def __init__(self,
calculator=None,
nbr_of_evals=5,
terms=["pair", "T1", "T2", "T3", "T4", "T5", "T6", "T7"],
r_cut=None,
mu=None,
mu_c=None,
dim=3,
c_stab=0.1,
force_stab=False,
reinitialize=False,
array_convention='C',
solver="auto",
solve_tol=1e-9,
apply_positions=True,
apply_cell=True,
logfile=None):
"""Initialise an Hessian_EAM preconditioner with given parameters.
Args:
calculator: matscipy eam calculator
The calculator that calculates the hessian of the system.
nbr_of_evals: int
The number of evaluation after the matrix is calculated.
terms: list of strings
The list which terms of the analytic eam hessian should be
calculated.
r_cut, mu, c_stab, dim, recalc_mu, array_convention: see
precon.__init__()
"""
super().__init__(r_cut=r_cut,
mu=mu,
mu_c=mu_c,
dim=dim,
c_stab=c_stab,
force_stab=force_stab,
reinitialize=reinitialize,
array_convention=array_convention,
solver=solver,
solve_tol=solve_tol,
apply_positions=apply_positions,
apply_cell=apply_cell,
logfile=logfile)
self.calculator = calculator
self.terms = terms
self.nbr_of_evals = nbr_of_evals
self.ctr_of_evals = 0
self.exp_precon = Exp()
self.fmax = float('inf')
def test_precon_amin():
cu0 = bulk("Cu") * (2, 2, 2)
sigma = cu0.get_distance(0, 1) * (2.**(-1. / 6))
lj = LennardJones(sigma=sigma)
# perturb the cell
cell = cu0.get_cell()
cell *= 0.95
cell[1, 0] += 0.2
cell[2, 1] += 0.5
cu0.set_cell(cell, scale_atoms=True)
energies = []
for use_armijo in [True, False]:
for a_min in [None, 1e-3]:
atoms = cu0.copy()
atoms.calc = lj
opt = PreconLBFGS(atoms,
precon=Exp(A=3),
use_armijo=use_armijo,
a_min=a_min,
variable_cell=True)
opt.run(fmax=1e-3, smax=1e-4)
energies.append(atoms.get_potential_energy())
# check we get the expected energy for all methods
assert np.abs(np.array(energies) - -63.5032311942).max() < 1e-4
def main(argv):
fname = argv[0]
if (int(argv[1]) == 1):
variable_cell = True
else:
variable_cell = False
atoms = read(fname)
#atoms = bulk("Al")
calc = gp.GPAW(mode=gp.PW(500), kpts=(12, 12, 12), xc="PBE", nbands=-20)
atoms.set_calculator(calc)
prc = Exp(mu=1.0, mu_c=1.0)
outfname = fname.split("/")[-1]
outfname = outfname.split(".")[0]
logfile = outfname + ".log"
traj_file = outfname + ".traj"
relaxer = PreconLBFGS(atoms,
logfile=logfile,
precon=prc,
use_armijo=True,
variable_cell=variable_cell)
trajObj = Trajectory(traj_file, 'w', atoms)
relaxer.attach(trajObj)
if (variable_cell):
relaxer.run(fmax=0.025, smax=0.003)
else:
relaxer.run(fmax=0.025)
outfname = fname.split("/")[-1]
outfname = outfname.split(".")[0]
outfname += "_relaxed.xyz"
print("Energy: {}".format(atoms.get_potential_energy()))
write(outfname, atoms)
def test_single_precon_initialisation(setup_images):
images, _, _ = setup_images
precon = Exp()
mep = NEB(images, method='spline', precon=precon)
mep.get_forces()
assert len(mep.precon) == len(mep.images)
assert mep.precon[0].mu == mep.precon[1].mu
def relax(runID):
db = connect(db_name)
atoms = db.get_atoms(id=runID)
con = sq.connect(db_name)
cur = con.cursor()
cur.execute("SELECT value FROM text_key_values WHERE id=? AND key='name'",
(runID, ))
name = cur.fetchone()[0]
con.close()
calc = gp.GPAW(mode=gp.PW(600),
xc="PBE",
kpts=(4, 4, 4),
nbands="120%",
symmetry="off")
atoms.set_calculator(calc)
precon = Exp(mu=1.0, mu_c=1.0)
save_to_db = SaveToDB(db_name, runID, name)
logfile = "logfile%d.log" % (runID)
traj = "trajectory%d.traj" % (runID)
uf = UnitCellFilter(atoms, hydrostatic_strain=True)
relaxer = PreconLBFGS(uf, logfile=logfile, use_armijo=True, precon=precon)
relaxer.attach(save_to_db, interval=1, atoms=atoms)
trajObj = Trajectory(traj, "w", atoms)
relaxer.attach(trajObj)
relaxer.run(fmax=0.05, smax=0.003)
def test_precon():
cu0 = bulk("Cu") * (2, 2, 2)
lj = LennardJones(sigma=cu0.get_distance(0,1))
cu = cu0.copy()
cu.set_cell(1.2*cu.get_cell())
cu.calc = lj
ucf = UnitCellFilter(cu, constant_volume=True)
opt = PreconLBFGS(ucf, precon=Exp(mu=1.0, mu_c=1.0))
opt.run(fmax=1e-3)
assert abs(np.linalg.det(cu.cell)/np.linalg.det(cu0.cell) - 1.2**3) < 1e-3
# EcpCellFilter allows relaxing to lower tolerance
cu = cu0.copy()
cu.set_cell(1.2*cu.get_cell())
cu.calc = lj
ecf = ExpCellFilter(cu, constant_volume=True)
opt = PreconLBFGS(ecf, precon=Exp(mu=1.0, mu_c=1.0))
opt.run(fmax=1e-3)
assert abs(np.linalg.det(cu.cell)/np.linalg.det(cu0.cell) - 1.2**3) < 1e-7
def test_linesearch_maxstep():
import numpy as np
from ase import Atoms
from ase.calculators.emt import EMT
from ase.optimize import BFGS, BFGSLineSearch
from ase.optimize.precon import Exp, PreconLBFGS
positions = [
[5.8324672234339969, 8.5510800490537271, 5.686535793302002],
[7.3587688835494625, 5.646353802990923, 6.8378173997818958],
[7.9908510609316235, 5.4456005797117335, 4.5249260246251213],
[9.7103024117445145, 6.4768915365291466, 4.6502022197421278],
[9.5232482249292509, 8.7417754382952051, 4.6747936030744448],
[8.2738330473112036, 7.640248516254645, 6.1624124370797215],
[7.4198265919217921, 9.2882534361810016, 4.3654132356242874],
[6.8506783463494623, 9.2004422130272605, 8.611538688631887],
[5.9081131977596133, 5.6951755645279949, 5.4134092632199602],
[9.356736354387575, 9.2718534012646359, 8.491942486888524],
