt.write_traj)
optimizer.run(fmax=opt.fmax)
def run(self,
fmax=0.05,
steps=200,
kernel='SQE',
max_step=0.25,
acq='min_energy',
full_output=False,
noise=0.005):
"""Executing run will start the optimization process.
Parameters
----------
fmax : float
Convergence criteria (in eV/Angstrom).
steps : int
Max. number of optimization steps.
kernel: string
Type of covariance function to be used.
Implemented are: SQE (fixed hyperparamters), SQE_opt and ARD_SQE.
max_step: float
Early stopping criteria. Maximum uncertainty before stopping the
optimization in the predicted landscape.
acq : string
The acquisition function that decides the next point to
evaluate. Implemented are: 'lcb', 'ucb', 'min_energy'.
full_output: boolean
Whether to print on screen the full output (True) or not (False).
noise:
Regularization parameter of the GP.
Returns
-------
Optimized atom structure.
"""
self.fmax = fmax
self.acq = acq
success_hyper = False
while not converged(self):
# 1. Train Machine Learning model.
train = np.copy(self.list_train)
targets = np.copy(self.list_targets)
gradients = np.copy(self.list_gradients)
self.u_prior = np.max(targets)
scaled_targets = targets - self.u_prior
sigma_f = 1e-3 + np.std(scaled_targets)**2
if kernel == 'SQE_fixed':
opt_hyper = False
kdict = [{
'type': 'gaussian',
'width': 0.4,
'dimension': 'single',
'bounds': ((0.4, 0.4), ),
'scaling': 1.0,
'scaling_bounds': ((1.0, 1.0), )
}, {
'type':
'noise_multi',
'hyperparameters': [noise * 0.4**2, noise],
'bounds': (
(noise * 0.4**2, noise * 0.4**2),
(noise, noise),
)
}]
if kernel == 'SQE':
opt_hyper = True
kdict = [{
'type': 'gaussian',
'width': 0.4,
'dimension': 'single',
'bounds': ((0.01, 1.0), ),
'scaling': sigma_f,
'scaling_bounds': ((sigma_f, sigma_f), )
}, {
'type':
'noise_multi',
'hyperparameters': [noise, noise * 0.4**2],
'bounds': (
(noise / 5., noise * 10.),
(noise / 5. * 0.4**2, noise * 10.),
)
}]
if kernel == 'ARD_SQE':
opt_hyper = True
kdict = [{
'type': 'gaussian',
'width': 0.4,
'dimension': 'features',
'bounds': ((0.01, 1.0), ) * len(self.index_mask),
'scaling': sigma_f,
'scaling_bounds': ((sigma_f, sigma_f), )
}, {
'type':
'noise_multi',
'hyperparameters': [noise / 2., noise / 10.],
'bounds': (
(noise / 5., noise),
(noise / 10., noise / 4.),
)
}]
if len(self.list_targets) == 1:
opt_hyper = False
kdict = [{
'type': 'gaussian',
'width': 0.20,
'dimension': 'single',
'bounds': ((0.20, 0.20), ),
'scaling': sigma_f,
'scaling_bounds': ((sigma_f, sigma_f), )
}, {
'type':
'noise_multi',
'hyperparameters': [noise * 0.4**2, noise],
'bounds': (
(noise * 0.4**2, noise * 0.4**2),
(noise, noise),
)
}]
if success_hyper is not False:
kdict = success_hyper
if self.index_mask is not None:
train = apply_mask(list_to_mask=train,
mask_index=self.index_mask)[1]
gradients = apply_mask(list_to_mask=gradients,
mask_index=self.index_mask)[1]
parprint('Training a GP process...')
parprint('Number of training points:', len(scaled_targets))
train = train.tolist()
gradients = gradients.tolist()
self.gp = fit(train, scaled_targets, gradients, kdict)
if opt_hyper is True:
if len(self.list_targets) > 5:
self.gp.optimize_hyperparameters()
if self.gp.theta_opt.success is True:
if full_output is True:
parprint(
'Hyperparam. optimization was successful.')
parprint('Updating kernel list...')
success_hyper = self.gp.kernel_list
if self.gp.theta_opt.success is not True:
if full_output is True:
parprint('Hyperparam. optimization unsuccessful.')
if success_hyper is False:
if full_output is True:
parprint('Not enough data...')
