def bandpath(self, path=None, npoints=50, special_points=None):
# npoints should depend on the length of the path
if special_points is None:
special_points = self.get_special_points()
if path is None:
path = self.variant.special_path
bandpath = BandPath(cell=self.tocell(),
labelseq=path,
special_points=special_points)
return bandpath.interpolate(npoints=npoints)
def bandpath(self, path=None, npoints=None, density=None,
special_points=None, eps=2e-4, *, pbc=None):
"""Build a :class:`~ase.dft.kpoints.BandPath` for this cell.
If special points are None, determine the Bravais lattice of
this cell and return a suitable Brillouin zone path with
standard special points.
If special special points are given, interpolate the path
directly from the available data.
Parameters:
path: string
String of special point names defining the path, e.g. 'GXL'.
npoints: int
Number of points in total. Note that at least one point
is added for each special point in the path.
density: float
density of kpoints along the path in Å⁻¹.
special_points: dict
Dictionary mapping special points to scaled kpoint coordinates.
For example ``{'G': [0, 0, 0], 'X': [1, 0, 0]}``.
eps: float
Tolerance for determining Bravais lattice.
pbc: three bools
Whether cell is periodic in each direction. Normally not
necessary. If cell has three nonzero cell vectors, use
e.g. pbc=[1, 1, 0] to request a 2D bandpath nevertheless.
Example
-------
>>> cell = Cell.fromcellpar([4, 4, 4, 60, 60, 60])
>>> cell.bandpath('GXW', npoints=20)
BandPath(path='GXW', cell=[3x3], special_points={GKLUWX}, kpts=[20x3])
"""
# TODO: Combine with the rotation transformation from bandpath()
cell = self if pbc is None else self.uncomplete(pbc)
if special_points is None:
from ase.lattice import identify_lattice
lat, op = identify_lattice(cell, eps=eps)
path = lat.bandpath(path, npoints=npoints, density=density)
return path.transform(op)
else:
from ase.dft.kpoints import BandPath, resolve_custom_points
path = resolve_custom_points(path, special_points, eps=eps)
path = BandPath(cell, path=path, special_points=special_points)
return path.interpolate(npoints=npoints, density=density)
def object_hook(dct):
if '__datetime__' in dct:
return datetime.datetime.strptime(dct['__datetime__'],
'%Y-%m-%dT%H:%M:%S.%f')
if '__complex_ndarray__' in dct:
r, i = (np.array(x) for x in dct['__complex_ndarray__'])
return r + i * 1j
if '__ase_objtype__' in dct:
objtype = dct.pop('__ase_objtype__')
dct = numpyfy(dct)
# We just try each object type one after another and instantiate
# them manually, depending on which kind it is.
# We can formalize this later if it ever becomes necessary.
if objtype == 'cell':
from ase.cell import Cell
obj = Cell(**dct)
elif objtype == 'bandstructure':
from ase.dft.band_structure import BandStructure
obj = BandStructure(**dct)
elif objtype == 'bandpath':
from ase.dft.kpoints import BandPath
obj = BandPath(path=dct.pop('labelseq'), **dct)
else:
raise RuntimeError('Do not know how to decode object type {} '
'into an actual object'.format(objtype))
assert obj.ase_objtype == objtype
return obj
return dct
def create_ase_object(objtype, dct):
# We just try each object type one after another and instantiate
# them manually, depending on which kind it is.
# We can formalize this later if it ever becomes necessary.
if objtype == 'cell':
from ase.cell import Cell
dct.pop('pbc', None) # compatibility; we once had pbc
obj = Cell(**dct)
elif objtype == 'bandstructure':
from ase.spectrum.band_structure import BandStructure
obj = BandStructure(**dct)
elif objtype == 'bandpath':
from ase.dft.kpoints import BandPath
obj = BandPath(path=dct.pop('labelseq'), **dct)
elif objtype == 'atoms':
from ase import Atoms
obj = Atoms.fromdict(dct)
elif objtype == 'densityofstates':
from ase.dft.dos import DOS
obj = DOS(**dct)
elif objtype == 'griddoscollection':
from ase.spectrum.doscollection import GridDOSCollection
obj = GridDOSCollection.fromdict(dct)
else:
raise ValueError('Do not know how to decode object type {} '
'into an actual object'.format(objtype))
assert obj.ase_objtype == objtype
return obj
def bandpath(self,
path=None,
npoints=None,
density=None,
special_points=None,
eps=2e-4):
"""Build a :class:`~ase.dft.kpoints.BandPath` for this cell.