[9.0390271264592403, 9.5752757925665453, 6.4771649275571779],
[7.0554382804264533, 7.0016335250680779, 8.418151938177477],
[9.4855926945401272, 5.5650406772147694, 6.8445655410690591],
]
atoms = Atoms('Pt13', positions=positions, cell=[15] * 3)
maxstep = 0.2
longest_steps = []
labels = [
'BFGS', 'BFGSLineSearch', 'PreconLBFGS_Armijo', 'PreconLBFGS_Wolff'
]
optimizers = [BFGS, BFGSLineSearch, PreconLBFGS, PreconLBFGS]
for i, Optimizer in enumerate(optimizers):
a = atoms.copy()
a.set_calculator(EMT())
kwargs = {'maxstep': maxstep, 'logfile': None}
if 'Precon' in labels[i]:
kwargs['precon'] = Exp(A=3)
kwargs['use_armijo'] = 'Armijo' in labels[i]
opt = Optimizer(a, **kwargs)
opt.run(steps=1)
dr = a.get_positions() - positions
steplengths = (dr**2).sum(1)**0.5
longest_step = np.max(steplengths)
print('%s: longest step = %.4f' % (labels[i], longest_step))
longest_steps.append(longest_step)
longest_steps = np.array(longest_steps)
assert (longest_steps < maxstep + 1e-8).all()
def test_preconlbfgs():
N = 1
a0 = bulk('Cu', cubic=True)
a0 *= (N, N, N)
# perturb the atoms
s = a0.get_scaled_positions()
s[:, 0] *= 0.995
a0.set_scaled_positions(s)
nsteps = []
energies = []
for OPT in [PreconLBFGS, PreconFIRE]:
for precon in [None, Exp(A=3, mu=1.0)]:
atoms = a0.copy()
atoms.calc = EMT()
opt = OPT(atoms, precon=precon, use_armijo=True)
opt.run(1e-4)
energies += [atoms.get_potential_energy()]
nsteps += [opt.get_number_of_steps()]
# check we get the expected energy for all methods
assert np.abs(np.array(energies) - -0.022726045433998365).max() < 1e-4
# test with fixed bondlength and fixed atom constraints
cu0 = bulk("Cu") * (2, 2, 2)
cu0.rattle(0.01)
a0 = cu0.get_distance(0, 1)
cons = [FixBondLength(0, 1), FixAtoms([2, 3])]
for precon in [None, Exp(mu=1.0)]:
cu = cu0.copy()
cu.calc = EMT()
cu.set_distance(0, 1, a0 * 1.2)
cu.set_constraint(cons)
opt = PreconLBFGS(cu, precon=precon, use_armijo=True)
opt.run(fmax=1e-3)
assert abs(cu.get_distance(0, 1) / a0 - 1.2) < 1e-3
assert np.all(abs(cu.positions[2] - cu0.positions[2]) < 1e-3)
assert np.all(abs(cu.positions[3] - cu0.positions[3]) < 1e-3)
def test_linesearch(optcls, name, atoms, positions):
maxstep = 0.2
kwargs = {'maxstep': maxstep, 'logfile': None}
if 'Precon' in name:
kwargs['precon'] = Exp(A=3)
kwargs['use_armijo'] = 'Armijo' in name
opt = optcls(atoms, **kwargs)
opt.run(steps=1)
dr = atoms.get_positions() - positions
steplengths = (dr**2).sum(1)**0.5
longest_step = np.max(steplengths)
assert longest_step < maxstep + 1e-8
def optimise_positions(self, fmax=0.01, use_precon=None, use_armijo=None):
""" Relax atoms positions with the fixed cell to a given force
threshold """
if use_precon is None:
use_precon = self.parameters.use_precon
if use_armijo is None:
use_armijo = self.parameters.use_armijo
if use_precon:
precon = Exp(A=3, use_pyamg=False)
else:
precon = None
if self.parameters.optimizer == 'BFGS':
relax = BFGS(self.atoms)
elif self.parameters.optimizer == 'FIRE':
relax = PreconFIRE(self.atoms, precon=precon)
elif self.parameters.optimizer == 'ase-FIRE':
relax = ASEFIRE(self.atoms)
elif self.parameters.optimizer == 'LBFGS':
relax = PreconLBFGS(self.atoms,
precon=precon,
use_armijo=use_armijo)
elif self.parameters.optimizer == 'ase-LBFGS':
relax = ASELBFGS(self.atoms)
else:
parprint("ERROR: unknown optimizer {}. "
"Reverting to BFGS".format(self.parameters.optimizer))
relax = BFGS(self.atoms)
name = self.atoms.get_chemical_formula()
relax.attach(
lambda: self.atoms.calc.write(name + '_relax.gpw', mode='all'))
relax.attach(lambda: write_atat_input(self.atoms, 'str_last.out'))
relax.run(fmax=fmax, steps=100)
if not relax.converged():
relax = ASELBFGS(self.atoms)
relax.run(fmax=fmax, steps=100)
if not relax.converged():
max_force = self.atoms.get_forces()
max_force = np.sqrt((max_force**2).sum(axis=1).max())
print('WARNING: optimisation not converged.' +
' Maximum force: %.4f' % max_force)
def run_dftb_precon(folder, param_file):
""" Run DFTB+ using a preconditioned optimizer
Unlike a regular DFTB+ run a result.tag file is not produced because ASE
deletes the file. Instead we dump the energy and forces to a json file so
we cna load it back in later.
Args:
folder (str): directory containing a structure to optimize
param_file (str): path to the parameter file for this structure.
"""
if param_file is None:
raise RuntimeError("A parameter file must be supplied to run \
batch_dftb+ in precon mode")
hsd_file = os.path.join(folder, 'dftb_pin.hsd')
file_name = 'dftb_pin.hsd' if os.path.isfile(hsd_file) else 'geo_end.gen'
atoms = io.read(os.path.join(folder, file_name))
params = load_input_file(param_file)
calc = make_dftb_calc(atoms, folder, params)
atoms.set_calculator(calc)
try:
opt = PreconLBFGS(atoms,
precon=Exp(A=3),
use_armijo=True,
logfile=None)
opt.run(steps=int(params['geom_steps']))
except:
return
results = {
'energy': calc.get_potential_energy(),
'forces': calc.get_forces().tolist()
}
json.dump(results, open(os.path.join(folder, "results.json"), 'w'))
def do_short_relax(atoms, index=None, vc_relax=False, precon=True,
maxsteps=20):
''' Performs a (usually short) local optimization.