if success_hyper is not False:
if full_output is True:
parprint('Using the last optimized '
'hyperparamters.')
if full_output is True:
parprint('Kernel list:', self.gp.kernel_list)
# 2. Optimize Machine Learning model.
self.list_interesting_points = []
self.list_interesting_energies = []
self.list_interesting_uncertainties = []
guess = self.ase_ini
guess_pos = np.array(self.list_train[-1])
guess.positions = guess_pos.reshape(-1, 3)
guess.set_calculator(
ASECalc(gp=self.gp,
index_constraints=self.index_mask,
scaling_targets=self.u_prior))
# Optimization in the predicted landscape:
ml_opt = MDMin(guess, trajectory=None, logfile=None, dt=0.020)
if full_output is True:
parprint('Starting optimization on the predicted landscape...')
ml_converged = False
n_steps_performed = 0
while ml_converged is False:
ml_opt.run(fmax=fmax * 0.90, steps=1)
pos_ml = np.array(guess.positions).flatten()
self.list_interesting_points.append(pos_ml)
pos_ml = apply_mask([pos_ml], mask_index=self.index_mask)[1]
pred_ml = self.gp.predict(test_fp=pos_ml, uncertainty=True)
energy_ml = pred_ml['prediction'][0][0]
unc_ml = pred_ml['uncertainty_with_reg'][0]
self.list_interesting_energies.append(energy_ml)
self.list_interesting_uncertainties.append(unc_ml)
n_steps_performed += 1
if n_steps_performed > 1000:
if full_output is True:
parprint('Not converged yet...')
ml_converged = True
if unc_ml >= max_step:
if full_output is True:
parprint('Maximum uncertainty reach. Early stop.')
ml_converged = True
if ml_opt.converged():
if full_output is True:
parprint('ML optimized.')
ml_converged = True
# Acquisition functions:
acq_pred = np.array(self.list_interesting_energies)
acq_unc = np.array(self.list_interesting_uncertainties)
if self.acq == 'ucb':
acq_values = UCB(predictions=acq_pred,
uncertainty=acq_unc,
objective='min',
kappa=-1.0)
if self.acq == 'lcb':
e_minus_unc = np.array(self.list_interesting_energies) - \
np.array(self.list_interesting_uncertainties)
acq_values = -e_minus_unc
if self.acq == 'min_energy':
acq_values = -np.array(self.list_interesting_energies)
max_score = np.argmax(acq_values)
self.interesting_point = self.list_interesting_points[max_score]
# 3. Evaluate and append interesting point.
if full_output is True:
parprint('Performing evaluation in the real landscape...')
eval_atom = self.ase_ini
pos_atom = self.interesting_point
eval_atom.positions = np.array(pos_atom).reshape((-1, 3))
eval_atom.set_calculator(self.ase_calc)
energy_atom = eval_atom.get_potential_energy(
force_consistent=self.fc)
forces_atom = -eval_atom.get_forces().reshape(-1)
# 4. Convergence and output.
self.list_train.append(pos_atom)
self.list_targets.append(energy_atom)
self.list_gradients.append(forces_atom)
self.list_fmax = get_fmax(np.array([self.list_gradients[-1]]))
self.max_abs_forces = np.max(np.abs(self.list_fmax))
self.list_max_abs_forces.append(self.max_abs_forces)
self.iter += 1
print_info(self)
# Save evaluated image.
self.list_atoms += [eval_atom]
TrajectoryWriter(atoms=self.ase_ini,
filename=self.filename,
mode='a').write()
# Maximum number of iterations reached.
if self.iter >= steps:
parprint(
'Not converged. Maximum number of iterations reached.')