If special points are None, determine the Bravais lattice of
this cell and return a suitable Brillouin zone path with
standard special points.
If special special points are given, interpolate the path
directly from the available data.
Parameters:
path: string
String of special point names defining the path, e.g. 'GXL'.
npoints: int
Number of points in total. Note that at least one point
is added for each special point in the path.
density: float
density of kpoints along the path in Å⁻¹.
special_points: dict
Dictionary mapping special points to scaled kpoint coordinates.
eps: float
Tolerance for determining Bravais lattice.
Example
-------
>>> cell = Cell.fromcellpar([4, 4, 4, 60, 60, 60])
>>> cell.bandpath('GXW', npoints=20)
BandPath(path='GXW', cell=[3x3], special_points={GKLUWX}, kpts=[20x3])
"""
# TODO: Combine with the rotation transformation from bandpath()
if special_points is None:
from ase.lattice import identify_lattice
lat, op = identify_lattice(self, eps=eps)
path = lat.bandpath(path, npoints=npoints, density=density)
return path.transform(op)
else:
from ase.dft.kpoints import BandPath, resolve_custom_points
path = resolve_custom_points(path, special_points, eps=eps)
path = BandPath(self, path=path, special_points=special_points)
return path.interpolate(npoints=npoints, density=density)
def atoms2bandpath(atoms,
path='default',
k_points=False,
ibz_k_points=False,
dimension=3,
verbose=False):
cell = atoms.get_cell()
icell = atoms.get_reciprocal_cell()
try:
cs = crystal_structure_from_cell(cell)
except ValueError:
cs = None
if verbose:
if cs:
print('Crystal:', cs)
print('Special points:', special_paths[cs])
print('Lattice vectors:')
for i, v in enumerate(cell):
print('{}: ({:16.9f},{:16.9f},{:16.9f})'.format(i + 1, *v))
print('Reciprocal vectors:')
for i, v in enumerate(icell):
print('{}: ({:16.9f},{:16.9f},{:16.9f})'.format(i + 1, *v))
# band path
special_points = None
if path:
if path == 'default':
path = special_paths[cs]
paths = []
special_points = get_special_points(cell)
for names in parse_path_string(path):
points = []
for name in names:
points.append(np.dot(icell.T, special_points[name]))
paths.append((names, points))
else:
paths = None
# k points
points = None
if atoms.calc is not None and hasattr(atoms.calc, 'get_bz_k_points'):
bzk = atoms.calc.get_bz_k_points()
if path is None:
try:
size, offset = get_monkhorst_pack_size_and_offset(bzk)
except ValueError:
# This was not a MP-grid. Must be a path in the BZ:
path = ''.join(labels_from_kpts(bzk, cell)[2])
if k_points:
points = bzk
elif ibz_k_points:
points = atoms.calc.get_ibz_k_points()
return BandPath(cell, kpts=points, special_points=special_points)
def atoms2bandstructure(atoms, parser, args):
cell = atoms.get_cell()
calc = atoms.calc
bzkpts = calc.get_bz_k_points()
ibzkpts = calc.get_ibz_k_points()
efermi = calc.get_fermi_level()
nibz = len(ibzkpts)
nspins = 1 + int(calc.get_spin_polarized())
eps = np.array([[calc.get_eigenvalues(kpt=k, spin=s)
for k in range(nibz)]
for s in range(nspins)])
if not args.quiet:
print('Spins, k-points, bands: {}, {}, {}'.format(*eps.shape))
if bzkpts is None:
if ibzkpts is None:
raise ValueError('Cannot find any k-point data')
else:
path_kpts = ibzkpts
else:
try:
size, offset = get_monkhorst_pack_size_and_offset(bzkpts)
except ValueError:
path_kpts = ibzkpts
else:
if not args.quiet:
print('Interpolating from Monkhorst-Pack grid (size, offset):')
print(size, offset)
if args.path is None:
err = 'Please specify a path!'
try:
cs = crystal_structure_from_cell(cell)
except ValueError:
err += ('\nASE cannot automatically '
'recognize this crystal structure')
else:
from ase.dft.kpoints import special_paths
kptpath = special_paths[cs]
err += ('\nIt looks like you have a {} crystal structure.'
