def generate_displacements(self,
distance=0.03,
cutoff_pair_distance=None,
is_plusminus='auto',
is_diagonal=True):
direction_dataset = get_third_order_displacements(
self._supercell,
self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal)
self._displacement_dataset = direction_to_displacement(
direction_dataset,
distance,
self._supercell,
cutoff_distance=cutoff_pair_distance)
if self._phonon_supercell_matrix is not None:
phonon_displacement_directions = get_least_displacements(
self._phonon_supercell_symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
self._phonon_displacement_dataset = direction_to_displacement_fc2(
phonon_displacement_directions,
distance,
self._phonon_supercell)
def generate_displacements(self,
distance=0.01,
is_plusminus='auto',
is_diagonal=True,
is_trigonal=False):
"""Generate displacements automatically
displacemsts: List of displacements in Cartesian coordinates.
[[0, 0.01, 0.00, 0.00], ...]
where each set of elements is defined by:
First value: Atom index in supercell starting with 0
Second to fourth: Displacement in Cartesian coordinates
displacement_directions:
List of directions with respect to axes. This gives only the
symmetrically non equivalent directions. The format is like:
[[0, 1, 0, 0],
[7, 1, 0, 1], ...]
where each list is defined by:
First value: Atom index in supercell starting with 0
Second to fourth: If the direction is displaced or not ( 1, 0, or -1 )
with respect to the axes.
"""
displacement_directions = get_least_displacements(
self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal,
log_level=self._log_level)
displacement_dataset = direction_to_displacement(
displacement_directions,
distance,
self._supercell)
self.set_displacement_dataset(displacement_dataset)
def generate_displacements(self,
distance=0.03,
cutoff_pair_distance=None,
is_plusminus='auto',
is_diagonal=True):
direction_dataset = get_third_order_displacements(
self._supercell,
self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal)
self._displacement_dataset = direction_to_displacement(
direction_dataset,
distance,
self._supercell,
cutoff_distance=cutoff_pair_distance)
if self._phonon_supercell_matrix is not None:
phonon_displacement_directions = get_least_displacements(
self._phonon_supercell_symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
self._phonon_displacement_dataset = direction_to_displacement_fc2(
phonon_displacement_directions,
distance,
self._phonon_supercell)
def generate_displacements(self,
distance=0.01,
is_plusminus='auto',
is_diagonal=True,
is_trigonal=False):
"""Generate displacements automatically
displacemsts: List of displacements in Cartesian coordinates.
[[0, 0.01, 0.00, 0.00], ...]
where each set of elements is defined by:
First value: Atom index in supercell starting with 0
Second to fourth: Displacement in Cartesian coordinates
displacement_directions:
List of directions with respect to axes. This gives only the
symmetrically non equivalent directions. The format is like:
[[0, 1, 0, 0],
[7, 1, 0, 1], ...]
where each list is defined by:
First value: Atom index in supercell starting with 0
Second to fourth: If the direction is displaced or not ( 1, 0, or -1 )
with respect to the axes.
"""
displacement_directions = get_least_displacements(
self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal,
log_level=self._log_level)
displacement_dataset = direction_to_displacement(
displacement_directions,
distance,
self._supercell)
self.set_displacement_dataset(displacement_dataset)
def get_fourth_order_displacements(cell,
symmetry,
is_plusminus='auto',
is_diagonal=False):
