def get_phonon_configs(calc, at, disps, scell, config_type):
cell = PhonopyAtoms(symbols=at.get_chemical_symbols(),
cell=at.get_cell(),
positions=at.get_positions())
phonon = Phonopy(cell, np.eye(3) * scell)
al = []
for disp in disps:
print(disp, config_type)
phonon.generate_displacements(distance=disp)
supercells = phonon.get_supercells_with_displacements()
for (i, scell) in enumerate(supercells):
at = ase.Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
at.set_calculator(calc)
e = at.get_potential_energy()
f = at.get_forces()
v = -1.0 * at.get_volume() * at.get_stress(voigt=False)
at.arrays["force"] = f
at.info["virial"] = v
at.info["config_type"] = "PH_" + config_type
at.info["energy_TB"] = e
#write("PH_{}_{}_scell_{}.xyz".format(config_type, i, disp), at)
al.append(at)
return al
def phonons(model, bulk, supercell, dx, mesh=None, points=None, n_points=50):
import model
unitcell = PhonopyAtoms(symbols=bulk.get_chemical_symbols(),
cell=bulk.get_cell(),
scaled_positions=bulk.get_scaled_positions())
phonon = Phonopy(unitcell, supercell)
phonon.generate_displacements(distance=dx)
sets_of_forces = []
for s in phonon.get_supercells_with_displacements():
at = Atoms(cell=s.get_cell(),
symbols=s.get_chemical_symbols(),
scaled_positions=s.get_scaled_positions(),
pbc=3 * [True])
at.set_calculator(model.calculator)
sets_of_forces.append(at.get_forces())
phonon.set_forces(sets_of_forces=sets_of_forces)
phonon.produce_force_constants()
properties = {}
if mesh is not None:
phonon.set_mesh(mesh, is_gamma_center=True)
qpoints, weights, frequencies, eigvecs = phonon.get_mesh()
properties["frequencies"] = frequencies.tolist()
properties["weights"] = weights.tolist()
if points is not None:
bands = []
for i in range(len(points) - 1):
band = []
for r in np.linspace(0, 1, n_points):
band.append(points[i] + (points[i + 1] - points[i]) * r)
bands.append(band)
phonon.set_band_structure(bands,
is_eigenvectors=True,
is_band_connection=False)
band_q_points, band_distances, band_frequencies, band_eigvecs = phonon.get_band_structure(
)
band_distance_max = np.max(band_distances)
band_distances = [(_b / band_distance_max).tolist()
for _b in band_distances]
band_frequencies = [_b.tolist() for _b in band_frequencies]
properties["band_q_points"] = band_q_points
properties["band_distances"] = band_distances
properties["band_frequencies"] = band_frequencies
properties["band_eigvecs"] = band_eigvecs
properties["phonopy"] = phonon
return properties
def do_phonons(strt=None, parameters=None, c_size=25):
"""
Setting up phonopy job using LAMMPS
Args:
strt: Structure object
parameters: LAMMPS input file parameters
c_size: cell-size
"""
p = get_phonopy_atoms(mat=strt)
bulk = p
dim1 = int((float(c_size) / float(max(abs(strt.lattice.matrix[0]))))) + 1
dim2 = int(float(c_size) / float(max(abs(strt.lattice.matrix[1])))) + 1
dim3 = int(float(c_size) / float(max(abs(strt.lattice.matrix[2])))) + 1
Poscar(strt).write_file("POSCAR")
tmp = strt.copy()
tmp.make_supercell([dim1, dim2, dim3])
Poscar(tmp).write_file("POSCAR-Super.vasp")
phonon = Phonopy(bulk, [[dim1, 0, 0], [0, dim2, 0], [0, 0, dim3]]) # ,
print("[Phonopy] Atomic displacements:")
disps = phonon.get_displacements()
for d in disps:
print("[Phonopy]", d[0], d[1:])
supercells = phonon.get_supercells_with_displacements()
# Force calculations by calculator
set_of_forces = []
disp = 0
for scell in supercells:
cell = Atoms(
symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True,
)
disp = disp + 1
mat = Poscar(AseAtomsAdaptor().get_structure(cell))
mat.comment = str("disp-") + str(disp)
parameters["min"] = "skip"
parameters["control_file"] = "/users/knc6/in.phonon"
# a,b,forces=run_job(mat=mat,parameters={'min':'skip','pair_coeff': '/data/knc6/JARVIS-FF-NEW/ALLOY4/Mishin-Ni-Al-2009.eam.alloy', 'control_file': '/users/knc6/in.phonon', 'pair_style': 'eam/alloy', 'atom_style': 'charge'})
a, b, forces = run_job(mat=mat, parameters=parameters)