break
images = [Atoms(initial)]
images += [Atoms(initial.copy()) for i in range(n_images)]
images += [Atoms(final)]
neb = NEB(images, k=0.1)
neb.interpolate()
for img in images:
img.set_calculator(model.calculator)
ase.io.write(sys.stdout, img, 'extxyz')
# perturb intermediate images
for img in images[1:-1]:
img.rattle(0.05)
# optimizer = FIRE(neb)
optimizer = MDMin(neb, dt=0.05)
optimizer.run(fmax=fmax)
neb_traj = open('model-' + model.name + '-vacancy-path.neb.xyz', 'w')
ase.io.write(neb_traj, neb.images, format='extxyz')
neb_traj.close()
Es = []
for img in images:
Es.append(img.get_potential_energy() - e_bulk_per_atom * len(img))
ase.io.write(sys.stdout, img, 'extxyz')
# dictionary of computed properties - this is output of this test, to
# be compared with other models
properties = {'vacancy_path': Es}
def main():
"""Adopted from ase/test/stress.py"""
# setup a Fist Lennard-Jones Potential
inp = """&FORCE_EVAL
&MM
&FORCEFIELD
&SPLINE
EMAX_ACCURACY 500.0
EMAX_SPLINE 1000.0
EPS_SPLINE 1.0E-9
&END
&NONBONDED
&LENNARD-JONES
atoms Ar Ar
EPSILON [eV] 1.0
SIGMA [angstrom] 1.0
RCUT [angstrom] 10.0
&END LENNARD-JONES
&END NONBONDED
&CHARGE
ATOM Ar
CHARGE 0.0
&END CHARGE
&END FORCEFIELD
&POISSON
&EWALD
EWALD_TYPE none
&END EWALD
&END POISSON
&END MM
&END FORCE_EVAL"""
calc = CP2K(label="test_stress", inp=inp, force_eval_method="Fist")
# Theoretical infinite-cutoff LJ FCC unit cell parameters
vol0 = 4 * 0.91615977036 # theoretical minimum
a0 = vol0**(1 / 3)
a = bulk('Ar', 'fcc', a=a0)
cell0 = a.get_cell()
a.calc = calc
a.set_cell(np.dot(a.cell,
[[1.02, 0, 0.03], [0, 0.99, -0.02], [0.1, -0.01, 1.03]]),
scale_atoms=True)
a *= (1, 2, 3)
cell0 *= np.array([1, 2, 3])[:, np.newaxis]
a.rattle()
# Verify analytical stress tensor against numerical value
s_analytical = a.get_stress()
s_numerical = a.calc.calculate_numerical_stress(a, 1e-5)
s_p_err = 100 * (s_numerical - s_analytical) / s_numerical
print("Analytical stress:\n", s_analytical)
print("Numerical stress:\n", s_numerical)
print("Percent error in stress:\n", s_p_err)
assert np.all(abs(s_p_err) < 1e-5)
# Minimize unit cell
opt = MDMin(UnitCellFilter(a), dt=0.01)
opt.run(fmax=1e-3)
# Verify minimized unit cell using Niggli tensors
g_minimized = np.dot(a.cell, a.cell.T)
g_theory = np.dot(cell0, cell0.T)
g_p_err = 100 * (g_minimized - g_theory) / g_theory
print("Minimized Niggli tensor:\n", g_minimized)
print("Theoretical Niggli tensor:\n", g_theory)
print("Percent error in Niggli tensor:\n", g_p_err)
assert np.all(abs(g_p_err) < 1)
print('passed test "stress"')
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / 2 / deps / vol
print(v, s, abs(s - sigma_vv[v, v]))
assert abs(s - sigma_vv[v, v]) < 1e-7
for v1 in range(3):
v2 = (v1 + 1) % 3
x = np.eye(3)
x[v1, v2] = deps
x[v2, v1] = deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
ep = a.calc.get_potential_energy(a, force_consistent=True)
x[v1, v2] = -deps
x[v2, v1] = -deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / deps / 4 / vol
print(v1, v2, s, abs(s - sigma_vv[v1, v2]))
assert abs(s - sigma_vv[v1, v2]) < 1e-7
opt = MDMin(UnitCellFilter(a), dt=0.01)
opt.run(fmax=0.5)
print(a.cell)
for i in range(3):
for j in range(3):
x = np.dot(a.cell[i], a.cell[j])
y = (i + 1) * (j + 1) * a0**2 / 2
if i != j:
y /= 2
print(i, j, x, (x - y) / x)
assert abs((x - y) / x) < 0.01
scale_atoms=True)
a *= (1, 2, 3)
cell0 *= np.array([1, 2, 3])[:, np.newaxis]
a.rattle()