atoms: an Atoms object
index: index to be used as suffix for the output files
vc_relax: whether to also optimize the cell vectors
(after having run several steps with fixed cell)
precon: whether to use the preconditioned optimizers
maxsteps: maximum number of ionic steps
'''
if vc_relax:
assert precon
t = time()
label = 'opt' if index is None else 'opt_' + str(index)
logfile = '%s.log' % label
trajfile = '%s.traj' % label
traj = Trajectory(trajfile, 'a', atoms)
nsteps = 0
maxsteps_no_vc = maxsteps / 2 if vc_relax else maxsteps
fmax = 2. if vc_relax else 0.1
try:
if precon:
dyn = PreconLBFGS_My(atoms, precon=Exp(A=3), variable_cell=False,
use_armijo=True, a_min=1e-2, logfile=logfile)
else:
dyn = BFGS(atoms, maxstep=0.4, logfile=logfile)
dyn.attach(traj)
dyn.run(fmax=fmax, steps=maxsteps_no_vc)
except RuntimeError:
nsteps += dyn.get_number_of_steps()
if precon:
dyn = PreconFIRE_My(atoms, precon=Exp(A=3), variable_cell=False,
use_armijo=False, logfile=logfile,
dt=0.1, maxmove=0.5, dtmax=1.0, finc=1.1)
else:
dyn = FIRE(atoms, logfile=logfile, dt=0.1, maxmove=0.5, dtmax=1.0,
finc=1.1)
dyn.attach(traj)
steps = maxsteps_no_vc - nsteps
dyn.run(fmax=fmax, steps=steps)
nsteps += dyn.get_number_of_steps()
if vc_relax:
L = atoms.get_volume() / 4. # largest cell vector length allowed
cellbounds = CellBounds(bounds={'phi':[20., 160.], 'a':[1.5, L],
'chi':[20., 160.], 'b':[1.5, L],
'psi':[20., 160.], 'c':[1.5, L]})
try:
dyn = PreconLBFGS_My(atoms, precon=Exp(A=3), variable_cell=True,
use_armijo=True, logfile=logfile,
cellbounds=cellbounds, a_min=1e-2)
dyn.e1 = None
try:
dyn._just_reset_hessian
except AttributeError:
dyn._just_reset_hessian = True
dyn.attach(traj)
steps = maxsteps - nsteps
dyn.run(fmax=0., smax=0., steps=steps)
except RuntimeError:
nsteps += dyn.get_number_of_steps()
dyn = PreconFIRE_My(atoms, precon=Exp(A=3), variable_cell=True,
use_armijo=False, logfile=logfile,
cellbounds=cellbounds,
dt=0.1, maxmove=0.5, dtmax=1.0, finc=1.1)
dyn.attach(traj)
steps = maxsteps - nsteps
dyn.run(fmax=0., steps=steps)
name = atoms.calc.name
print('%s relaxation took %.3f seconds' % (name, time()-t))
return atoms
import numpy as np
from ase.build import bulk
from ase.calculators.lj import LennardJones
from ase.optimize.precon import PreconLBFGS, Exp
from ase.constraints import UnitCellFilter
cu0 = bulk("Cu") * (2, 2, 2)
lj = LennardJones(sigma=cu0.get_distance(0, 1))
cu = cu0.copy()
cu.set_cell(1.2 * cu.get_cell())
cu.set_calculator(lj)
ucf = UnitCellFilter(cu, constant_volume=True)
opt = PreconLBFGS(ucf, precon=Exp(mu=1.0, mu_c=1.0))
opt.run(fmax=1e-3)
assert abs(np.linalg.det(cu.cell) / np.linalg.det(cu0.cell) - 1.2**3) < 1e-3
calc = GPAW(mode=PW(e_cut),
nbands=nbands,
xc='PBE',
spinpol=True,
kpts=(k_pts, k_pts, k_pts),
occupations=FermiDirac(smear),
txt=system_name + '.out')
bulk_mat.set_calculator(calc)
#Save the initial state of the calculations
#calc.write('Fe_relaxer_initial.gpw')
save_atoms(bulk_mat, e_cut, nbands, k_pts, smear, a, initial_magmom, 1,
str(sys.argv[6]))
precon = Exp()
saver = Gpw_save(calc, system_name + '_relaxed.gpw')
traj = Trajectory(system_name + '_relaxed.traj', 'w', bulk_mat)
relaxer = PreconFire(bulk_mat,
precon=precon,
variable_cell=True,
logfile=system_name + '.txt')
relaxer.attach(traj)
relaxer.attach(saver)
relaxer.run(fmax=0.025, smax=0.003)
bulk_mat.get_potential_energy()
#Save the final state of the calculations
calc.write(system_name + '_relaxer_final.gpw')
save_atoms(bulk_mat, e_cut, nbands, k_pts, smear, a, initial_magmom, 0,
str(sys.argv[6]))
def __init__(self,
atoms,
restart=None,
logfile='-',
trajectory=None,
maxstep=None,
memory=100,
damping=1.0,
alpha=70.0,
master=None,
precon='auto',
variable_cell=False,
use_armijo=True,
c1=0.23,
c2=0.46,
a_min=None,
rigid_units=None,
rotation_factors=None,
Hinv=None):
"""Parameters:
atoms: Atoms object
The Atoms object to relax.
restart: string
Pickle file used to store vectors for updating the inverse of
Hessian matrix. If set, file with such a name will be searched
and information stored will be used, if the file exists.
logfile: file object or str
If *logfile* is a string, a file with that name will be opened.
Use '-' for stdout.
trajectory: string
Pickle file used to store trajectory of atomic movement.
maxstep: float
How far is a single atom allowed to move. This is useful for DFT
calculations where wavefunctions can be reused if steps are small.
Default is 0.04 Angstrom.
memory: int
Number of steps to be stored. Default value is 100. Three numpy
arrays of this length containing floats are stored.
damping: float
The calculated step is multiplied with this number before added to
the positions.
alpha: float
Initial guess for the Hessian (curvature of energy surface). A
conservative value of 70.0 is the default, but number of needed
steps to converge might be less if a lower value is used. However,
a lower value also means risk of instability.
master: boolean
Defaults to None, which causes only rank 0 to save files. If
set to true, this rank will save files.
precon: ase.optimize.precon.Precon instance or compatible.
Apply the given preconditioner during optimization. Defaults to
'auto', which will choose the `Exp` preconditioner unless the system
is too small (< 100 atoms) in which case a standard LBFGS fallback
is used. To enforce use of the `Exp` preconditioner, use `precon =
'Exp'`. Other options include 'C1', 'Pfrommer' and 'FF' - see the
corresponding classes in the `ase.optimize.precon` module for more
details. Pass precon=None or precon='ID' to disable preconditioning.
use_armijo: boolean
Enforce only the Armijo condition of sufficient decrease of
of the energy, and not the second Wolff condition for the forces.
Often significantly faster than full Wolff linesearch.