print("forces=", forces)
drift_force = forces.sum(axis=0)
print("drift forces=", drift_force)
print("[Phonopy] Drift force:", "%11.5f" * 3 % tuple(drift_force))
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
set_of_forces.append(forces)
phonon.produce_force_constants(forces=set_of_forces)
write_FORCE_CONSTANTS(phonon.get_force_constants(), filename="FORCE_CONSTANTS")
print()
print("[Phonopy] Phonon frequencies at Gamma:")
def create_supercells_with_displacements_inline(**kwargs):
from phonopy.structure.atoms import Atoms as PhonopyAtoms
from phonopy import Phonopy
structure = kwargs.pop('structure')
phonopy_input = kwargs.pop('phonopy_input').get_dict()
# Generate phonopy phonon object
bulk = PhonopyAtoms(symbols=[site.kind_name for site in structure.sites],
positions=[site.position for site in structure.sites],
cell=structure.cell)
phonon = Phonopy(bulk,
phonopy_input['supercell'],
primitive_matrix=phonopy_input['primitive'],
symprec=phonopy_input['symmetry_precision'])
phonon.generate_displacements(distance=phonopy_input['distance'])
cells_with_disp = phonon.get_supercells_with_displacements()
# Transform cells to StructureData and set them ready to return
disp_cells = {}
for i, phonopy_supercell in enumerate(cells_with_disp):
supercell = StructureData(cell=phonopy_supercell.get_cell())
for symbol, position in zip(phonopy_supercell.get_chemical_symbols(),
phonopy_supercell.get_positions()):
supercell.append_atom(position=position, symbols=symbol)
disp_cells["structure_{}".format(i)] = supercell
return disp_cells
def create_supercells_with_displacements_using_phonopy(structure, ph_settings):
"""
Use phonopy to create the supercells with displacements to calculate the force constants by using
finite displacements methodology
:param structure: StructureData object
:param phonopy_input: ParametersData object containing a dictionary with the data needed for phonopy
:return: A set of StructureData Objects containing the supercells with displacements
"""
from phonopy import Phonopy
# Generate phonopy phonon object
phonon = Phonopy(phonopy_bulk_from_structure(structure),
supercell_matrix=ph_settings.dict.supercell,
primitive_matrix=ph_settings.dict.primitive,
symprec=ph_settings.dict.symmetry_precision)
phonon.generate_displacements(distance=ph_settings.dict.distance)
cells_with_disp = phonon.get_supercells_with_displacements()
# Transform cells to StructureData and set them ready to return
data_sets = phonon.get_displacement_dataset()
data_sets_object = ForceSetsData(data_sets=data_sets)
disp_cells = {'data_sets': data_sets_object}
for i, phonopy_supercell in enumerate(cells_with_disp):
supercell = StructureData(cell=phonopy_supercell.get_cell())
for symbol, position in zip(phonopy_supercell.get_chemical_symbols(),
phonopy_supercell.get_positions()):
supercell.append_atom(position=position, symbols=symbol)
disp_cells["structure_{}".format(i)] = supercell
return disp_cells
def get_displaced_structures(pmg_structure,
atom_disp=0.01,
supercell_matrix=None,
yaml_fname=None,
**kwargs):
r"""
Generate a set of symmetrically inequivalent displaced structures for
phonon calculations.
Args:
pmg_structure (Structure): A pymatgen structure object.
atom_disp (float): Atomic displacement. Default is 0.01 $\\AA$.
supercell_matrix (3x3 array): Scaling matrix for supercell.
yaml_fname (string): If not None, it represents the full path to
the outputting displacement yaml file, e.g. disp.yaml.
**kwargs: Parameters used in Phonopy.generate_displacement method.
Return:
A list of symmetrically inequivalent structures with displacements, in
which the first element is the perfect supercell structure.