# Verify analytical stress tensor against numerical value
s_analytical = a.get_stress()
s_numerical = a.calc.calculate_numerical_stress(a, 1e-5)
s_p_err = 100 * (s_numerical - s_analytical) / s_numerical
print("Analytical stress:\n", s_analytical)
print("Numerical stress:\n", s_numerical)
print("Percent error in stress:\n", s_p_err)
assert np.all(abs(s_p_err) < 1e-5)
# Minimize unit cell
opt = MDMin(UnitCellFilter(a), dt=0.01)
opt.run(fmax=1e-3)
# Verify minimized unit cell using Niggli tensors
g_minimized = np.dot(a.cell, a.cell.T)
g_theory = np.dot(cell0, cell0.T)
g_p_err = 100 * (g_minimized - g_theory) / g_theory
print("Minimized Niggli tensor:\n", g_minimized)
print("Theoretical Niggli tensor:\n", g_theory)
print("Percent error in Niggli tensor:\n", g_p_err)
assert np.all(abs(g_p_err) < 1)
def main():
"""Adopted from ase/test/stress.py"""
if "ASE_CP2K_COMMAND" not in os.environ:
raise NotAvailable('$ASE_CP2K_COMMAND not defined')
# setup a Fist Lennard-Jones Potential
inp = """&FORCE_EVAL
&MM
&FORCEFIELD
&SPLINE
EMAX_ACCURACY 500.0
EMAX_SPLINE 1000.0
EPS_SPLINE 1.0E-9
&END
&NONBONDED
&LENNARD-JONES
atoms Ar Ar
EPSILON [eV] 1.0
SIGMA [angstrom] 1.0
RCUT [angstrom] 10.0
&END LENNARD-JONES
&END NONBONDED
&CHARGE
ATOM Ar
CHARGE 0.0
&END CHARGE
&END FORCEFIELD
&POISSON
&EWALD
EWALD_TYPE none
&END EWALD
&END POISSON
&END MM
&END FORCE_EVAL"""
calc = CP2K(label="test_stress", inp=inp, force_eval_method="Fist")
vol0 = 4 * 0.91615977036 # theoretical minimum
a0 = vol0**(1 / 3)
a = bulk('Ar', 'fcc', a=a0)
a.calc = calc
a.set_cell(np.dot(a.cell,
[[1.02, 0, 0.03], [0, 0.99, -0.02], [0.1, -0.01, 1.03]]),
scale_atoms=True)
a *= (1, 2, 3)
a.rattle()
sigma_vv = a.get_stress(voigt=False)
# print(sigma_vv)
# print(a.get_potential_energy() / len(a))
vol = a.get_volume()
# compare stress tensor with numeric derivative
deps = 1e-5
cell = a.cell.copy()
for v in range(3):
x = np.eye(3)
x[v, v] += deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
ep = a.calc.get_potential_energy(a, force_consistent=True)
x[v, v] -= 2 * deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / 2 / deps / vol
# print(v, s, abs(s - sigma_vv[v, v]))
assert abs(s - sigma_vv[v, v]) < 1e-7
for v1 in range(3):
v2 = (v1 + 1) % 3
x = np.eye(3)
x[v1, v2] = deps
x[v2, v1] = deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
ep = a.calc.get_potential_energy(a, force_consistent=True)
x[v1, v2] = -deps
x[v2, v1] = -deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / deps / 4 / vol
# print(v1, v2, s, abs(s - sigma_vv[v1, v2]))
assert abs(s - sigma_vv[v1, v2]) < 1e-7
# run a cell optimization, see if it finds back original crystal structure
opt = MDMin(UnitCellFilter(a), dt=0.01, logfile=None)
opt.run(fmax=0.5)
# print(a.cell)
for i in range(3):
for j in range(3):
x = np.dot(a.cell[i], a.cell[j])
y = (i + 1) * (j + 1) * a0**2 / 2
if i != j:
y /= 2
# print(i, j, x, (x - y) / x)
assert abs((x - y) / x) < 0.01
print('passed test "stress"')
def main():
"""Adopted from ase/test/stress.py"""
if "ASE_CP2K_COMMAND" not in os.environ:
raise NotAvailable('$ASE_CP2K_COMMAND not defined')
# setup a Fist Lennard-Jones Potential
inp = """&FORCE_EVAL
&MM
&FORCEFIELD
&SPLINE
EMAX_ACCURACY 500.0
EMAX_SPLINE 1000.0
EPS_SPLINE 1.0E-9
&END
&NONBONDED
&LENNARD-JONES
atoms Ar Ar
EPSILON [eV] 1.0
SIGMA [angstrom] 1.0
RCUT [angstrom] 10.0
&END LENNARD-JONES
&END NONBONDED
&CHARGE
ATOM Ar
CHARGE 0.0
&END CHARGE
&END FORCEFIELD
&POISSON
&EWALD
EWALD_TYPE none