# Atoms 1, 2, and 3 are defined as follows:
#
# Atom 1: The first displaced atom. Fourth order force constant
# between Atoms 1, 2, 3, and 4 is calculated.
# Atom 2: The second displaced atom. Third order force constant
# between Atoms 2, 3, and 4 is calculated.
# Atom 3: The third displaced atom. Second order force constant
# between Atoms 3 and 4 is calculated.
# Atom 4: Force is mesuared on this atom.
# Least displacements for third order force constants
#
# Data structure
# [{'number': atom1,
# 'displacement': [0.00000, 0.007071, 0.007071],
# 'second_atoms': [ {'number': atom2,
# 'displacement': [0.007071, 0.000000, 0.007071],
# 'third_atoms': [ {'number': atom3,
# 'displacements':
# [[-0.007071, 0.000000, -0.007071],
# ,...]}, {...}, ... ]},
# Least displacements of first atoms (Atom 1) are searched by
# using respective site symmetries of the original crystal.
disps_first = get_least_displacements(symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
symprec = symmetry.get_symmetry_tolerance()
dds = []
for disp in disps_first:
atom1 = disp[0]
disp1 = disp[1:4]
site_sym = symmetry.get_site_symmetry(atom1)
dds_atom1 = {'number': atom1, 'direction': disp1, 'second_atoms': []}
reduced_site_sym = get_reduced_site_symmetry(site_sym, disp1, symprec)
second_atoms = get_least_orbits(atom1, cell, reduced_site_sym, symprec)
for atom2 in second_atoms:
reduced_bond_sym = get_bond_symmetry(reduced_site_sym,
cell.get_scaled_positions(),
atom1, atom2, symprec)
for disp2 in _get_displacements_second(reduced_bond_sym, symprec,
is_diagonal):
dds_atom2 = _get_second_displacements(atom2, disp2, cell,
reduced_bond_sym,
symprec, is_diagonal)
dds_atom1['second_atoms'].append(dds_atom2)
dds.append(dds_atom1)
write_supercells_with_three_displacements(cell, dds)
return dds
def generate_displacements(self,
distance=0.03,
cutoff_pair_distance=None,
is_plusminus='auto',
is_diagonal=True):
direction_dataset = get_third_order_displacements(
self._supercell,
self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal)
self._displacement_dataset = direction_to_displacement(
direction_dataset,
distance,
self._supercell,
cutoff_distance=cutoff_pair_distance)
if self._phonon_supercell_matrix is not None:
# 'is_diagonal=False' below is made intentionally. For
# third-order force constants, we need better accuracy,
# and I expect this choice is better for it, but not very
# sure.
# In phono3py, two atoms are displaced for each
# configuration and the displacements are chosen, first
# displacement from the perfect supercell, then second
# displacement, considering symmetry. If I choose
# is_diagonal=False for the first displacement, the
# symmetry is less broken and the number of second
# displacements can be smaller than in the case of
# is_diagonal=True for the first displacement. This is
# done in the call get_least_displacements() in
# phonon3.displacement_fc3.get_third_order_displacements().
#
# The call get_least_displacements() is only for the
# second order force constants, but 'is_diagonal=False' to
# be consistent with the above function call, and also for
# the accuracy when calculating ph-ph interaction
# strength because displacement directions are better to be
# close to perpendicular each other to fit force constants.
#
# On the discussion of the accuracy, these are just my
# expectation when I designed phono3py in the early time,
# and in fact now I guess not very different. If these are
# little different, then I should not surprise users to
# change the default behaviour. At this moment, this is
# open question and we will have more advance and should
# have better specificy external software on this.
phonon_displacement_directions = get_least_displacements(
self._phonon_supercell_symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
self._phonon_displacement_dataset = directions_to_displacement_dataset(
phonon_displacement_directions,
distance,
self._phonon_supercell)
def get_fourth_order_displacements(cell, symmetry, is_plusminus="auto", is_diagonal=False):