'\nMaybe you want its special path:'
' {}'.format(cs, kptpath))
parser.error(err)
bz2ibz = calc.get_bz_to_ibz_map()
path_kpts = bandpath(args.path, atoms.cell, args.points).kpts
icell = atoms.get_reciprocal_cell()
eps = monkhorst_pack_interpolate(path_kpts, eps.transpose(1, 0, 2),
icell, bz2ibz, size, offset)
eps = eps.transpose(1, 0, 2)
special_points = get_special_points(cell)
path = BandPath(atoms.cell, kpts=path_kpts,
special_points=special_points)
return BandStructure(path, eps, reference=efermi)
def test_band_structure_setup(testing_calculator):
c = testing_calculator
from ase.dft.kpoints import BandPath
atoms = ase.build.bulk('Ag')
bp = BandPath(cell=atoms.cell,
path='GX',
special_points={
'G': [0, 0, 0],
'X': [0.5, 0, 0.5]
})
bp = bp.interpolate(npoints=10)
c.set_bandpath(bp)
kpt_list = c.cell.bs_kpoint_list.value.split('\n')
assert len(kpt_list) == 10
assert list(map(float, kpt_list[0].split())) == [0., 0., 0.]
assert list(map(float, kpt_list[-1].split())) == [0.5, 0.0, 0.5]
def read_bands(self):
outputyaml = self.outputdir.joinpath("band.yaml")
assert outputyaml.exists(), "File band.yaml not found."
with open(outputyaml, "r") as stream:
try:
data = yaml.safe_load(stream)
except yaml.YAMLError as exc:
raise Exception(exc)
labels = data["labels"]
bpstring = []
for i, pair in enumerate(labels):
if i == 0:
bpstring.append(pair[0])
elif i == len(labels) - 1:
bpstring.append(pair[0])
bpstring.append(pair[1])
else:
bpstring.append(pair[0])
bpstring = "".join(bpstring)
bpstring = bpstring.replace("|", ",")
bplist = parse_path_string(bpstring)
special_points = (self.structure.cell.get_bravais_lattice().bandpath().
special_points)
self._bandpath = BandPath(path=bpstring,
cell=self.structure.cell,
special_points=special_points)
phon = data["phonon"]
nqpoints = data["segment_nqpoint"]
qpoints = np.array([k["q-position"] for k in phon], dtype=np.float32)
pbands = np.array([[l["frequency"] for l in k["band"]] for k in phon],
dtype=np.float32)
b = namedtuple("band", ["qpoints", "frequencies"])
count = 0
bands = {}
i = 0
for segment in bplist:
for pair in zip(segment[:-1], segment[1:]):
j1, j2 = count, nqpoints[i] + count
count = j2
qp = qpoints[j1:j2, :]
pb = pbands[j1:j2, :]
bands[pair] = b(qp, pb)
rev = (pair[1], pair[0])
bands[rev] = b(qp[::-1], pb[::-1])
i += 1
return bands
def bandpath(self,
path=None,
npoints=None,
special_points=None,
density=None,
transformation=None):
"""Return a :class:`~ase.dft.kpoints.BandPath` for this lattice.
See :meth:`ase.cell.Cell.bandpath` for description of parameters.
>>> BCT(3, 5).bandpath()
BandPath(path='GXYSGZS1NPY1Z,XP', cell=[3x3], \
special_points={GNPSS1XYY1Z}, kpts=[51x3])
.. note:: This produces the standard band path following AFlow
conventions. If your cell does not follow this convention,
you will need :meth:`ase.cell.Cell.bandpath` instead or
the kpoints may not correspond to your particular cell.