Defaults to True.
c1: float
c1 parameter for the line search. Default is c1=0.23.
c2: float
c2 parameter for the line search. Default is c2=0.46.
a_min: float
minimal value for the line search step parameter. Default is
a_min=1e-8 (use_armijo=False) or 1e-10 (use_armijo=True).
Higher values can be useful to avoid performing many
line searches for comparatively small changes in geometry.
variable_cell: bool
If True, wrap atoms an ase.constraints.UnitCellFilter to
relax both postions and cell. Default is False.
rigid_units: each I = rigid_units[i] is a list of indices, which
describes a subsystem of atoms that forms a (near-)rigid unit
If rigid_units is not None, then special search-paths are
are created to take the rigidness into account
rotation_factors: list of scalars; acceleration factors deteriming
the rate of rotation as opposed to the rate of stretch in the
rigid units
"""
if variable_cell:
atoms = UnitCellFilter(atoms)
Optimizer.__init__(self, atoms, restart, logfile, trajectory, master)
# default preconditioner
# TODO: introduce a heuristic for different choices of preconditioners
if precon == 'auto':
if len(atoms) < 100:
precon = None
warnings.warn(
'The system is likely too small to benefit from ' +
'the standard preconditioner, hence it is ' +
'disabled. To re-enable preconditioning, call' +
'`PreconLBFGS` by explicitly providing the ' +
'kwarg `precon`')
else:
precon = 'Exp'
if maxstep is not None:
if maxstep > 1.0:
raise ValueError('You are using a much too large value for ' +
'the maximum step size: %.1f Angstrom' %
maxstep)
self.maxstep = maxstep
else:
self.maxstep = 0.04
self.memory = memory
self.H0 = 1. / alpha # Initial approximation of inverse Hessian
# 1./70. is to emulate the behaviour of BFGS
# Note that this is never changed!
self.Hinv = Hinv
self.damping = damping
self.p = None
# construct preconditioner if passed as a string
if isinstance(precon, basestring):
if precon == 'C1':
precon = C1()
if precon == 'Exp':
precon = Exp()
elif precon == 'Pfrommer':
precon = Pfrommer()
elif precon == 'ID':
precon = None
else:
raise ValueError('Unknown preconditioner "{0}"'.format(precon))
self.precon = precon
self.use_armijo = use_armijo
self.c1 = c1
self.c2 = c2
self.a_min = a_min
if self.a_min is None:
self.a_min = 1e-10 if use_armijo else 1e-8
# CO
self.rigid_units = rigid_units
self.rotation_factors = rotation_factors
def relax_precon(atoms,
calc,
fmax=5e-2,
smax=1e-4,
variable_cell=False,
trajfile=None,
logfile=None,
maxsteps=10000,
verbose=True,
dEmin=1e-3,
a_min=1e-8,
optimizer='LBFGS',
cellbounds=None,
fix_bond_lengths_pairs=None,
debug=False):
""" Locally optimizes the geometry using the preconditioned optimizers.
atoms: the Atoms object
calc: a calculator instance to attach to the Atoms object
fmax: the force convergence criterion (in eV/Angstrom)
smax: the stress convergence criterion (in eV/Angstrom^3)
variable_cell: whether to also optimize the cell vectors
trajfile: filename of the trajectory to attach to the optimizers
logfile: filename of the logfile for the optimizers
maxsteps: maximum allowed total number of ionic steps
verbose: whether to print output or remain silent
dEmin: minimum (absolute) energy difference for the main loop
iterations; if the energy difference is smaller, the
minimization is aborted
a_min: minimal value for the linesearch parameter in the
PreconLBFGS optimizer
optimizer: 'LBFGS' or 'FIRE', the preferred type of
(preconditioned) optimizer
cellbounds: ase.ga.bulk_utilities.CellBounds instance for
setting bounds on the cell shape and size
during variable-cell relaxation
fix_bond_lengths_pairs: list of (i,j) tuples of atom pairs
for which the (minimum image) bond distance
will be kept fixed
debug: if True, extra output may be printed to stdout
"""
assert optimizer in ['LBFGS', 'FIRE']
class UnitCellFilterFixBondLengthsWrapper(UnitCellFilterFixBondLengths):
""" Wrapper to nitCellFilterFixBondLengths,
required because of ase.optimize.precon.estimate_mu.
"""
def __init__(self, atoms):
UnitCellFilterFixBondLengths.__init__(self,
atoms,
maxiter=1000,
pairs=fix_bond_lengths_pairs)
if variable_cell:
atoms.set_pbc(True)
else:
smax = None
cellbounds = None
atoms.wrap()
atoms.set_calculator(calc)
nsteps = 0
if trajfile is not None:
if os.path.exists(trajfile):
os.remove(trajfile)
traj = Trajectory(trajfile, 'a', atoms)
else:
traj = None
if fix_bond_lengths_pairs is not None:
original_constraints = [c for c in atoms.constraints]
bond_lengths = np.zeros(len(fix_bond_lengths_pairs))
for i, ab in enumerate(fix_bond_lengths_pairs):
bond_lengths[i] = atoms.get_distance(ab[0], ab[1], mic=True)
fbl_constraint = FixBondLengths(fix_bond_lengths_pairs)
atoms.set_constraint(original_constraints + [fbl_constraint])
if variable_cell:
# Start with partial relaxation using fixed cell vectors
if fix_bond_lengths_pairs or optimizer == 'FIRE':
# PreconFIRE is more suitable in this case
dyn = PreconFIRE_My(atoms,
precon=Exp(A=3),
use_armijo=True,
variable_cell=False,
logfile=logfile)
else:
dyn = PreconLBFGS_My(atoms,
precon=Exp(A=3),
use_armijo=True,
variable_cell=False,
logfile=logfile,
maxstep=0.2,
a_min=a_min)
attach1 = VarianceError(atoms, dyn, N=5)
dyn.attach(attach1)
attach2 = DivergenceError(atoms, dyn, N=2, max_slope=0.05)
dyn.attach(attach2)
if traj is not None:
dyn.attach(traj)
try:
dyn.run(fmax=1., steps=25)
except RuntimeError as err:
if debug:
print(err.message, flush=True)
nsteps += dyn.get_number_of_steps()
if variable_cell and fix_bond_lengths_pairs is not None:
# Fixing bond lengths will be taken care of
# by the modified UnitCellFilter
atoms.set_constraint(original_constraints)
atoms = UnitCellFilterFixBondLengthsWrapper(atoms)
elif variable_cell:
atoms = UnitCellFilter(atoms)
steps = 30
niter = 0
maxiter = 50
nerr = 0
maxerr = 10
e_prev = 1e64
while nsteps < maxsteps and niter < maxiter and nerr < maxerr:
e = atoms.get_potential_energy()
if abs(e - e_prev) < dEmin:
break
e_prev = e
try:
if optimizer == 'LBFGS':
dyn = PreconLBFGS_My(atoms,
precon=Exp(A=3),
use_armijo=True,
logfile=logfile,
a_min=a_min,
variable_cell=False,