&END EWALD
&END POISSON
&END MM
&END FORCE_EVAL"""
calc = CP2K(label="test_stress", inp=inp, force_eval_method="Fist")
# Theoretical infinite-cutoff LJ FCC unit cell parameters
vol0 = 4 * 0.91615977036 # theoretical minimum
a0 = vol0 ** (1 / 3)
a = bulk('Ar', 'fcc', a=a0)
cell0 = a.get_cell()
a.calc = calc
a.set_cell(np.dot(a.cell,
[[1.02, 0, 0.03],
[0, 0.99, -0.02],
[0.1, -0.01, 1.03]]),
scale_atoms=True)
a *= (1, 2, 3)
cell0 *= np.array([1, 2, 3])[:, np.newaxis]
a.rattle()
# Verify analytical stress tensor against numerical value
s_analytical = a.get_stress()
s_numerical = a.calc.calculate_numerical_stress(a, 1e-5)
s_p_err = 100 * (s_numerical - s_analytical) / s_numerical
print("Analytical stress:\n", s_analytical)
print("Numerical stress:\n", s_numerical)
print("Percent error in stress:\n", s_p_err)
assert np.all(abs(s_p_err) < 1e-5)
# Minimize unit cell
opt = MDMin(UnitCellFilter(a), dt=0.01)
opt.run(fmax=1e-3)
# Verify minimized unit cell using Niggli tensors
g_minimized = np.dot(a.cell, a.cell.T)
g_theory = np.dot(cell0, cell0.T)
g_p_err = 100 * (g_minimized - g_theory) / g_theory
print("Minimized Niggli tensor:\n", g_minimized)
print("Theoretical Niggli tensor:\n", g_theory)
print("Percent error in Niggli tensor:\n", g_p_err)
assert np.all(abs(g_p_err) < 1)
print('passed test "stress"')
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / 2 / deps / vol
print(v, s, abs(s - sigma_vv[v, v]))
assert abs(s - sigma_vv[v, v]) < 1e-7
for v1 in range(3):
v2 = (v1 + 1) % 3
x = np.eye(3)
x[v1, v2] = deps
x[v2, v1] = deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
ep = a.calc.get_potential_energy(a, force_consistent=True)
x[v1, v2] = -deps
x[v2, v1] = -deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / deps / 4 / vol
print(v1, v2, s, abs(s - sigma_vv[v1, v2]))
assert abs(s - sigma_vv[v1, v2]) < 1e-7
opt = MDMin(UnitCellFilter(a), dt=0.01)
opt.run(fmax=0.5)
print(a.cell)
for i in range(3):
for j in range(3):
x = np.dot(a.cell[i], a.cell[j])
y = (i + 1) * (j + 1) * a0**2 / 2
if i != j:
y /= 2
print(i, j, x, (x - y) / x)
assert abs((x - y) / x) < 0.01
# 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)
print(mask)
for image in images:
# Let all images use an EMT calculator:
image.set_calculator(EMT())
image.set_constraint(constraint)
# Relax the initial and final states:
QuasiNewton(initial).run(fmax=0.05)
QuasiNewton(final).run(fmax=0.05)
# Create a Nudged Elastic Band:
neb = NEB(images)
# Make a starting guess for the minimum energy path (a straight line
# from the initial to the final state):
neb.interpolate()
# Relax the NEB path:
minimizer = MDMin(neb)
minimizer.run(fmax=0.05)
# Write the path to a trajectory:
view(images)
# 564 meV
write('jump2.traj', images)
from ase.structure import molecule
from ase.structure import nanotube
from ase.optimize import BFGS, MDMin
from asap3 import BrennerPotential
from asap3.testtools import ReportTest
import numpy as np
atoms = nanotube(5, 5, length=10)
atoms.set_calculator(BrennerPotential())
uc = atoms.get_cell()
l0 = uc[2,2]
e = -1e100
for eps in np.linspace(0, 0.5, 201):
uc[2,2] = l0 * (1 + eps)
atoms.set_cell(uc, scale_atoms=True)
dyn = MDMin(atoms, logfile=None, dt=0.05)
dyn.run(fmax=0.01, steps=100)
epot = atoms.get_potential_energy()
if epot > e:
e = epot
print "%.3f %f" % (eps, epot)
print "Maximal energy:", e
ReportTest("Maximal energy", e, -969.0, 5.0)
if abs(e - -620.98) < 1.0:
print "Bug 42 is back!"