# Atoms 1, 2, and 3 are defined as follows:
#
# Atom 1: The first displaced atom. Fourth order force constant
# between Atoms 1, 2, 3, and 4 is calculated.
# Atom 2: The second displaced atom. Third order force constant
# between Atoms 2, 3, and 4 is calculated.
# Atom 3: The third displaced atom. Second order force constant
# between Atoms 3 and 4 is calculated.
# Atom 4: Force is mesuared on this atom.
# Least displacements for third order force constants
#
# Data structure
# [{'number': atom1,
# 'displacement': [0.00000, 0.007071, 0.007071],
# 'second_atoms': [ {'number': atom2,
# 'displacement': [0.007071, 0.000000, 0.007071],
# 'third_atoms': [ {'number': atom3,
# 'displacements':
# [[-0.007071, 0.000000, -0.007071],
# ,...]}, {...}, ... ]},
# Least displacements of first atoms (Atom 1) are searched by
# using respective site symmetries of the original crystal.
disps_first = get_least_displacements(symmetry, is_plusminus=is_plusminus, is_diagonal=False)
symprec = symmetry.get_symmetry_tolerance()
dds = []
for disp in disps_first:
atom1 = disp[0]
disp1 = disp[1:4]
site_sym = symmetry.get_site_symmetry(atom1)
dds_atom1 = {"number": atom1, "direction": disp1, "second_atoms": []}
reduced_site_sym = get_reduced_site_symmetry(site_sym, disp1, symprec)
second_atoms = get_least_orbits(atom1, cell, reduced_site_sym, symprec)
for atom2 in second_atoms:
reduced_bond_sym = get_bond_symmetry(reduced_site_sym, cell.get_scaled_positions(), atom1, atom2, symprec)
for disp2 in _get_displacements_second(reduced_bond_sym, symprec, is_diagonal):
dds_atom2 = _get_second_displacements(atom2, disp2, cell, reduced_bond_sym, symprec, is_diagonal)
dds_atom1["second_atoms"].append(dds_atom2)
dds.append(dds_atom1)
write_supercells_with_three_displacements(cell, dds)
return dds
def generate_displacements(self,
distance=0.01,
is_plusminus='auto',
is_diagonal=True,
is_trigonal=False):
"""Generate displacements automatically
displacements:
List of displacements in Cartesian coordinates.
See 'set_displacements'
displacement_directions:
List of directions with respect to axes. This gives only the
symmetrically non equivalent directions. The format is like:
[[0, 1, 0, 0],
[7, 1, 0, 1], ...]
where each list is defined by:
First value: Atom index in supercell starting with 0
Second to fourth: If the direction is displaced or not ( 1, 0, or -1 )
with respect to the axes.
"""
lattice = self._supercell.get_cell()
self._displacements = []
self._displacement_directions = \
get_least_displacements(self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal,
log_level=self._log_level)
for disp in self._displacement_directions:
atom_num = disp[0]
disp_cartesian = np.dot(disp[1:], lattice)
disp_cartesian *= distance / np.linalg.norm(disp_cartesian)
self._displacements.append([
atom_num, disp_cartesian[0], disp_cartesian[1],
disp_cartesian[2]
])
self._set_supercells_with_displacements()
def generate_displacements(self,
distance=0.01,
is_plusminus='auto',
is_diagonal=True,
is_trigonal=False):
"""Generate displacements automatically
displacements:
List of displacements in Cartesian coordinates.
See 'set_displacements'
displacement_directions:
List of directions with respect to axes. This gives only the
symmetrically non equivalent directions. The format is like:
[[0, 1, 0, 0],
[7, 1, 0, 1], ...]
where each list is defined by:
First value: Atom index in supercell starting with 0
Second to fourth: If the direction is displaced or not ( 1, 0, or -1 )
with respect to the axes.
"""
lattice = self._supercell.get_cell()
self._displacements = []
self._displacement_directions = \
get_least_displacements(self._symmetry,
is_plusminus=is_plusminus,
is_diagonal=is_diagonal,
is_trigonal=is_trigonal,
log_level=self._log_level)
for disp in self._displacement_directions:
atom_num = disp[0]
disp_cartesian = np.dot(disp[1:], lattice)
disp_cartesian *= distance / np.linalg.norm(disp_cartesian)
self._displacements.append([atom_num,
disp_cartesian[0],
disp_cartesian[1],
disp_cartesian[2]])
self._set_supercells_with_displacements()
def get_third_order_displacements(cell,
symmetry,
is_plusminus='auto',
is_diagonal=False):
# Atoms 1, 2, and 3 are defined as follows:
#
# Atom 1: The first displaced atom. Third order force constant
# between Atoms 1, 2, and 3 is calculated.
# Atom 2: The second displaced atom. Second order force constant
# between Atoms 2 and 3 is calculated.
# Atom 3: Force is mesuared on this atom.
positions = cell.get_scaled_positions()
lattice = cell.get_cell()