maxstep=0.2,
cellbounds=cellbounds)
elif optimizer == 'FIRE':
dyn = PreconFIRE_My(atoms,
precon=Exp(A=3),
use_armijo=True,
variable_cell=False,
logfile=logfile,
maxmove=0.5,
cellbounds=cellbounds)
dyn.e1 = None
try:
dyn._just_reset_hessian
except AttributeError:
dyn._just_reset_hessian = True
if traj is not None:
dyn.attach(traj)
attach1 = VarianceError(atoms, dyn, N=5)
dyn.attach(attach1)
attach2 = DivergenceError(atoms, dyn, N=2, max_slope=0.05)
dyn.attach(attach2)
dyn.run(fmax=fmax, smax=smax, steps=steps)
nsteps += dyn.get_number_of_steps()
except RuntimeError as err:
if debug:
print(err.message, flush=True)
nerr += 1
nsteps += dyn.get_number_of_steps()
dyn = PreconFIRE_My(atoms,
precon=Exp(A=3),
use_armijo=False,
variable_cell=False,
logfile=logfile,
maxmove=0.5,
cellbounds=cellbounds)
if traj is not None:
dyn.attach(traj)
attach1 = VarianceError(atoms, dyn, N=5)
dyn.attach(attach1)
attach2 = DivergenceError(atoms, dyn, N=2, max_slope=0.05)
dyn.attach(attach2)
try:
dyn.run(fmax=fmax, smax=smax, steps=steps)
except RuntimeError as err:
if debug:
print(err.message, flush=True)
nerr += 1
nsteps += dyn.get_number_of_steps()
niter += 1
try:
if dyn.converged():
break
except RuntimeError:
break
if isinstance(atoms, UnitCellFilterFixBondLengthsWrapper):
atoms = atoms.atoms
atoms.wrap()
pos = atoms.get_positions()
cell = atoms.get_cell()
pbc = atoms.get_pbc()
for (i1, i2), bl in zip(fix_bond_lengths_pairs, bond_lengths):
vec = pos[i2] - pos[i1]
vec = find_mic([vec], cell, pbc)[0][0]
pos[i2] = pos[i1] + vec * bl / np.linalg.norm(vec)
atoms.set_positions(pos)
atoms = UnitCellFilterFixBondLengthsWrapper(atoms)
calculate_regular = False
if fix_bond_lengths_pairs is not None:
# Guarantee that the fixed bonds have the specified length
pos = atoms.get_positions()
if isinstance(atoms, Filter):
cell = atoms.atoms.get_cell()
pbc = atoms.atoms.get_pbc()
else:
cell = atoms.get_cell()
pbc = atoms.get_pbc()
for (i1, i2), bl in zip(fix_bond_lengths_pairs, bond_lengths):
vec = pos[i2] - pos[i1]
vec = find_mic([vec], cell, pbc)[0][0]
pos[i2] = pos[i1] + vec * bl / np.linalg.norm(vec)
if isinstance(atoms, Filter):
atoms = atoms.atoms
atoms.set_positions(pos[:len(atoms)])
atoms = UnitCellFilterFixBondLengthsWrapper(atoms)
try:
E = atoms.get_potential_energy()
F = atoms.get_forces()[:len(atoms.atoms)]
S = atoms.stress
except RuntimeError:
calculate_regular = True
else:
atoms.set_constraint(original_constraints)
atoms.set_positions(pos)
atoms.set_constraint(original_constraints + [fbl_constraint])
calculate_regular = True
if isinstance(atoms, Filter):
atoms = atoms.atoms
if fix_bond_lengths_pairs is None or calculate_regular:
E = atoms.get_potential_energy()
F = atoms.get_forces()
S = atoms.get_stress() if variable_cell else None
atoms.wrap()
if verbose:
print('Done E=%8.3f, maxF=%5.3f, maxS=%5.3e, nsteps=%d' % \
(E, (F**2).sum(axis=1).max()**0.5,
0. if S is None else np.max(np.abs(S)), nsteps), flush=True)
finalize(atoms, energy=E, forces=F, stress=S)
return atoms
atoms.set_cell(atoms.cell * np.diag([1.0 + s, 1.0 - s * nu, 1.0 - s * nu]),
scale_atoms=True)
# simple header for the output
print(" Iteration Time Energy max Force")
# loop to perform the successive small strain increments
for i in range(50):
# record and print the current strain
atoms.info["strain"] = (atoms.cell[0, 0] -
origLx) / origLx # Engineering strain
print "strain: ", atoms.info["strain"]
# set up an optimizer, this is a particularly efficient one
opt = PreconLBFGS(atoms, precon=Exp(3.0))
# attach the optimiser to the atoms object, asking it to call our helper function
# that writes out the atomic positions, after every 2nd iterations of the optimisation
opt.attach(write_frame, 2, atoms)
# run the optimizer, until the maximum force on any atom is less than a tolerance in eV/Ang
opt.run(fmax=0.02)
# update the "grip" by applying the small strain increment.
s = 0.01 # small strain increment
atoms.set_cell(atoms.cell * np.diag([1.0 + s, 1.0 - s * nu, 1.0 - s * nu]),
scale_atoms=True)
#######################################################################
#
]
atoms = Atoms('Pt13', positions=positions, cell=[15] * 3)
maxstep = 0.2
longest_steps = []
labels = ['BFGS', 'BFGSLineSearch', 'PreconLBFGS_Armijo', 'PreconLBFGS_Wolff']
optimizers = [BFGS, BFGSLineSearch, PreconLBFGS, PreconLBFGS]
for i, Optimizer in enumerate(optimizers):
a = atoms.copy()
a.set_calculator(EMT())
kwargs = {'maxstep': maxstep, 'logfile': None}
if 'Precon' in labels[i]:
kwargs['precon'] = Exp(A=3)
kwargs['use_armijo'] = 'Armijo' in labels[i]
opt = Optimizer(a, **kwargs)
opt.run(steps=1)
dr = a.get_positions() - positions
steplengths = (dr**2).sum(1)**0.5
longest_step = np.max(steplengths)
print('%s: longest step = %.4f' % (labels[i], longest_step))
longest_steps.append(longest_step)
longest_steps = np.array(longest_steps)
assert (longest_steps < maxstep + 1e-8).all()
atoms.set_cell(atoms.cell * np.diag([1.0 + s, 1.0 - s * nu, 1.0 - s * nu]),
scale_atoms=True)
# simple header for the output
print(" Iteration Time Energy max Force")
# loop to perform the successive small strain increments
for i in range(10):
# record and print the current strain
atoms.info["strain"] = (atoms.cell[0, 0] -
origLx) / origLx # Engineering strain
print("strain: ", atoms.info["strain"])
# set up an optimizer, this is a particularly efficient one
opt = PreconLBFGS(atoms, precon=Exp(3.0, use_pyamg=False))
# attach the optimiser to the atoms object, asking it to call our helper function
# that writes out the atomic positions, after every iteration of the optimisation
opt.attach(write_frame, 1, atoms)
# run the optimizer, until the maximum force on any atom is less than a tolerance in eV/Ang
opt.run(fmax=0.02)
# update the "grip" by applying the small strain increment.
s = 0.01 # small strain increment
atoms.set_cell(atoms.cell * np.diag([1.0 + s, 1.0 - s * nu, 1.0 - s * nu]),
scale_atoms=True)
#######################################################################
#
class Hessian_EAM_EXP(SparsePrecon):
""" Creates matrix with the hessian matrix of the matscipy EAM calculator.