"""
if special_points is None:
special_points = self.get_special_points()
if path is None:
path = self._variant.special_path
elif not isinstance(path, str):
from ase.dft.kpoints import resolve_custom_points
special_points = dict(special_points)
path = resolve_custom_points(path, special_points, self._eps)
cell = self.tocell()
if transformation is not None:
cell = transformation.dot(cell)
bandpath = BandPath(cell=cell,
path=path,
special_points=special_points)
return bandpath.interpolate(npoints=npoints, density=density)
def _set_bandpath(self, bandpathstring=None):
if bandpathstring == None:
pbc = [1, 1, 1] if not self.is_2d else [1, 1, 0]
bandpath = self.structure.cell.get_bravais_lattice(
pbc=pbc).bandpath()
self._special_points = bandpath.special_points
bandpathstring = bandpath.path
bp = BandPath(
path=bandpathstring,
cell=self.structure.cell,
special_points=self.special_points,
)
self._bandpath = bp
self._special_points = bp.special_points
def create_ase_object(objtype, dct):
# We just try each object type one after another and instantiate
# them manually, depending on which kind it is.
# We can formalize this later if it ever becomes necessary.
if objtype == 'cell':
from ase.cell import Cell
obj = Cell(**dct)
elif objtype == 'bandstructure':
from ase.dft.band_structure import BandStructure
obj = BandStructure(**dct)
elif objtype == 'bandpath':
from ase.dft.kpoints import BandPath
obj = BandPath(path=dct.pop('labelseq'), **dct)
else:
raise ValueError('Do not know how to decode object type {} '
'into an actual object'.format(objtype))
assert obj.ase_objtype == objtype
return obj
def set_bandpath(self, bandpathstring):
new_bandpath = parse_path_string(bandpathstring)
old_path = self.bandpath
special_points = old_path.special_points
pairs = [(s[0], s[1]) for s in self.bands.keys()]
for segment in new_bandpath:
assert len(segment) > 1, "A vertex needs at least two points."
p = zip(segment[:-1], segment[1:])
for s1, s2 in p:
assert any(x in pairs for x in ((s1, s2), (
s2,
s1))), "The k-path {}-{} has not been calculated.".format(
s1, s2)
else:
new_path = BandPath(
path=bandpathstring,
cell=self.structure.cell,
special_points=special_points,
)
self._bandpath = new_path
def read_bandstructure(self):
if not os.path.isfile(f'{self.label}_band.dat'):
return
# Construct the higher-resolution bandpath from the *_band.labelinfo.dat file
with open(f'{self.label}_band.labelinfo.dat') as fd:
flines = fd.readlines()
kpts = []
self.atoms.cell.pbc = True
for start, end in zip(flines[:-1], flines[1:]):
start_label, i_start = start.split()[:2]
end_label, i_end = end.split()[:2]
kpts += self.atoms.cell.bandpath(start_label + end_label,
int(i_end) - int(i_start) +
1).kpts[:-1].tolist()
kpts.append([float(x) for x in flines[-1].split()[-3:]])
path = self.parameters.kpoint_path.path
special_points = self.parameters.kpoint_path.special_points
kpath = BandPath(self.atoms.cell,
kpts,
path=path,
special_points=special_points)
# Read in the eigenvalues from the *_band.dat file
with open(f'{self.label}_band.dat') as fd:
flines = fd.readlines()
eigs = [[]]
for line in flines[:-1]:
splitline = line.strip().split()
if len(splitline) == 0:
eigs.append([])
else:
eigs[-1].append(line.strip().split()[-1])
eigs = np.array(eigs, dtype=float).T
# Construct the bandstructure
bs = BandStructure(kpath, eigs[np.newaxis, :, :])
self.results['band structure'] = bs
def _set_bandpath_from_sections(self):
sections = self.band_sections
special_points = {k.symbol1: k.k1 for k in sections}
special_points.update({k.symbol2: k.k2 for k in sections})
pathstring = [[k.symbol1, k.symbol2] for k in sections]
rev_string = []
for i, k in enumerate(pathstring):
s1, s2 = k
if i == 0:
rev_string.append(s1)
rev_string.append(s2)
elif s1 == rev_string[-1]:
rev_string.append(s2)
else: # s1 != rev_string[-1]:
rev_string.append(",")
rev_string.append(s1)
rev_string.append(s2)
pathstring = "".join(rev_string)
bp = BandPath(path=pathstring,
cell=self.structure.cell,
special_points=special_points)
self._bandpath = bp
def get_band_structure(atoms=None, calc=None, _bandpath=None, _reference=None):
"""Create band structure object from Atoms or calculator."""