"""
is_plusminus = kwargs.get("is_plusminus", "auto")
is_diagonal = kwargs.get("is_diagonal", True)
is_trigonal = kwargs.get("is_trigonal", False)
ph_structure = get_phonopy_structure(pmg_structure)
if supercell_matrix is None:
supercell_matrix = np.eye(3) * np.array((1, 1, 1))
phonon = Phonopy(unitcell=ph_structure, supercell_matrix=supercell_matrix)
phonon.generate_displacements(
distance=atom_disp,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal,
)
if yaml_fname is not None:
displacements = phonon.get_displacements()
write_disp_yaml(
displacements=displacements,
supercell=phonon.get_supercell(),
filename=yaml_fname,
)
# Supercell structures with displacement
disp_supercells = phonon.get_supercells_with_displacements()
# Perfect supercell structure
init_supercell = phonon.get_supercell()
# Structure list to be returned
structure_list = [get_pmg_structure(init_supercell)]
for c in disp_supercells:
if c is not None:
structure_list.append(get_pmg_structure(c))
return structure_list
def do_phonons(strt=None,parameters=None):
p= get_phonopy_atoms(mat=strt)
bulk =p
c_size=parameters['phon_size']
dim1=int((float(c_size)/float( max(abs(strt.lattice.matrix[0])))))+1
dim2=int(float(c_size)/float( max(abs(strt.lattice.matrix[1]))))+1
dim3=int(float(c_size)/float( max(abs(strt.lattice.matrix[2]))))+1
Poscar(strt).write_file("POSCAR")
tmp=strt.copy()
tmp.make_supercell([dim1,dim2,dim3])
Poscar(tmp).write_file("POSCAR-Super.vasp")
print ('supercells',dim1,dim2,dim3)
phonon = Phonopy(bulk,[[dim1,0,0],[0,dim2,0],[0,0,dim3]])
print ("[Phonopy] Atomic displacements:")
disps = phonon.get_displacements()
for d in disps:
print ("[Phonopy]", d[0], d[1:])
supercells = phonon.get_supercells_with_displacements()
# Force calculations by calculator
set_of_forces = []
disp=0
for scell in supercells:
cell = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
disp=disp+1
mat = Poscar(AseAtomsAdaptor().get_structure(cell))
mat.comment=str("disp-")+str(disp)
parameters['min']='skip'
parameters['control_file']= parameters['phonon_control_file'] #'/users/knc6/in.phonon'
#a,b,forces=run_job(mat=mat,parameters={'min':'skip','pair_coeff': '/data/knc6/JARVIS-FF-NEW/ALLOY4/Mishin-Ni-Al-2009.eam.alloy', 'control_file': '/users/knc6/in.phonon', 'pair_style': 'eam/alloy', 'atom_style': 'charge'})
a,b,forces=run_job(mat=mat,parameters=parameters)
#print "forces=",forces
drift_force = forces.sum(axis=0)
#print "drift forces=",drift_force
#print "[Phonopy] Drift force:", "%11.5f"*3 % tuple(drift_force)
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
set_of_forces.append(forces)
phonon.produce_force_constants(forces=set_of_forces)
write_FORCE_CONSTANTS(phonon.get_force_constants(),
filename="FORCE_CONSTANTS")
#print
#print "[Phonopy] Phonon frequencies at Gamma:"
for i, freq in enumerate(phonon.get_frequencies((0, 0, 0))):
print ("[Phonopy] %3d: %10.5f THz" % (i + 1, freq)) # THz
def get_displaced_structures(pmg_structure, atom_disp=0.01,
supercell_matrix=None, yaml_fname=None, **kwargs):
"""
Generate a set of symmetrically inequivalent displaced structures for
phonon calculations.
Args:
pmg_structure (Structure): A pymatgen structure object.
atom_disp (float): Atomic displacement. Default is 0.01 $\\AA$.
supercell_matrix (3x3 array): Scaling matrix for supercell.
yaml_fname (string): If not None, it represents the full path to
the outputting displacement yaml file, e.g. disp.yaml.
**kwargs: Parameters used in Phonopy.generate_displacement method.
Return:
A list of symmetrically inequivalent structures with displacements, in
which the first element is the perfect supercell structure.
"""
is_plusminus = kwargs.get("is_plusminus", "auto")
is_diagonal = kwargs.get("is_diagonal", True)
is_trigonal = kwargs.get("is_trigonal", False)
ph_structure = get_phonopy_structure(pmg_structure)
if supercell_matrix is None:
supercell_matrix = np.eye(3) * np.array((1, 1, 1))
phonon = Phonopy(unitcell=ph_structure, supercell_matrix=supercell_matrix)
phonon.generate_displacements(distance=atom_disp,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal)
if yaml_fname is not None:
displacements = phonon.get_displacements()
directions = phonon.get_displacement_directions()
write_disp_yaml(displacements=displacements,
supercell=phonon.get_supercell(),
directions=directions, filename=yaml_fname)
# Supercell structures with displacement
disp_supercells = phonon.get_supercells_with_displacements()
# Perfect supercell structure
init_supercell = phonon.get_supercell()
# Structure list to be returned
structure_list = [get_pmg_structure(init_supercell)]
for c in disp_supercells:
if c is not None:
structure_list.append(get_pmg_structure(c))
return structure_list
def _calc_quick(atoms, supercell=(1, 1, 1), delta=0.01):
"""Calculates the Hessian for a given atoms object just like :func:`calc`,
*but*, it uses symmetry to speed up the calculation. Depending on the
calculator being used, it is possible that the symmetrized result may be
different from the full result with all displacements, done manually by
:func:`calc`.
Args:
atoms (matdb.atoms.Atoms): atomic structure of the *primitive*.
supercell (list): or `tuple` or :class:`numpy.ndarray` specifying the
integer supercell matrix.
delta (float): displacement in Angstroms of each atom when computing the
phonons.
Returns:
numpy.ndarray: Hessian matrix that has dimension `(natoms*3, natoms*3)`,
where `natoms` is the number of atoms in the *supercell*.