# Least displacements for third order force constants in yaml file
#
# Data structure
# [{'number': atom1,
# 'displacement': [0.00000, 0.007071, 0.007071],
# 'second_atoms': [ {'number': atom2,
# 'displacements': [[0.007071, 0.000000, 0.007071],
# [-0.007071, 0.000000, -0.007071]
# ,...]},
# {'number': ... } ] },
# {'number': atom1, ... } ]
# Least displacements of first atoms (Atom 1) are searched by
# using respective site symmetries of the original crystal.
disps_first = get_least_displacements(symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
symprec = symmetry.get_symmetry_tolerance()
dds = []
for disp in disps_first:
atom1 = disp[0]
disp1 = disp[1:4]
site_sym = symmetry.get_site_symmetry(atom1)
dds_atom1 = {'number': atom1,
'direction': disp1,
'second_atoms': []}
# Reduced site symmetry at the first atom with respect to
# the displacement of the first atoms.
reduced_site_sym = get_reduced_site_symmetry(site_sym, disp1, symprec)
# Searching orbits (second atoms) with respect to
# the first atom and its reduced site symmetry.
second_atoms = get_least_orbits(atom1,
cell,
reduced_site_sym,
symprec)
for atom2 in second_atoms:
dds_atom2 = get_next_displacements(atom1,
atom2,
reduced_site_sym,
positions,
symprec,
is_diagonal)
min_distance = np.linalg.norm(
np.dot(get_equivalent_smallest_vectors(
atom1,
atom2,
cell,
lattice,
symprec)[0], lattice))
dds_atom2['distance'] = min_distance
dds_atom1['second_atoms'].append(dds_atom2)
dds.append(dds_atom1)
return dds
def get_third_order_displacements(cell,
symmetry,
is_plusminus='auto',
is_diagonal=False):
# Atoms 1, 2, and 3 are defined as follows:
#
# Atom 1: The first displaced atom. Third order force constant
# between Atoms 1, 2, and 3 is calculated.
# Atom 2: The second displaced atom. Second order force constant
# between Atoms 2 and 3 is calculated.
# Atom 3: Force is mesuared on this atom.
positions = cell.get_scaled_positions()
lattice = cell.get_cell()
# Least displacements for third order force constants in yaml file
#
# Data structure
# [{'number': atom1,
# 'displacement': [0.00000, 0.007071, 0.007071],
# 'second_atoms': [ {'number': atom2,
# 'displacements': [[0.007071, 0.000000, 0.007071],
# [-0.007071, 0.000000, -0.007071]
# ,...]},
# {'number': ... } ] },
# {'number': atom1, ... } ]
# Least displacements of first atoms (Atom 1) are searched by
# using respective site symmetries of the original crystal.
disps_first = get_least_displacements(symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
symprec = symmetry.get_symmetry_tolerance()
dds = []
for disp in disps_first:
atom1 = disp[0]
disp1 = disp[1:4]
site_sym = symmetry.get_site_symmetry(atom1)
dds_atom1 = {'number': atom1,
'direction': disp1,
'second_atoms': []}
# Reduced site symmetry at the first atom with respect to
# the displacement of the first atoms.
reduced_site_sym = get_reduced_site_symmetry(site_sym, disp1, symprec)
# Searching orbits (second atoms) with respect to
# the first atom and its reduced site symmetry.
second_atoms = get_least_orbits(atom1,
cell,
reduced_site_sym,
symprec)
for atom2 in second_atoms:
dds_atom2 = get_next_displacements(atom1,
atom2,
reduced_site_sym,
positions,
symprec,
is_diagonal)
min_distance = np.linalg.norm(
np.dot(get_equivalent_smallest_vectors(
atom1,
atom2,
cell,
lattice,
symprec)[0], lattice))
dds_atom2['distance'] = min_distance
dds_atom1['second_atoms'].append(dds_atom2)
dds.append(dds_atom1)
return dds
def get_third_order_displacements(cell,
symmetry,
is_plusminus='auto',
is_diagonal=False):
"""Create dispalcement dataset
Note
----
Atoms 1, 2, and 3 are defined as follows:
Atom 1: The first displaced atom. Third order force constant
between Atoms 1, 2, and 3 is calculated.
Atom 2: The second displaced atom. Second order force constant
between Atoms 2 and 3 is calculated.
Atom 3: Force is mesuared on this atom.