# _bandpath and _reference are used internally at the moment, but
# the exact implementation will probably change. WIP.
#
# XXX We throw away info about the bandpath when we create the calculator.
# If we have kept the bandpath, we can provide it as an argument here.
# It would be wise to check that the bandpath kpoints are the same as
# those stored in the calculator.
atoms = atoms if atoms is not None else calc.atoms
calc = calc if calc is not None else atoms.calc
kpts = calc.get_ibz_k_points()
energies = []
for s in range(calc.get_number_of_spins()):
energies.append(
[calc.get_eigenvalues(kpt=k, spin=s) for k in range(len(kpts))])
energies = np.array(energies)
if _bandpath is None:
from ase.dft.kpoints import BandPath, get_cellinfo, labels_from_kpts
cellinfo = get_cellinfo(cell=atoms.cell)
special_points = cellinfo.special_points
_, _, labels = labels_from_kpts(kpts,
cell=atoms.cell,
special_points=special_points)
_bandpath = BandPath(labelseq=labels,
cell=atoms.cell,
scaled_kpts=kpts,
special_points=special_points)
if _reference is None:
# Fermi level should come from the GS calculation, not the BS one!
_reference = calc.get_fermi_level()
return BandStructure(path=_bandpath,
energies=energies,
reference=_reference)
def construct_kpoint_path(path: str, cell: Cell, bands_point_num: int) -> BandPath:
path_lengths = _path_lengths(path, cell, bands_point_num)
special_points = cell.bandpath().special_points
path_list = path_str_to_list(path, special_points)
kpts = []
for start, end, npoints in zip(path_list[:-1], path_list[1:], path_lengths):
if start == ',':
pass
elif end == ',':
kpts.append(special_points[start].tolist())
else:
bp = bandpath(start + end, cell, npoints + 1)
kpts += bp.kpts[:-1].tolist()
# Don't forget about the final kpoint
kpts.append(bp.kpts[-1].tolist())
if len(kpts) != sum(path_lengths) + 1:
raise AssertionError(
'Did not get the expected number of kpoints; this suggests there is a bug in the code')
return BandPath(cell=cell, kpts=kpts, path=path, special_points=special_points)
def test_castep_interface():
"""Simple shallow test of the CASTEP interface"""
import os
import re
import tempfile
import warnings
import numpy as np
import ase
import ase.lattice.cubic
from ase.calculators.castep import (Castep, CastepOption, CastepParam,
CastepCell, make_cell_dict,
make_param_dict, CastepKeywords,
create_castep_keywords,
import_castep_keywords,
CastepVersionError)
# XXX on porting this test to pytest it wasn't skipped as it should be.
# At any rate it failed then. Maybe someone should look into that ...
#
# Hence, call the constructor to trigger our test skipping hack:
Castep()
tmp_dir = tempfile.mkdtemp()
# We have fundamentally two sets of tests: one if CASTEP is present, the other
# if it isn't
has_castep = False
# Try creating and importing the castep keywords first
try:
create_castep_keywords(castep_command=os.environ['CASTEP_COMMAND'],
path=tmp_dir,
fetch_only=20)
has_castep = True # If it worked, it must be present
except KeyError:
print('Could not find the CASTEP_COMMAND environment variable - please'
' set it to run the full set of Castep tests')
except CastepVersionError:
print(
'Invalid CASTEP_COMMAND provided - please set the correct one to '
'run the full set of Castep tests')
try:
castep_keywords = import_castep_keywords(
castep_command=os.environ.get('CASTEP_COMMAND', ''))
except CastepVersionError:
castep_keywords = None
# Start by testing the fundamental parts of a CastepCell/CastepParam object
boolOpt = CastepOption('test_bool', 'basic', 'defined')
boolOpt.value = 'TRUE'
assert boolOpt.raw_value is True
float3Opt = CastepOption('test_float3', 'basic', 'real vector')
float3Opt.value = '1.0 2.0 3.0'
assert np.isclose(float3Opt.raw_value, [1, 2, 3]).all()
# Generate a mock keywords object
mock_castep_keywords = CastepKeywords(make_param_dict(), make_cell_dict(),
[], [], 0)
mock_cparam = CastepParam(mock_castep_keywords, keyword_tolerance=2)
mock_ccell = CastepCell(mock_castep_keywords, keyword_tolerance=2)
# Test special parsers
mock_cparam.continuation = 'default'
mock_cparam.reuse = 'default'
assert mock_cparam.reuse.value is None