"""
#We need to make sure we are at the zero of the potential before
ratoms = atoms.copy()
try:
with open("phonons.log", 'w') as f:
with redirect_stdout(f):
print(ratoms.get_forces())
minim = FIRE(ratoms)
minim.run(fmax=1e-4, steps=100)
except:
#The potential is unstable probably. Issue a warning.
msg.warn(
"Couldn't optimize the atoms object. Potential may be unstable.")
primitive = matdb_to_phonopy(ratoms)
phonon = Phonopy(primitive, conform_supercell(supercell))
phonon.generate_displacements(distance=delta)
supercells = phonon.get_supercells_with_displacements()
pot = atoms.get_calculator()
assert pot is not None
forces = []
for scell in supercells:
matoms = phonopy_to_matdb(scell)
#Call a manual reset of the calculator so that we explicitly recalculate
#the forces for the current atoms object.
pot.reset()
matoms.set_calculator(pot)
forces.append(matoms.get_forces())
phonon.set_forces(forces)
phonon.produce_force_constants()
return unroll_fc(phonon._force_constants)
def create_supercells_with_displacements_using_phonopy(structure,
phonopy_input):
"""
Create the supercells with the displacements to use the finite displacements methodology to calculate the
force constants
:param structure: Aiida StructureData Object
:param phonopy_input: Aiida Parametersdata object containing a dictionary with the data needed to run phonopy:
supercells matrix, primitive matrix and displacement distance.
:return: dictionary of Aiida StructureData Objects containing the cells with displacements
"""
from phonopy.structure.atoms import Atoms as PhonopyAtoms
from phonopy import Phonopy
import numpy as np
# Generate phonopy phonon object
bulk = PhonopyAtoms(symbols=[site.kind_name for site in structure.sites],
positions=[site.position for site in structure.sites],
cell=structure.cell)
phonopy_input = phonopy_input.get_dict()
phonon = Phonopy(bulk,
phonopy_input['supercell'],
primitive_matrix=phonopy_input['primitive'])
phonon.generate_displacements(distance=phonopy_input['distance'])
cells_with_disp = phonon.get_supercells_with_displacements()
# Transform cells to StructureData and set them ready to return
data_sets = phonon.get_displacement_dataset()
data_sets_object = ArrayData()
for i, first_atoms in enumerate(data_sets['first_atoms']):
data_sets_array = np.array([
first_atoms['direction'], first_atoms['number'],
first_atoms['displacement']
])
data_sets_object.set_array('data_sets_{}'.format(i), data_sets_array)
disp_cells = {'data_sets': data_sets_object}
for i, phonopy_supercell in enumerate(cells_with_disp):
supercell = StructureData(cell=phonopy_supercell.get_cell())
for symbol, position in zip(phonopy_supercell.get_chemical_symbols(),
phonopy_supercell.get_positions()):
supercell.append_atom(position=position, symbols=symbol)
disp_cells["structure_{}".format(i)] = supercell
return disp_cells
def _get_phononobject_phonopy(self,
structure,
potential,
smat,
save_parameters,
path,
displacement_distance=0.01):
cell = get_phonopy_structure(structure)
phonon = Phonopy(cell,
smat,
primitive_matrix=[[1.0, 0.0, 0.0], [0.0, 1, 0.0],
[0., 0., 1.0]],
factor=VaspToTHz)
# displacements
phonon.generate_displacements(distance=displacement_distance)
print("[Phonopy] Atomic displacements:")
disps = phonon.get_displacements()
for d in disps:
print("[Phonopy] %d %s" % (d[0], d[1:]))
supercells = phonon.get_supercells_with_displacements()
# Force calculations by calculator
set_of_forces = []
for scell in supercells:
cell = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
cell.set_calculator(potential)
# this part is adapted from: https://web.archive.org/web/20200610084959/https://github.com/phonopy/phonopy/blob/develop/example/ase/8Si-phonon.py
# Copyright by Atsushi Togo
forces = cell.get_forces()
drift_force = forces.sum(axis=0)
print(
("[Phonopy] Drift force:" + "%11.5f" * 3) % tuple(drift_force))
for force in forces:
force -= drift_force / forces.shape[0]
set_of_forces.append(forces)
phonon.produce_force_constants(forces=set_of_forces)
if save_parameters:
phonon.save(path)
return phonon
def get_phonon_configs(calc, at, disps, scell, config_type):
cell = PhonopyAtoms(symbols=at.get_chemical_symbols(),
cell=at.get_cell(),
positions=at.get_positions())
phonon = Phonopy(cell, np.eye(3) * scell)
al = []
for disp in disps:
phonon.generate_displacements(distance=disp)
supercells = phonon.get_supercells_with_displacements()
for (i, scell) in enumerate(supercells):
at = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
at.set_calculator(calc)
energy = at.get_potential_energy(force_consistent=True)
forces = at.get_forces()
stress = at.get_stress(voigt=False)
drift_force = forces.sum(axis=0)
print(("[Phonopy] Drift force:" + "%11.5f" * 3) %
tuple(drift_force))
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
at.arrays["force"] = forces
at.info["virial"] = -1.0 * at.get_volume() * stress
at.info["energy"] = energy
at.info["config_type"] = "PH_" + config_type
write("PH_{}_{}_scell_{}.xyz".format(config_type, i, disp), at)
al.append(at)
return al
class PhononFromModel(object):
"""
This class uses frozen phonon method to calculate the phonon dispersion curves and thermodynamic
properties of a structure.