"""
def __init__(self,
calculator=None,
nbr_of_evals=5,
terms=["pair", "T1", "T2", "T3", "T4", "T5", "T6", "T7"],
r_cut=None,
mu=None,
mu_c=None,
dim=3,
c_stab=0.1,
force_stab=False,
reinitialize=False,
array_convention='C',
solver="auto",
solve_tol=1e-9,
apply_positions=True,
apply_cell=True,
logfile=None):
"""Initialise an Hessian_EAM preconditioner with given parameters.
Args:
calculator: matscipy eam calculator
The calculator that calculates the hessian of the system.
nbr_of_evals: int
The number of evaluation after the matrix is calculated.
terms: list of strings
The list which terms of the analytic eam hessian should be
calculated.
r_cut, mu, c_stab, dim, recalc_mu, array_convention: see
precon.__init__()
"""
super().__init__(r_cut=r_cut,
mu=mu,
mu_c=mu_c,
dim=dim,
c_stab=c_stab,
force_stab=force_stab,
reinitialize=reinitialize,
array_convention=array_convention,
solver=solver,
solve_tol=solve_tol,
apply_positions=apply_positions,
apply_cell=apply_cell,
logfile=logfile)
self.calculator = calculator
self.terms = terms
self.nbr_of_evals = nbr_of_evals
self.ctr_of_evals = 0
self.exp_precon = Exp()
self.fmax = float('inf')
def make_precon(self, atoms, reinitialize=None):
start_time = time.time()
forces = atoms.get_forces()
last_fmax = self.fmax
self.fmax = sqrt((forces**2).sum(axis=1).max())
# Create the preconditioner:
if (self.P is None or self.ctr_of_evals >= self.nbr_of_evals
or (self.fmax <= 0.1 and last_fmax > 0.1)):
self._make_sparse_precon(atoms, force_stab=self.force_stab)
self.ctr_of_evals = 0
if self.fmax <= 0.1:
self.ctr_of_evals += 1
self.logfile.write('--- Precon created in %s seconds ---\n' %
(time.time() - start_time))
def _make_sparse_precon(self,
atoms,
initial_assembly=False,
force_stab=False):
"""Create a sparse preconditioner matrix based on the passed atoms.
Args:
atoms: the Atoms object used to create the preconditioner.
Returns:
A scipy.sparse.csr_matrix object, representing a d*N by d*N matrix
(where N is the number of atoms, and d is the value of self.dim).
BE AWARE that using numpy.dot() with this object will result in
errors/incorrect results - use the .dot method directly on the
sparse matrix instead.
"""
self.logfile.write('creating eam hessian: terms={}'.format(self.terms))
start_time = time.time()
if self.fmax > 0.1:
self.exp_precon.make_precon(atoms)
self.P = self.exp_precon.P
print("Fmax > 1")
else:
self.P = self.calculator.calculate_hessian_matrix(atoms,
terms=self.terms)
val, vec = eigsh(self.P, k=1, which="SA")
a_s = 0.00001
a = a_s
for k in range(100):
self.P += a * sparse.eye(self.P.shape[0])
val, vec = eigsh(self.P, k=1, which="SA")
if (val > 0):
break
a = 1.5 * a
self.logfile.write('--- Hessian created in %s seconds ---\n' %
(time.time() - start_time))
self.create_solver()
from ase.optimize.precon import Exp, PreconLBFGS, PreconFIRE
from ase.constraints import FixBondLength, FixAtoms
N = 1
a0 = bulk('Cu', cubic=True)
a0 *= (N, N, N)
# perturb the atoms
s = a0.get_scaled_positions()
s[:, 0] *= 0.995
a0.set_scaled_positions(s)
nsteps = []
energies = []
for OPT in [PreconLBFGS, PreconFIRE]:
for precon in [None, Exp(A=3, mu=1.0)]:
atoms = a0.copy()
atoms.set_calculator(EMT())
opt = OPT(atoms, precon=precon, use_armijo=True)
opt.run(1e-4)
energies += [atoms.get_potential_energy()]
nsteps += [opt.get_number_of_steps()]
# check we get the expected energy for all methods
assert np.abs(np.array(energies) - -0.022726045433998365).max() < 1e-4
# test with fixed bondlength and fixed atom constraints
cu0 = bulk("Cu") * (2, 2, 2)
cu0.rattle(0.01)
a0 = cu0.get_distance(0, 1)
cons = [FixBondLength(0,1), FixAtoms([2,3])]
calc = GFN2(charge=args.charge,
accuracy=args.acc,
temperature=args.etemp,
max_iterations=args.maxiter,
print_level=2,
solvent=args.solvent)
else:
raise Exception("Method not implemented.")