mock_ccell.species_pot = ('Si', 'Si.usp')
mock_ccell.species_pot = ('C', 'C.usp')
assert 'Si Si.usp' in mock_ccell.species_pot.value
assert 'C C.usp' in mock_ccell.species_pot.value
symops = (np.eye(3)[None], np.zeros(3)[None])
mock_ccell.symmetry_ops = symops
assert """1.0 0.0 0.0
0.0 1.0 0.0
0.0 0.0 1.0
0.0 0.0 0.0""" in mock_ccell.symmetry_ops.value
# check if the CastepOpt, CastepCell comparison mechanism works
if castep_keywords:
p1 = CastepParam(castep_keywords)
p2 = CastepParam(castep_keywords)
assert p1._options == p2._options
p1._options['xc_functional'].value = 'PBE'
p1.xc_functional = 'PBE'
assert p1._options != p2._options
c = Castep(directory=tmp_dir, label='test_label', keyword_tolerance=2)
if castep_keywords:
c.xc_functional = 'PBE'
else:
c.param.xc_functional = 'PBE' # In "forgiving" mode, we need to specify
lattice = ase.lattice.cubic.BodyCenteredCubic('Li')
print('For the sake of evaluating this test, warnings')
print('about auto-generating pseudo-potentials are')
print('normal behavior and can be safely ignored')
lattice.calc = c
param_fn = os.path.join(tmp_dir, 'myParam.param')
with open(param_fn, 'w') as param:
param.write('XC_FUNCTIONAL : PBE #comment\n')
param.write('XC_FUNCTIONAL : PBE #comment\n')
param.write('#comment\n')
param.write('CUT_OFF_ENERGY : 450.\n')
c.merge_param(param_fn)
assert c.calculation_required(lattice)
if has_castep:
assert c.dryrun_ok()
c.prepare_input_files(lattice)
# detecting pseudopotentials tests
# typical filenames
files = [
'Ag_00PBE.usp', 'Ag_00.recpot', 'Ag_C18_PBE_OTF.usp',
'ag-optgga1.recpot', 'Ag_OTF.usp', 'ag_pbe_v1.4.uspp.F.UPF',
'Ni_OTF.usp', 'fe_pbe_v1.5.uspp.F.UPF', 'Cu_01.recpot'
]
pp_path = os.path.join(tmp_dir, 'test_pp')
os.makedirs(pp_path)
for f in files:
with open(os.path.join(pp_path, f), 'w') as _f:
_f.write('DUMMY PP')
c = Castep(directory=tmp_dir,
label='test_label_pspots',
castep_pp_path=pp_path)
c._pedantic = True
atoms = ase.build.bulk('Ag')
atoms.calc = c
# I know, unittest would be nicer... maybe at a later point
# disabled, but may be useful still
# try:
# # this should yield no files
# atoms.calc.find_pspots(suffix='uspp')
# raise AssertionError
# # this should yield no files
# atoms.calc.find_pspots(suffix='uspp')
# raise AssertionError
# except RuntimeError as e:
# #print(e)
# pass
# # print(e)
# pass
try:
# this should yield non-unique files
atoms.calc.find_pspots(suffix='recpot')
raise AssertionError
except RuntimeError:
pass
# now let's see if we find all...
atoms.calc.find_pspots(pspot='00PBE', suffix='usp')
assert atoms.calc.cell.species_pot.value.split()[-1] == 'Ag_00PBE.usp'
atoms.calc.find_pspots(pspot='00', suffix='recpot')
assert atoms.calc.cell.species_pot.value.split()[-1] == 'Ag_00.recpot'
atoms.calc.find_pspots(pspot='C18_PBE_OTF', suffix='usp')
assert atoms.calc.cell.species_pot.value.split(
)[-1] == 'Ag_C18_PBE_OTF.usp'
atoms.calc.find_pspots(pspot='optgga1', suffix='recpot')
assert atoms.calc.cell.species_pot.value.split()[-1] == 'ag-optgga1.recpot'
atoms.calc.find_pspots(pspot='OTF', suffix='usp')
assert atoms.calc.cell.species_pot.value.split()[-1] == 'Ag_OTF.usp'
atoms.calc.find_pspots(suffix='UPF')
assert (atoms.calc.cell.species_pot.value.split()[-1] ==
'ag_pbe_v1.4.uspp.F.UPF')
# testing regular workflow
c = Castep(directory=tmp_dir,
label='test_label_pspots',
castep_pp_path=pp_path,
find_pspots=True,
keyword_tolerance=2)
c._build_missing_pspots = False
atoms = ase.build.bulk('Ag')
atoms.calc = c
# this should raise an error due to ambuiguity
try:
c._fetch_pspots()
raise AssertionError
except RuntimeError:
pass
for e in ['Ni', 'Fe', 'Cu']:
atoms = ase.build.bulk(e)
atoms.calc = c
c._fetch_pspots()
# test writing to file
tmp_dir = os.path.join(tmp_dir, 'input_files')
c = Castep(directory=tmp_dir,
find_pspots=True,
castep_pp_path=pp_path,
keyword_tolerance=2)
c._label = 'test'
atoms = ase.build.bulk('Cu')
atoms.calc = c
c.prepare_input_files()
with open(os.path.join(tmp_dir, 'test.cell'), 'r') as f:
assert re.search(r'Cu Cu_01\.recpot',
''.join(f.readlines())) is not None
# test keyword conflict management
c = Castep(cut_off_energy=300.)