Parameters
----------
cell : PhonopyAtoms
Supercell
symmetry : Symmetry
Symmetry of supercell
is_plusminus : str or bool, optional
Type of displacements, plus only (False), always plus and minus (True),
and plus and minus depending on site symmetry ('auto').
is_diagonal : bool, optional
Whether allow diagonal displacements of Atom 2 or not
Returns
-------
dict
Data structure is like:
{'natom': 64,
'cutoff_distance': 4.000000,
'first_atoms':
[{'number': atom1,
'displacement': [0.03, 0., 0.],
'second_atoms': [ {'number': atom2,
'displacement': [0., -0.03, 0.],
'distance': 2.353},
{'number': ... }, ... ] },
{'number': atom1, ... } ]}
"""
positions = cell.get_scaled_positions()
lattice = cell.get_cell().T
# Least displacements of first atoms (Atom 1) are searched by
# using respective site symmetries of the original crystal.
# 'is_diagonal=False' below is made intentionally to expect
# better accuracy.
disps_first = get_least_displacements(symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
symprec = symmetry.get_symmetry_tolerance()
dds = []
for disp in disps_first:
atom1 = disp[0]
disp1 = disp[1:4]
site_sym = symmetry.get_site_symmetry(atom1)
dds_atom1 = {'number': atom1, 'direction': disp1, 'second_atoms': []}
# Reduced site symmetry at the first atom with respect to
# the displacement of the first atoms.
reduced_site_sym = get_reduced_site_symmetry(site_sym, disp1, symprec)
# Searching orbits (second atoms) with respect to
# the first atom and its reduced site symmetry.
second_atoms = get_least_orbits(atom1, cell, reduced_site_sym, symprec)
for atom2 in second_atoms:
dds_atom2 = get_next_displacements(atom1, atom2, reduced_site_sym,
lattice, positions, symprec,
is_diagonal)
min_vec = get_equivalent_smallest_vectors(atom1, atom2, cell,
symprec)[0]
min_distance = np.linalg.norm(np.dot(lattice, min_vec))
dds_atom2['distance'] = min_distance
dds_atom1['second_atoms'].append(dds_atom2)
dds.append(dds_atom1)
return dds
def get_third_order_displacements(cell: PhonopyAtoms,
symmetry: Symmetry,
is_plusminus="auto",
is_diagonal=False):
"""Create dispalcement dataset.
Note
----
Atoms 1, 2, and 3 are defined as follows:
Atom 1: The first displaced atom. Third order force constant
between Atoms 1, 2, and 3 is calculated.
Atom 2: The second displaced atom. Second order force constant
between Atoms 2 and 3 is calculated.
Atom 3: Force is mesuared on this atom.
Parameters
----------
cell : PhonopyAtoms
Supercell
symmetry : Symmetry
Symmetry of supercell
is_plusminus : str or bool, optional
Type of displacements, plus only (False), always plus and minus (True),
and plus and minus depending on site symmetry ('auto').
is_diagonal : bool, optional
Whether allow diagonal displacements of Atom 2 or not
Returns
-------
[{'number': atom1,
'direction': [1, 0, 0], # int
'second_atoms': [ {'number': atom2,
'directions': [ [1, 0, 0], [-1, 0, 0], ... ]
'distance': distance-between-atom1-and-atom2},
{'number': ... }, ... ] },
{'number': atom1, ... } ]
"""
positions = cell.scaled_positions
lattice = cell.cell.T
# Least displacements of first atoms (Atom 1) are searched by
# using respective site symmetries of the original crystal.
# 'is_diagonal=False' below is made intentionally to expect
# better accuracy.
disps_first = get_least_displacements(symmetry,
is_plusminus=is_plusminus,
is_diagonal=False)
symprec = symmetry.tolerance
dds = []
for disp in disps_first:
atom1 = disp[0]
disp1 = disp[1:4]
site_sym = symmetry.get_site_symmetry(atom1)
dds_atom1 = {"number": atom1, "direction": disp1, "second_atoms": []}
# Reduced site symmetry at the first atom with respect to
# the displacement of the first atoms.
reduced_site_sym = get_reduced_site_symmetry(site_sym, disp1, symprec)
# Searching orbits (second atoms) with respect to
# the first atom and its reduced site symmetry.
second_atoms = get_least_orbits(atom1, cell, reduced_site_sym, symprec)
for atom2 in second_atoms:
dds_atom2 = _get_next_displacements(atom1, atom2, reduced_site_sym,
lattice, positions, symprec,
is_diagonal)
min_vec = get_smallest_vector_of_atom_pair(atom1, atom2, cell,
symprec)
min_distance = np.linalg.norm(np.dot(lattice, min_vec))
dds_atom2["distance"] = min_distance
dds_atom1["second_atoms"].append(dds_atom2)
dds.append(dds_atom1)
return dds