mol.set_calculator(calc)
e = mol.get_potential_energy()
print('Initial energy: eV, Eh', e, e / Hartree)
if args.precon:
precon = Exp(A=3, r_NN=args.rnn + 0.1, r_cut=args.rnn + 0.6)
else:
precon = None
if args.optcell:
sf = ExpCellFilter(mol)
relax = PatchedOptimizer(sf,
precon=precon,
trajectory=args.trajectory,
logfile=args.logfile,
use_armijo=args.armijo)
else:
relax = PatchedOptimizer(mol,
precon=precon,
trajectory=args.trajectory,
logfile=args.logfile,
dimer.positions[3:, 0] += 2.8
dimer.constraints = FixBondLengths([
((selection[i] + 3) % 6, (selection[i - 1] + 3) % 6) for i in range(3)
])
dimer.calc = EIQMMM(selection,
GPAW(txt=name + '.txt', h=0.16),
TIP4P(),
interaction,
vacuum=4,
embedding=Embedding(rc=0.2, rc2=20, width=1),
output=name + '.out')
opt = LBFGS(dimer, trajectory=name + '.traj')
opt.run(0.02)
monomer = dimer[selection]
monomer.center(vacuum=4)
monomer.calc = GPAW(txt=name + 'M.txt', h=0.16)
opt = PreconLBFGS(monomer, precon=Exp(A=3), trajectory=name + 'M.traj')
opt.run(0.02)
e0 = monomer.get_potential_energy()
be = dimer.get_potential_energy() - e0
d = dimer.get_distance(0, 3)
print(name, be, d)
if name == '012':
assert abs(be - -0.288) < 0.002
assert abs(d - 2.76) < 0.02
else:
assert abs(be - -0.316) < 0.002
assert abs(d - 2.67) < 0.02
# creates: precon.png
from ase.build import bulk
from ase.calculators.emt import EMT
from ase.optimize.precon import Exp, PreconLBFGS
from ase.calculators.loggingcalc import LoggingCalculator
import matplotlib.pyplot as plt
a0 = bulk('Cu', cubic=True)
a0 *= [3, 3, 3]
del a0[0]
a0.rattle(0.1)
nsteps = []
energies = []
log_calc = LoggingCalculator(EMT())
for precon, label in [(None, 'None'), (Exp(A=3, mu=1.0), 'Exp(A=3)')]:
log_calc.label = label
atoms = a0.copy()
atoms.set_calculator(log_calc)
opt = PreconLBFGS(atoms, precon=precon, use_armijo=True)
opt.run(fmax=1e-3)
log_calc.plot(markers=['r-', 'b-'], energy=False, lw=2)
plt.savefig('precon.png')
def estimate_mu(self, structure, fixed_frame, parameters):
"""Estimate scaling parameter mu for
Expoential preconditioner scheme.
For more implementation detail see Packwood et. al:
A universal preconditioner for simulating condensed phase materials,
J. Chem. Phys. 144, 164109 (2016).
https://aip.scitation.org/doi/full/10.1063/1.4947024
and
https://wiki.fysik.dtu.dk/ase/ase/optimize.html
First reads the parameters file and checks if the
estimation of mu is necessary. Then Estimates mu
with default parameters of r_cut=2*r_NN, where r_NN
is estimated nearest neighbour distance. Parameter
A=3.0 set to default value as was mentioned in the
paper.
Args:
structure {GenSec structure}: structure object
fixed_frame {GenSec fixed frame}: fixed frame object
parameters {JSON} : Parameters from file
Returns:
float: Scaling parameter mu
"""
# Figure out for which atoms Exp is applicapble
precons_parameters = {
"mol":
parameters["calculator"]["preconditioner"]["mol"]["precon"],
"fixed_frame":
parameters["calculator"]["preconditioner"]["fixed_frame"]
["precon"],
"mol-mol":
parameters["calculator"]["preconditioner"]["mol-mol"]["precon"],
"mol-fixed_frame":
parameters["calculator"]["preconditioner"]["mol-fixed_frame"]
["precon"],
}
precons_parameters_init = {
"mol":
parameters["calculator"]["preconditioner"]["mol"]["initial"],
"fixed_frame":
parameters["calculator"]["preconditioner"]["fixed_frame"]
["initial"],
"mol-mol":
parameters["calculator"]["preconditioner"]["mol-mol"]["initial"],
"mol-fixed_frame":
parameters["calculator"]["preconditioner"]["mol-fixed_frame"]
["initial"],
}
precons_parameters_update = {
"mol":
parameters["calculator"]["preconditioner"]["mol"]["update"],
"fixed_frame":
parameters["calculator"]["preconditioner"]["fixed_frame"]
["update"],
"mol-mol":
parameters["calculator"]["preconditioner"]["mol-mol"]["update"],
"mol-fixed_frame":
parameters["calculator"]["preconditioner"]["mol-fixed_frame"]
["update"],
}
need_for_exp = False
for i in range(len(list(precons_parameters.values()))):
if list(precons_parameters.values())[i] == "Exp":
if (list(precons_parameters_init.values())[i]
or list(precons_parameters_update.values())[i]):
need_for_exp = True
mu = 1.0
if need_for_exp:
if len(structure.molecules) > 1:
a0 = structure.molecules[0].copy()
for i in range(1, len(structure.molecules)):
a0 += structure.molecules[i]
else:
a0 = structure.molecules[0]
if hasattr(fixed_frame, "fixed_frame"):
all_atoms = a0 + fixed_frame.fixed_frame
else:
all_atoms = a0
atoms = all_atoms.copy()
atoms.set_calculator(self.calculator)
self.set_constrains(atoms, parameters)
r_NN = estimate_nearest_neighbour_distance(atoms)
try:
mu = Exp(r_cut=2.0 * r_NN, A=3.0).estimate_mu(atoms)[0]
except:
print("Something is wrong!")
return mu
# creates: precon.png
from ase.build import bulk
from ase.calculators.emt import EMT
from ase.optimize.precon import Exp, PreconLBFGS
from ase.calculators.loggingcalc import LoggingCalculator
import matplotlib.pyplot as plt
a0 = bulk('Cu', cubic=True)
a0 *= [3, 3, 3]
del a0[0]
a0.rattle(0.1)
nsteps = []
energies = []
log_calc = LoggingCalculator(EMT())
for precon, label in [(None, 'None'), (Exp(A=3, use_pyamg=False), 'Exp(A=3)')]:
log_calc.label = label
atoms = a0.copy()
atoms.set_calculator(log_calc)
opt = PreconLBFGS(atoms, precon=precon, use_armijo=True)
opt.run(fmax=1e-3)
log_calc.plot(markers=['r-', 'b-'], energy=False, lw=2)
plt.savefig('precon.png')
import numpy as np
from ase.build import bulk
from ase.calculators.emt import EMT
from ase.optimize.precon import Exp, PreconLBFGS, PreconFIRE
N = 1
a0 = bulk('Cu', cubic=True)
a0 *= (N, N, N)
# perturb the atoms
s = a0.get_scaled_positions()
s[:, 0] *= 0.995
a0.set_scaled_positions(s)
nsteps = []
energies = []
for OPT in [PreconLBFGS, PreconFIRE]:
for precon in [None, Exp(A=3, use_pyamg=False)]:
atoms = a0.copy()
atoms.set_calculator(EMT())
opt = OPT(atoms, precon=precon, use_armijo=True)
opt.run(1e-4)
energies += [atoms.get_potential_energy()]
nsteps += [opt.get_number_of_steps()]
# check we get the expected energy for all methods
assert np.abs(np.array(energies) - -0.022726045433998365).max() < 1e-4
def calc(primitive,
cachedir=None,
supercell=(1, 1, 1),
delta=0.01,
quick=True):
"""Calculates the Hessian for a given atoms object (which *must* have an
attached calculator).
.. note:: We choose to use the Hessian as the fundamental quantity in
vibrational analysis in `matdb`.