assert float(c.param.cut_off_energy.value) == 300.0
with warnings.catch_warnings(record=True) as w:
warnings.simplefilter("always")
c.basis_precision = 'MEDIUM'
assert issubclass(w[-1].category, UserWarning)
assert "conflicts" in str(w[-1].message)
assert c.param.cut_off_energy.value is None
assert c.param.basis_precision.value.strip() == 'MEDIUM'
with warnings.catch_warnings(record=True) as w:
warnings.simplefilter("always")
c.cut_off_energy = 200.0
assert c.param.basis_precision.value is None
assert issubclass(w[-1].category, UserWarning)
assert 'option "cut_off_energy" conflicts' in str(w[-1].message)
# test kpoint setup options
with warnings.catch_warnings():
warnings.simplefilter("ignore")
# This block of tests is going to generate a lot of conflict warnings.
# We already tested that those work, so just hide them from the output.
c = Castep(kpts=[
(0.0, 0.0, 0.0, 1.0),
])
assert c.cell.kpoint_list.value == '0.0 0.0 0.0 1.0'
c.set_kpts(((0.0, 0.0, 0.0, 0.25), (0.25, 0.25, 0.3, 0.75)))
assert c.cell.kpoint_list.value == '0.0 0.0 0.0 0.25\n0.25 0.25 0.3 0.75'
c.set_kpts(c.cell.kpoint_list.value.split('\n'))
assert c.cell.kpoint_list.value == '0.0 0.0 0.0 0.25\n0.25 0.25 0.3 0.75'
c.set_kpts([3, 3, 2])
assert c.cell.kpoint_mp_grid.value == '3 3 2'
c.set_kpts(None)
assert c.cell.kpoints_list.value is None
assert c.cell.kpoint_list.value is None
assert c.cell.kpoint_mp_grid.value is None
c.set_kpts('2 2 3')
assert c.cell.kpoint_mp_grid.value == '2 2 3'
c.set_kpts({'even': True, 'gamma': True})
assert c.cell.kpoint_mp_grid.value == '2 2 2'
assert c.cell.kpoint_mp_offset.value == '0.25 0.25 0.25'
c.set_kpts({'size': (2, 2, 4), 'even': False})
assert c.cell.kpoint_mp_grid.value == '3 3 5'
assert c.cell.kpoint_mp_offset.value == '0.0 0.0 0.0'
atoms = ase.build.bulk('Ag')
atoms.calc = c
c.set_kpts({'density': 10, 'gamma': False, 'even': None})
assert c.cell.kpoint_mp_grid.value == '27 27 27'
assert c.cell.kpoint_mp_offset.value == '0.018519 0.018519 0.018519'
c.set_kpts({
'spacing': (1 / (np.pi * 10)),
'gamma': False,
'even': True
})
assert c.cell.kpoint_mp_grid.value == '28 28 28'
assert c.cell.kpoint_mp_offset.value == '0.0 0.0 0.0'
# test band structure setup
from ase.dft.kpoints import BandPath
atoms = ase.build.bulk('Ag')
bp = BandPath(cell=atoms.cell,
path='GX',
special_points={
'G': [0, 0, 0],
'X': [0.5, 0, 0.5]
})
bp = bp.interpolate(npoints=10)
c = Castep(bandpath=bp)
kpt_list = c.cell.bs_kpoint_list.value.split('\n')
assert len(kpt_list) == 10
assert list(map(float, kpt_list[0].split())) == [0., 0., 0.]