The steps are as follows:
1. Displaced structures are obtained from pristine structure via phonopy.
2. The forces of each displaced structures are calculated by model
3. The forces are passed to phonopy object and the force constant are produced
4. Phonon is calculated once the force constant matrix is available.
Args:
model (model object): a model object that has a method "calculate_forces" that takes in a list of
structures and return a list of N*3 forces, where N are the number of atoms in each structures
structure (pymatgen structure): a pristine pymatgen structure
atom_disp (float): small displacements in Angstrom
"""
def __init__(self, model=None, structure=None, atom_disp=0.015, **kwargs):
self.model = model
self.structure = structure
self.atom_disp = atom_disp
self.qpoints, self.vertices = get_qpoints_and_vertices(self.structure)
is_plusminus = kwargs.get('is_plusminus', True)
is_diagonal = kwargs.get('is_diagonal', True)
is_trigonal = kwargs.get('is_diagonal', False)
supercell_matrix = kwargs.get('is_diagonal', None)
ph_structure = get_phonopy_structure(self.structure)
if supercell_matrix is None:
supercell_matrix = np.eye(3) * np.array((1, 1, 1))
self.phonon = Phonopy(unitcell=ph_structure, supercell_matrix=supercell_matrix)
self.phonon.generate_displacements(distance=self.atom_disp,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal)
disp_supercells = self.phonon.get_supercells_with_displacements()
# Perfect supercell structure
init_supercell = self.phonon.get_supercell()
# Structure list to be returned
self.structure_list = [get_pmg_structure(init_supercell)]
for c in disp_supercells:
if c is not None:
self.structure_list.append(get_pmg_structure(c))
forces = self.model.calculate_forces(self.structure_list)
self.phonon.set_forces(forces[1:])
self.phonon.produce_force_constants()
logging.info("Force constant produced")
def get_thermo_properties(self, mesh=[8, 8, 8], t_step=10, t_max=3000, t_min=0):
self.phonon.set_mesh(mesh=mesh)
self.phonon.set_thermal_properties(t_step=t_step,
t_max=t_max,
t_min=t_min)
plt = self.phonon.plot_thermal_properties()
return plt
def get_bs_plot(self, points_per_line=50, figsize=(6, 4), ylim=[-1, 5]):
bands = []
bands = append_bands(bands, self.qpoints, points_per_line)
self.phonon.set_band_structure(bands)
q_points, self.distances, self.frequencies, eigvecs = self.phonon.get_band_structure()
special_points = self.phonon._band_structure._special_points
distance = self.phonon._band_structure._distance
plt.figure(figsize=figsize)
for j, (d, f) in enumerate(zip(self.distances, self.frequencies)):
for i, freqs in enumerate(f.T):
if i == 0 and j == 0:
plt.plot(d, freqs, "b-", lw=1)
else:
plt.plot(d, freqs, "b-", lw=1)
for sp in special_points:
plt.axvline(x=sp, linestyle=':', linewidth=1, color='k')
plt.axhline(y=0, linestyle=':', linewidth=1, color='k')
plt.xticks(special_points, ["$\mathrm{%s}$" % i for i in self.vertices])
plt.xlabel("Wave vector")
plt.ylabel("Frequency (THz)")
plt.xlim(0, distance)
plt.ylim(ylim)
plt.yticks(list(range(ylim[0], ylim[-1]+1)))
plt.tight_layout()
return plt
def get_phonon_distrib_alist(
prim_cell,
NNN,
T,
seed_range,
calc,
cp_files=None,
plus_minus=True,
delta=0.01,
):
"""
prim_cell (str)
ASE readable primitive unitcell structure file.
NNN (list of int, shape: (3,3))
Supercell matrix used to calculate force constants.
T (float)
Temperature in Kelvin unit.
seed_range (range or list of int)
Seeds for random number generation.
calc (str, choices: ('lmp', 'vasp'))
Calculator for force calculation.
cp_files (list of str)
List of input files for force calculation.
plus_minus (bool)
Option handed to ASE function.
delta (float)
Displacement in Angstrom for finite displacement method.