xc = 'BEEF-vdW'
#################################################
vacuum = 8 # Angstrom
a = 2.53959*2 # Angstrom
input_structure = "str.cif"
fmaxx = 0.03
maxstep = 0.05
atoms = read(input_structure)
atoms.set_calculator(GPAW(xc=xc, kpts = kpoints, gpts=gpoints, txt='bfgs.txt'))
cellpar = atoms.cell.cellpar()
scaled_pos = atoms.get_scaled_positions()
# Constraints- fix atoms in the first first unit cell from origin and the last two unit cells from origin
indices = []
for i in range(len(atoms)):
if atoms[i].symbol == 'C':
indices.append(i)
elif scaled_pos[i][0] <= (3*a/2 + vacuum)/cellpar[0]:
indices.append(i)
elif scaled_pos[i][0] >= 1 - (vacuum + 5*a/2)/cellpar[0]:
indices.append(i)
atoms.set_constraint(FixAtoms(indices))
dyn=MDMin(atoms=atoms, trajectory='traj.traj', logfile = 'qn.log')
dyn.run(fmax=fmaxx)
def main():
"""Adopted from ase/test/stress.py"""
if "ASE_CP2K_COMMAND" not in os.environ:
raise NotAvailable('$ASE_CP2K_COMMAND not defined')
# setup a Fist Lennard-Jones Potential
inp = """&FORCE_EVAL
&MM
&FORCEFIELD
&SPLINE
EMAX_ACCURACY 500.0
EMAX_SPLINE 1000.0
EPS_SPLINE 1.0E-9
&END
&NONBONDED
&LENNARD-JONES
atoms Ar Ar
EPSILON [eV] 1.0
SIGMA [angstrom] 1.0
RCUT [angstrom] 10.0
&END LENNARD-JONES
&END NONBONDED
&CHARGE
ATOM Ar
CHARGE 0.0
&END CHARGE
&END FORCEFIELD
&POISSON
&EWALD
EWALD_TYPE none
&END EWALD
&END POISSON
&END MM
&END FORCE_EVAL"""
calc = CP2K(label="test_stress", inp=inp, force_eval_method="Fist")
vol0 = 4 * 0.91615977036 # theoretical minimum
a0 = vol0 ** (1 / 3)
a = bulk('Ar', 'fcc', a=a0)
a.calc = calc
a.set_cell(np.dot(a.cell,
[[1.02, 0, 0.03],
[0, 0.99, -0.02],
[0.1, -0.01, 1.03]]),
scale_atoms=True)
a *= (1, 2, 3)
a.rattle()
sigma_vv = a.get_stress(voigt=False)
# print(sigma_vv)
# print(a.get_potential_energy() / len(a))
vol = a.get_volume()
# compare stress tensor with numeric derivative
deps = 1e-5
cell = a.cell.copy()
for v in range(3):
x = np.eye(3)
x[v, v] += deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
ep = a.calc.get_potential_energy(a, force_consistent=True)
x[v, v] -= 2 * deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / 2 / deps / vol
# print(v, s, abs(s - sigma_vv[v, v]))
assert abs(s - sigma_vv[v, v]) < 1e-7
for v1 in range(3):
v2 = (v1 + 1) % 3
x = np.eye(3)
x[v1, v2] = deps
x[v2, v1] = deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
ep = a.calc.get_potential_energy(a, force_consistent=True)
x[v1, v2] = -deps
x[v2, v1] = -deps
a.set_cell(np.dot(cell, x), scale_atoms=True)
em = a.calc.get_potential_energy(a, force_consistent=True)
s = (ep - em) / deps / 4 / vol
# print(v1, v2, s, abs(s - sigma_vv[v1, v2]))
assert abs(s - sigma_vv[v1, v2]) < 1e-7
# run a cell optimization, see if it finds back original crystal structure
opt = MDMin(UnitCellFilter(a), dt=0.01, logfile=None)
opt.run(fmax=0.1)
# print(a.cell)
for i in range(3):
for j in range(3):
x = np.dot(a.cell[i], a.cell[j])
y = (i + 1) * (j + 1) * a0 ** 2 / 2
if i != j:
y /= 2
# print(i, j, x, (x - y) / x)
assert abs((x - y) / x) < 0.01
print('passed test "stress"')