assert list(map(float, kpt_list[-1].split())) == [0.5, 0.0, 0.5]
assert c.cell.kpoint_mp_grid.value == '2 2 2'
assert c.cell.kpoint_mp_offset.value == '0.25 0.25 0.25'
c.set_kpts({'size': (2, 2, 4), 'even': False})
assert c.cell.kpoint_mp_grid.value == '3 3 5'
assert c.cell.kpoint_mp_offset.value == '0.0 0.0 0.0'
atoms = ase.build.bulk('Ag')
atoms.set_calculator(c)
c.set_kpts({'density': 10, 'gamma': False, 'even': None})
assert c.cell.kpoint_mp_grid.value == '27 27 27'
assert c.cell.kpoint_mp_offset.value == '0.018519 0.018519 0.018519'
c.set_kpts({'spacing': (1 / (np.pi *10)), 'gamma': False, 'even': True})
assert c.cell.kpoint_mp_grid.value == '28 28 28'
assert c.cell.kpoint_mp_offset.value == '0.0 0.0 0.0'
# test band structure setup
from ase.dft.kpoints import BandPath
atoms = ase.build.bulk('Ag')
bp = BandPath(cell=atoms.cell,
path='GX',
special_points={'G': [0, 0, 0], 'X': [0.5, 0, 0.5]})
bp = bp.interpolate(npoints=10)
c = Castep(bandpath=bp)
kpt_list = c.cell.bs_kpoint_list.value.split('\n')
assert len(kpt_list) == 10
assert list(map(float, kpt_list[0].split())) == [0., 0., 0.]
assert list(map(float, kpt_list[-1].split())) == [0.5, 0.0, 0.5]
# cleanup
os.chdir(cwd)
shutil.rmtree(tmp_dir)
def get_band_structure(atoms=None, calc=None, path=None, reference=None):
"""Create band structure object from Atoms or calculator."""
# path and reference are used internally at the moment, but
# the exact implementation will probably change. WIP.
#
# XXX We throw away info about the bandpath when we create the calculator.
# If we have kept the bandpath, we can provide it as an argument here.
# It would be wise to check that the bandpath kpoints are the same as
# those stored in the calculator.
atoms = atoms if atoms is not None else calc.atoms
calc = calc if calc is not None else atoms.calc
kpts = calc.get_ibz_k_points()
energies = []
for s in range(calc.get_number_of_spins()):
energies.append(
[calc.get_eigenvalues(kpt=k, spin=s) for k in range(len(kpts))])
energies = np.array(energies)
if path is None:
from ase.dft.kpoints import (BandPath, resolve_custom_points,
find_bandpath_kinks)
standard_path = atoms.cell.bandpath(npoints=0)
# Kpoints are already evaluated, we just need to put them into
# the path (whether they fit our idea of what the path is, or not).
#
# Depending on how the path was established, the kpoints might
# be valid high-symmetry points, but since there are multiple
# high-symmetry points of each type, they may not coincide
# with ours if the bandpath was generated by another code.
#
# Here we hack it so the BandPath has proper points even if they
# come from some weird source.
#
# This operation (manually hacking the bandpath) is liable to break.
# TODO: Make it available as a proper (documented) bandpath method.
kinks = find_bandpath_kinks(atoms.cell, kpts, eps=1e-5)
pathspec, special_points = resolve_custom_points(
kpts[kinks], standard_path.special_points, eps=1e-5)
path = BandPath(standard_path.cell,
kpts=kpts,
path=pathspec,
special_points=special_points)
# XXX If we *did* get the path, now would be a good time to check
# that it matches the cell! Although the path can only be passed
# because we internally want to not re-evaluate the Bravais
# lattice type. (We actually need an eps parameter, too.)
if reference is None:
# Fermi level should come from the GS calculation, not the BS one!
reference = calc.get_fermi_level()
if reference is None:
# Fermi level may not be available, e.g., with non-Fermi smearing.
# XXX Actually get_fermi_level() should raise an error when Fermi
# level wasn't available, so we should fix that.
reference = 0.0
return BandStructure(path=path, energies=energies, reference=reference)