"""
# Main
from ase.io import read, write
atoms = read(prim_cell)
from phonopy import Phonopy
phonon = Phonopy(
atoms,
NNN,
)
phonon.generate_displacements(
delta,
)
pho_super = phonon.get_supercell()
pho_disp = phonon.get_supercells_with_displacements()
from phonopy.interface import vasp
vasp.write_supercells_with_displacements(
pho_super,
pho_disp,
)
import ss_phonopy as ssp
phonon = ssp.calc_phonon(
calc,
phonon,
cp_files=cp_files,
)
masses = pho_super.masses
job_name = 'eig_x{}{}{}_d{:5.3f}_sym{}'.format(NNN[0][0], NNN[1][1], NNN[2][2], delta, phonon._is_symmetry)
try:
e_s = np.load('{}.npz'.format(job_name))
except:
print('Failed to load {}.npz file. Start to solve eigen problem.'.format(job_name))
eigen_set = get_eigen_set(
phonon.get_force_constants(),
masses,
)
np.savez('{}.npz'.format(job_name), w2=eigen_set[0], D=eigen_set[1])
else:
print('Successfully loaded {}.npz file!'.format(job_name))
eigen_set = (e_s['w2'], e_s['D'])
from ase.md.velocitydistribution import phonon_harmonics
from ase import Atoms, units
alist = []
for i in seed_range:
d_ac, v_ac = phonon_harmonics(
None,
masses,
T *units.kB,
eigen_set=eigen_set,
# rng=np.random.rand,
seed=i,
quantum=True,
plus_minus=plus_minus,
# return_eigensolution=False,
# failfast=True,
)
new_super = Atoms(
cell = pho_super.get_cell(),
symbols = pho_super.get_chemical_symbols(),
positions = pho_super.get_positions() + d_ac,
velocities = v_ac,
pbc = True,
)
alist.append(new_super)
return(alist)
relax.run(fmax=fmax)
Unit_cell = api_ph.aseAtoms_to_phonopyAtoms(ucell_ase)
Intf_vasp.write_vasp('POSCAR_relx', Unit_cell)
else:
Unit_cell = Intf_vasp.read_vasp(
"POSCAR") # read prim cell from the POSCAR file
# generate displacements
prim_mat = np.eye(3) #[[0, 0.5, 0.5],[0.5, 0, 0.5],[0.5, 0.5, 0]]
phonon_scell = Phonopy(
Unit_cell, np.diag(Ncells),
primitive_matrix=prim_mat) # generate an phononpy object for LD calc.
phonon_scell.generate_displacements(distance=0.03) # vasp
Scells_phonopy = phonon_scell.get_supercells_with_displacements(
) # This returns a list of Phononpy atoms object
# convert phonopy atoms objects to quippy atom objects
Scells_quippy = []
for scell in Scells_phonopy:
scell_qp = api_ph.phonopyAtoms_to_aseAtoms(scell)
Scells_quippy.append(scell_qp)
# calculate forces and convert to phonopy force_sets
force_gap_scells = api_q.calc_force_sets_GAP(gp_xml_file, Scells_quippy)
#parse force set and calc force constants
phonon_scell.set_forces(force_gap_scells)
PhonIO.write_FORCE_SETS(phonon_scell.get_displacement_dataset()
) # write forces & displacements to FORCE_SET
force_set = PhonIO.parse_FORCE_SETS() # parse force_sets
def phonons(self,
atoms=None,
lammps_cmd="",
enforce_c_size=15.0,
parameters={}):
"""Make Phonon calculation setup."""
from phonopy import Phonopy
from phonopy.file_IO import (
# parse_FORCE_CONSTANTS,
write_FORCE_CONSTANTS, )
bulk = atoms.phonopy_converter()
dim = get_supercell_dims(atoms, enforce_c_size=enforce_c_size)
atoms = atoms.make_supercell([dim[0], dim[1], dim[2]])
Poscar(atoms).write_file("POSCAR")
atoms = atoms.make_supercell_matrix([dim[0], dim[1], dim[2]])
Poscar(atoms).write_file("POSCAR-Super.vasp")
phonon = Phonopy(bulk,
[[dim[0], 0, 0], [0, dim[1], 0], [0, 0, dim[2]]])
print("[Phonopy] Atomic displacements1:", bulk)
print("[Phonopy] Atomic displacements2:", phonon, dim[0], dim[1],
dim[2])
phonon.generate_displacements(distance=0.03)
disps = phonon.get_displacements()
print("[Phonopy] Atomic displacements3:", disps)
for d in disps:
print("[Phonopy]", d[0], d[1:])
supercells = phonon.get_supercells_with_displacements()
# Force calculations by calculator
set_of_forces = []
disp = 0
from ase import Atoms as AseAtoms
for scell in supercells:
ase_atoms = AseAtoms(
symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True,
)
j_atoms = ase_to_atoms(ase_atoms)
disp = disp + 1
parameters["control_file"] = "run0.mod"
a, b, forces = LammpsJob(
atoms=j_atoms,
lammps_cmd=lammps_cmd,
parameters=parameters,
jobname="disp-" + str(disp),
).runjob()
print("forces=", forces)
drift_force = forces.sum(axis=0)
print("drift forces=", drift_force)
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
set_of_forces.append(forces)
phonon.produce_force_constants(forces=set_of_forces)
write_FORCE_CONSTANTS(phonon.get_force_constants(),
filename="FORCE_CONSTANTS")
print()
print("[Phonopy] Phonon frequencies at Gamma:")
def calculate_phonon(atoms,
calc,
ndim=np.eye(3),
primitive_matrix=np.eye(3),
distance=0.01,
factor=VaspToTHz,
is_symmetry=True,
symprec=1e-5,
func=None,
**func_args):
"""
"""
if 'magmoms' in atoms.arrays:
is_mag = True
else:
is_mag = False
# 1. get displacements and supercells
atoms.set_calculator(calc)
# bulk = PhonopyAtoms(atoms=atoms)
if is_mag:
bulk = PhonopyAtoms(
symbols=atoms.get_chemical_symbols(),
scaled_positions=atoms.get_scaled_positions(),
cell=atoms.get_cell(),
magmoms=atoms.arrays['magmoms'],
)
else:
bulk = PhonopyAtoms(symbols=atoms.get_chemical_symbols(),
scaled_positions=atoms.get_scaled_positions(),
cell=atoms.get_cell())
phonon = Phonopy(bulk,
ndim,
primitive_matrix=primitive_matrix,
factor=factor,
symprec=symprec)
phonon.generate_displacements(distance=distance)
disps = phonon.get_displacements()
for d in disps:
print("[phonopy] %d %s" % (d[0], d[1:]))
supercell0 = phonon.get_supercell()
supercells = phonon.get_supercells_with_displacements()
write_supercells_with_displacements(supercell0, supercells)
write_disp_yaml(disps, supercell0)