.. note:: `atoms` will be relaxed before calculating the Hessian.
Args:
primitive (matdb.atoms.Atoms): atomic structure of the *primitive*.
cachedir (str): path to the directory where phonon calculations are
cached. If not specified, a temporary directory will be used.
supercell (tuple): number of times to duplicate the cell when
forming the supercell.
delta (float): displacement in Angstroms of each atom when computing the
phonons.
quick (bool): when True, use symmetry to speed up the Hessian
calculation. See :func:`_calc_quick`.
Returns:
numpy.ndarray: Hessian matrix that has dimension `(natoms*3, natoms*3)`,
where `natoms` is the number of atoms in the *supercell*.
"""
if quick:
return _calc_quick(primitive, supercell, delta)
else:
atoms = primitive.make_supercell(supercell)
atoms.set_calculator(primitive.get_calculator())
from ase.vibrations import Vibrations
#The phonon calculator caches the displacements and force sets for each
#atomic displacement using pickle. This generates three files for each
#atomic degree of freedom (one for each cartesian direction). We want to
#save these in a special directory.
tempcache = False
if cachedir is None:
cachedir = mkdtemp()
tempcache = True
else:
cachedir = path.abspath(path.expanduser(cachedir))
if not path.isdir(cachedir):
mkdir(cachedir)
result = None
precon = Exp(A=3)
aphash = None
#Calculate a hash of the calculator and atoms object that we are calculating
#for. If the potential doesn't have a `to_dict` method, then we ignore the
#hashing.
if not tempcache and hasattr(atoms, "to_dict") and hasattr(
atoms._calc, "to_dict"):
atoms_pot = {"atoms": atoms.to_dict(), "pot": atoms._calc.to_dict()}
#This UUID will probably be different, even if the positions and species
#are identical.
del atoms_pot["atoms"]["uuid"]
hash_str = convert_dict_to_str(atoms_pot)
aphash = str(sha1(hash_str).hexdigest())
if not tempcache:
#Check whether we should clobber the cache or not.
extras = ["vibsummary.log", "vib.log", "phonons.log"]
with chdir(cachedir):
hash_match = False
if path.isfile("atomspot.hash"):
with open("atomspot.hash") as f:
xhash = f.read()
hash_match = xhash == aphash
hascache = False
if not hash_match:
for vibfile in glob("vib.*.pckl"):
remove(vibfile)
hascache = True
for xfile in extras:
if path.isfile(xfile):
remove(xfile)
hascache = True
if hascache:
msg.warn(
"Using hard-coded cache directory. We were unable to "
"verify that the atoms-potential combination matches "
"the one for which existing cache files exist. So, we "
"clobbered the existing files to get the science "
"right. You can fix this by using `matdb.atoms.Atoms` "
"and `matdb.calculators.*Calculator` objects.")
with chdir(cachedir):
#Relax the cell before we calculate the Hessian; this gets the forces
#close to zero before we make harmonic approximation.
try:
with open("phonons.log") as f:
with redirect_stdout(f):
minim = PreconLBFGS(atoms, precon=precon, use_armijo=True)
minim.run(fmax=1e-5)
except:
#The potential is unstable probably. Issue a warning.
msg.warn(
"Couldn't optimize the atoms object. Potential may be unstable."
)
vib = Vibrations(atoms, delta=delta)
with open("vib.log", 'a') as f:
with redirect_stdout(f):
vib.run()
vib.summary(log="vibsummary.log")
result = vib.H
#Cache the hash of the atoms object and potential that we were using so
#that we can check next time whether we should clobber the cache or not.
if aphash is not None and not tempcache:
with open(path.join(cachedir, "atomspot.hash"), 'w') as f:
f.write(aphash)
return result
import numpy as np
from ase.build import bulk
from ase.calculators.lj import LennardJones
from ase.optimize.precon import Exp, PreconLBFGS
cu0 = bulk("Cu") * (2, 2, 2)
sigma = cu0.get_distance(0,1)*(2.**(-1./6))
lj = LennardJones(sigma=sigma)
# perturb the cell
cell = cu0.get_cell()
cell *= 0.95
cell[1,0] += 0.2
cell[2,1] += 0.5
cu0.set_cell(cell, scale_atoms=True)
energies = []
for use_armijo in [True, False]:
for a_min in [None, 1e-3]:
atoms = cu0.copy()
atoms.set_calculator(lj)
opt = PreconLBFGS(atoms, precon=Exp(A=3), use_armijo=use_armijo,
a_min=a_min, variable_cell=True)
opt.run(fmax=1e-3, smax=1e-4)
energies.append(atoms.get_potential_energy())
# check we get the expected energy for all methods
assert np.abs(np.array(energies) - -63.5032311942).max() < 1e-4
def main():
atoms = build.bulk("Al")
atoms = atoms * (2, 2, 2)
print(len(atoms))
nRuns = 10
optimizerFname = "optimizer.pck"
for i in range(nRuns):
nMgAtoms = np.random.randint(0, len(atoms) / 2)
# Insert Mg atoms
system = cp.copy(atoms)
if (parallel.rank == 0):
for j in range(nMgAtoms):
system[i].symbol = "Mg"
# Shuffle the list
for j in range(10 * len(system)):
first = np.random.randint(0, len(system))
second = np.random.randint(0, len(system))
symb1 = system[first].symbol
system[first].symbol = system[second].symbol
system[second].symbol = symb1
system = parallel.broadcast(system)
# Initialize the calculator
calc = gp.GPAW(mode=gp.PW(400), xc="PBE", kpts=(4, 4, 4), nbands=-10)
system.set_calculator(calc)
traj = Trajectory("trajectoryResuse.traj", 'w', atoms)
if (i == 0):
relaxer = PreconLBFGS(UnitCellFilter(system), logfile="resuse.log")
else:
relaxer = None
relaxParams = None
if (parallel.rank == 0):
with open(optimizerFname, 'rb') as infile:
relaxParams = pck.load(infile)
relaxParams = parallel.broadcast(relaxParams)
precon = Exp(r_cut=relaxParams["r_cut"],
r_NN=relaxParams["r_NN"],
mu=relaxParams["mu"],
mu_c=relaxParams["mu_c"])
relaxer = PreconLBFGS(UnitCellFilter(system),
logfile="resuse.log",
precon=precon)
relaxer.attach(traj)
relaxer.run(fmax=0.05)
print(relaxer.iteration)
if (parallel.rank == 0):
with open(optimizerFname, 'wb') as outfile:
relaxParams = {
"r_cut": relaxer.precon.r_cut,
"r_NN": relaxer.precon.r_NN,
"mu": relaxer.precon.mu,
"mu_c": relaxer.precon.mu_c
}
pck.dump(relaxParams, outfile, pck.HIGHEST_PROTOCOL)
parallel.barrier()