initial_ase = read('initial_opt.traj')
final_ase = read('final_opt.traj')
constraint = FixAtoms(mask=[atom.tag > 1 for atom in initial_ase])
images_ase = [initial_ase]
for i in range(1, n_images - 1):
image = initial_ase.copy()
image.set_calculator(copy.deepcopy(ase_calculator))
images_ase.append(image)
images_ase.append(final_ase)
neb_ase = NEB(images_ase, climb=True, method='aseneb')
neb_ase.interpolate(method='idpp')
qn_ase = MDMin(neb_ase, trajectory='neb_ase.traj')
qn_ase.run(fmax=0.05)
# 2.B. NEB using CatLearn ####################################################
neb_catlearn = MLNEB(start='initial_opt.traj',
end='final_opt.traj',
ase_calc=copy.deepcopy(ase_calculator),
n_images=n_images,
interpolation='idpp',
restart=False)
neb_catlearn.run(fmax=0.05, trajectory='ML-NEB.traj')
# 3. Summary of the results #################################################
print_version(1)
size = 5
atoms = FaceCenteredCubic(size=(size,size,size), symbol="Cu", pbc=True)
defsize = atoms.get_volume()
atoms.set_cell(atoms.get_cell() * 1.1, scale_atoms=True)
atoms.set_calculator(EMT())
def printvol(a):
print "Volume:", a.get_volume(), " energy:",\
atoms.get_potential_energy() + atoms.get_kinetic_energy(),\
" stress:", atoms.get_stress()[:3]
f = StrainFilter(atoms, [1, 1, 1, 0, 0, 0])
opt = MDMin(f, logfile="/dev/null", dt=0.01/(atoms.get_cell()[0,0]))
printvol(atoms)
opt.attach(printvol, 10, atoms)
opt.run(0.01)
printvol(atoms)
print "Original vol:", defsize
print
stress = atoms.get_stress()
for i in range(6):
ReportTest("Stress component %d (T=0)" % (i,), stress[0], 0.0, 1e-5)
atoms = FaceCenteredCubic(size=(size,size,size), symbol="Cu", pbc=True)
atoms.set_calculator(EMT())
dyn = Langevin(atoms, 10*units.fs, 500*units.kB, 0.02)
dyn.attach(printvol, 100, atoms)
dyn.run(500)
pstress = patom.get_cell() * 0.0
fixstrain = np.ones((3, 3))
ref_atom = refatom.copy()
ref_coord = refatom.get_cell()
pstress[2][2] = 1.34523705e+01
# PK1 can be replaced by PK2 or Cauchy
pbox = stressbox(patom,
express=pstress,
fixstrain=fixstrain,
ref_atom=ref_atom,
stress_type='PK1')
dyn = MDMin(pbox)
#dyn=FIRE(pbox)
#dyn=BFGS(pbox)
f_max = 1E-6
dyn.run(fmax=f_max, steps=10000)
print('pk1 stress=', pbox.get_stress_pk1() / units.GPa)
print('pk2 stress=', pbox.get_stress_pk2() / units.GPa)
print('cauchy stress=', pbox.get_stress(voigt=False) / units.GPa)
print('deformation gradient=', pbox.get_defgrad())
write("output.lmpdata", patom, format='lammps-data', atom_style='atomic')
temp.translate([x * a, y * a, z * a])
for i in range(4):
print((x, y, z, i))
initial.append(temp[i])
tempPos = initial[0].position
del initial[0]
final = initial.copy()
final[1].position = tempPos
#QuasiNewton(initial).run(fmax=0.05)
#QuasiNewton(final).run(fmax=0.05)
images = [initial]
images += [initial.copy() for i in range(3)]
images += [final]
neb = NEB(images)
neb.interpolate()
for image in images[1:4]:
image.set_calculator(calc)
print("its go time")
optimizer = MDMin(neb, trajectory='neb.traj')
optimizer.run(fmax=0.04)
time = datetime.now().time()
print(time)