# 2. calculated forces.
set_of_forces = []
for iscell, scell in enumerate(supercells):
cell = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
if is_mag:
cell.set_initial_magnetic_moments(
atoms.get_initial_magnetic_moments())
cell.set_calculator(calc)
dir_name = "PHON_CELL%s" % iscell
cur_dir = os.getcwd()
if not os.path.exists(dir_name):
os.mkdir(dir_name)
os.chdir(dir_name)
forces = cell.get_forces()
#print "[Phonopy] Forces: %s" % forces
# Do something other than calculating the forces with func.
# func: func(atoms, calc, func_args)
if func is not None:
func(cell, calc, **func_args)
os.chdir(cur_dir)
drift_force = forces.sum(axis=0)
#print "[Phonopy] Drift force:", "%11.5f" * 3 % tuple(drift_force)
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
set_of_forces.append(forces)
# Phonopy post-process
phonon.produce_force_constants(forces=set_of_forces)
force_constants = phonon.get_force_constants()
write_FORCE_CONSTANTS(force_constants, filename='FORCE_CONSTANTS')
print('')
print("[Phonopy] Phonon frequencies at Gamma:")
for i, freq in enumerate(phonon.get_frequencies((0, 0, 0))):
print("[Phonopy] %3d: %10.5f THz" % (i + 1, freq)) # THz
print("[Phonopy] %3d: %10.5f cm-1" % (i + 1, freq * 33.35)) #cm-1
return phonon
def calculate_phonon(atoms,
calc=None,
forces_set_file=None,
ndim=np.eye(3),
primitive_matrix=np.eye(3),
distance=0.01,
factor=VaspToTHz,
is_plusminus='auto',
is_symmetry=True,
symprec=1e-5,
func=None,
prepare_initial_wavecar=False,
skip=None,
restart=True,
parallel=True,
sc_mag=None,
**func_args):
"""
"""
if 'magmoms' in atoms.arrays or 'initial_magmoms' in atoms.arrays:
is_mag = True
else:
is_mag = False
print("is_mag: ", is_mag)
# 1. get displacements and supercells
if calc is not None:
atoms.set_calculator(calc)
# bulk = PhonopyAtoms(atoms=atoms)
if is_mag:
bulk = PhonopyAtoms(
symbols=atoms.get_chemical_symbols(),
scaled_positions=atoms.get_scaled_positions(),
cell=atoms.get_cell(),
magmoms=atoms.arrays['initial_magmoms'],
)
else:
bulk = PhonopyAtoms(symbols=atoms.get_chemical_symbols(),
scaled_positions=atoms.get_scaled_positions(),
cell=atoms.get_cell())
phonon = Phonopy(bulk,
ndim,
primitive_matrix=primitive_matrix,
factor=factor,
symprec=symprec)
phonon.generate_displacements(distance=distance, is_plusminus=is_plusminus)
disps = phonon.get_displacements()
for d in disps:
print(("[phonopy] %d %s" % (d[0], d[1:])))
supercell0 = phonon.get_supercell()
supercells = phonon.get_supercells_with_displacements()
#write_supercells_with_displacements(supercell0, supercells)
write_disp_yaml(disps, supercell0)
# 2. calculated forces.
if forces_set_file is not None:
symmetry = phonon.get_symmetry()
set_of_forces = parse_FORCE_SETS(
is_translational_invariance=False,
filename=forces_set_file) # ['first_atoms']
# set_of_forces=np.array(set_of_forces)
#set_of_forces=[np.asarray(f) for f in set_of_forces]
phonon.set_displacement_dataset(set_of_forces)
phonon.produce_force_constants()
else:
# initialize set of forces
if restart and os.path.exists('forces_set.pickle'):
try:
with open("forces_set.pickle", 'rb') as myfile:
set_of_forces = pickle.load(myfile)
iskip = len(set_of_forces) - 1
except:
set_of_forces = []
iskip = -1
else:
set_of_forces = []
iskip = -1
if prepare_initial_wavecar and skip is None:
scell = supercell0
cell = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
if is_mag:
cell.set_initial_magnetic_moments(sc_mag)
write('Supercell.cif', cell)
mcalc = copy.deepcopy(calc)
mcalc.set(lwave=True, lcharg=True)
cell.set_calculator(mcalc)
dir_name = "SUPERCELL0"
cur_dir = os.getcwd()
if not os.path.exists(dir_name):
os.mkdir(dir_name)
os.chdir(dir_name)
mcalc.scf_calculation(cell)
os.chdir(cur_dir)
def calc_force(iscell):
scell = supercells[iscell]
cell = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
if is_mag:
cell.set_initial_magnetic_moments(sc_mag)
cell.set_calculator(copy.deepcopy(calc))
dir_name = "PHON_CELL%s" % iscell
cur_dir = os.getcwd()
if not os.path.exists(dir_name):
os.mkdir(dir_name)
if prepare_initial_wavecar:
os.system('ln -s %s %s' %
(os.path.abspath("SUPERCELL0/WAVECAR"),
os.path.join(dir_name, 'WAVECAR')))
os.chdir(dir_name)
forces = cell.get_forces()
print("[Phonopy] Forces: %s" % forces)
# Do something other than calculating the forces with func.
# func: func(atoms, calc, func_args)
if func is not None:
func(cell, calc, **func_args)
os.chdir(cur_dir)
drift_force = forces.sum(axis=0)
print("[Phonopy] Drift force:", "%11.5f" * 3 % tuple(drift_force))
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
return forces
if parallel:
p = Pool()
set_of_forces = p.map(calc_force,
list(range(iskip, len(supercells))))
else:
for iscell, scell in enumerate(supercells):
if iscell > iskip:
fs = calc_force(iscell)
set_of_forces.append(fs)
with open("forces_set.pickle", 'wb') as myfile:
pickle.dump(set_of_forces, myfile)
phonon.produce_force_constants(forces=np.array(set_of_forces))
force_constants = phonon.get_force_constants()
write_FORCE_CONSTANTS(force_constants, filename='FORCE_CONSTANTS')
#print("[Phonopy] Phonon frequencies at Gamma:")
# for i, freq in enumerate(phonon.get_frequencies((0, 0, 0))):
# print(("[Phonopy] %3d: %10.5f THz" % (i + 1, freq))) # THz
# print(("[Phonopy] %3d: %10.5f cm-1" % (i + 1, freq * 33.35))) #cm-1
with open('phonon.pickle', 'wb') as myfile:
pickle.dump(phonon, myfile)
phonon.save(settings={'force_constants': True})
return phonon
phonon = Phonopy(
atoms,
# [[N,0,0],[0,N,0],[0,0,N]],
NNN,
# primitive_matrix = [[0.5,0.5,0],[0,0.5,0.5],[0.5,0,0.5]],
primitive_matrix=primitive_matrix,
nac_params=nac_params,
factor=factor,
is_symmetry=is_symmetry,
)
phonon.generate_displacements(
distance=delta,
is_plusminus=is_plusminus,
)
pho_disp = phonon.get_supercells_with_displacements()
vasp.write_supercells_with_displacements(
phonon.get_supercell(),
pho_disp,
)
######### get new phonon object ##########
#
import ss_phonopy as ssp
phonon = ssp.calc_phonon(
calc,
phonon,
acoustic_sum_rule=acou_sum_rule,
rot_sum_rule=rot_sum_rule,
r_cut=r_cut,
calc = GPAW(mode=PW(300),
kpts={'size': (4, 4, 4)},
symmetry={'symmorphic': False})
phonon = Phonopy(bulk,
[[1,0,0],[0,1,0],[0,0,1]],
primitive_matrix=[[0, 0.5, 0.5],
[0.5, 0, 0.5],
[0.5, 0.5, 0]],
distance=0.01)
print "[Phonopy] Atomic displacements:"
disps = phonon.get_displacements()
for d in disps:
print "[Phonopy]", d[0], d[1:]
supercells = phonon.get_supercells_with_displacements()
# Force calculations by calculator
set_of_forces = []
for scell in supercells:
cell = Atoms(symbols=scell.get_chemical_symbols(),
scaled_positions=scell.get_scaled_positions(),
cell=scell.get_cell(),
pbc=True)
cell.set_calculator(calc)
forces = cell.get_forces()
drift_force = forces.sum(axis=0)
print "[Phonopy] Drift force:", "%11.5f"*3 % tuple(drift_force)
# Simple translational invariance
for force in forces:
force -= drift_force / forces.shape[0]
