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"""
This module contains functionality for reading and writing an ASE
Atoms object in VASP POSCAR format.
"""
import os
def get_atomtypes(fname):
"""Given a file name, get the atomic symbols.
The function can get this information from OUTCAR and POTCAR
format files. The files can also be compressed with gzip or
bzip2.
"""
atomtypes = []
if fname.find('.gz') != -1:
import gzip
f = gzip.open(fname)
elif fname.find('.bz2') != -1:
import bz2
f = bz2.BZ2File(fname)
else:
f = open(fname)
for line in f:
if line.find('TITEL') != -1:
atomtypes.append(line.split()[3].split('_')[0].split('.')[0])
return atomtypes
def atomtypes_outpot(posfname, numsyms):
"""Try to retrieve chemical symbols from OUTCAR or POTCAR
If getting atomtypes from the first line in POSCAR/CONTCAR fails, it might
be possible to find the data in OUTCAR or POTCAR, if these files exist.
posfname -- The filename of the POSCAR/CONTCAR file we're trying to read
numsyms -- The number of symbols we must find
"""
import os.path as op
import glob
# First check files with exactly same name except POTCAR/OUTCAR instead
# of POSCAR/CONTCAR.
fnames = [posfname.replace('POSCAR', 'POTCAR').replace('CONTCAR',
'POTCAR')]
fnames.append(posfname.replace('POSCAR', 'OUTCAR').replace('CONTCAR',
'OUTCAR'))
# Try the same but with compressed files
fsc = []
for fn in fnames:
fsc.append(fn + '.gz')
fsc.append(fn + '.bz2')
for f in fsc:
fnames.append(f)
# Finally try anything with POTCAR or OUTCAR in the name
vaspdir = op.dirname(posfname)
fs = glob.glob(vaspdir + '*POTCAR*')
for f in fs:
fnames.append(f)
fs = glob.glob(vaspdir + '*OUTCAR*')
for f in fs:
fnames.append(f)
tried = []
files_in_dir = os.listdir('.')
for fn in fnames:
if fn in files_in_dir:
tried.append(fn)
at = get_atomtypes(fn)
if len(at) == numsyms:
return at
raise IOError('Could not determine chemical symbols. Tried files ' +
str(tried))
def get_atomtypes_from_formula(formula):
"""Return atom types from chemical formula (optionally prepended
with and underscore).
"""
from ase.atoms import string2symbols
symbols = string2symbols(formula.split('_')[0])
atomtypes = [symbols[0]]
for s in symbols[1:]:
if s != atomtypes[-1]:
atomtypes.append(s)
return atomtypes
def read_vasp(filename='CONTCAR'):
"""Import POSCAR/CONTCAR type file.
Reads unitcell, atom positions and constraints from the POSCAR/CONTCAR
file and tries to read atom types from POSCAR/CONTCAR header, if this fails
the atom types are read from OUTCAR or POTCAR file.
"""
from ase import Atoms
from ase.constraints import FixAtoms, FixScaled
from ase.data import chemical_symbols
import numpy as np
if isinstance(filename, str):
f = open(filename)
else: # Assume it's a file-like object
f = filename
# The first line is in principle a comment line, however in VASP
# 4.x a common convention is to have it contain the atom symbols,
# eg. "Ag Ge" in the same order as later in the file (and POTCAR
# for the full vasp run). In the VASP 5.x format this information
# is found on the fifth line. Thus we save the first line and use
# it in case we later detect that we're reading a VASP 4.x format
# file.
line1 = f.readline()
lattice_constant = float(f.readline().split()[0])
# Now the lattice vectors
a = []
for ii in range(3):
s = f.readline().split()
floatvect = float(s[0]), float(s[1]), float(s[2])
a.append(floatvect)
basis_vectors = np.array(a) * lattice_constant
# Number of atoms. Again this must be in the same order as
# in the first line
# or in the POTCAR or OUTCAR file
atom_symbols = []
numofatoms = f.readline().split()
# Check whether we have a VASP 4.x or 5.x format file. If the
# format is 5.x, use the fifth line to provide information about
# the atomic symbols.
vasp5 = False
try:
int(numofatoms[0])
except ValueError:
vasp5 = True
atomtypes = numofatoms
numofatoms = f.readline().split()
# check for comments in numofatoms line and get rid of them if necessary
commentcheck = np.array(['!' in s for s in numofatoms])
if commentcheck.any():
# only keep the elements up to the first including a '!':
numofatoms = numofatoms[:np.arange(len(numofatoms))[commentcheck][0]]
if not vasp5:
atomtypes = line1.split()
numsyms = len(numofatoms)
if len(atomtypes) < numsyms:
# First line in POSCAR/CONTCAR didn't contain enough symbols.
# Sometimes the first line in POSCAR/CONTCAR is of the form
# "CoP3_In-3.pos". Check for this case and extract atom types
if len(atomtypes) == 1 and '_' in atomtypes[0]:
atomtypes = get_atomtypes_from_formula(atomtypes[0])
else:
atomtypes = atomtypes_outpot(f.name, numsyms)
else:
try:
for atype in atomtypes[:numsyms]:
if atype not in chemical_symbols:
raise KeyError
except KeyError:
atomtypes = atomtypes_outpot(f.name, numsyms)
for i, num in enumerate(numofatoms):
numofatoms[i] = int(num)
[atom_symbols.append(atomtypes[i]) for na in range(numofatoms[i])]
# Check if Selective dynamics is switched on
sdyn = f.readline()
selective_dynamics = sdyn[0].lower() == 's'
# Check if atom coordinates are cartesian or direct
if selective_dynamics:
ac_type = f.readline()
else:
ac_type = sdyn
cartesian = ac_type[0].lower() == 'c' or ac_type[0].lower() == 'k'
tot_natoms = sum(numofatoms)
atoms_pos = np.empty((tot_natoms, 3))
if selective_dynamics:
selective_flags = np.empty((tot_natoms, 3), dtype=bool)
for atom in range(tot_natoms):
ac = f.readline().split()
atoms_pos[atom] = (float(ac[0]), float(ac[1]), float(ac[2]))
if selective_dynamics:
curflag = []
for flag in ac[3:6]:
curflag.append(flag == 'F')
selective_flags[atom] = curflag
# Done with all reading
if isinstance(filename, str):
f.close()
if cartesian:
atoms_pos *= lattice_constant
atoms = Atoms(symbols=atom_symbols, cell=basis_vectors, pbc=True)
if cartesian:
atoms.set_positions(atoms_pos)
else:
atoms.set_scaled_positions(atoms_pos)
if selective_dynamics:
constraints = []
indices = []
for ind, sflags in enumerate(selective_flags):
if sflags.any() and not sflags.all():
constraints.append(FixScaled(atoms.get_cell(), ind, sflags))
elif sflags.all():
indices.append(ind)
if indices:
constraints.append(FixAtoms(indices))
if constraints:
atoms.set_constraint(constraints)
return atoms
def read_vasp_out(filename='OUTCAR', index=-1, force_consistent=False):
"""Import OUTCAR type file.
Reads unitcell, atom positions, energies, and forces from the OUTCAR file
and attempts to read constraints (if any) from CONTCAR/POSCAR, if present.
"""
import numpy as np
from ase.calculators.singlepoint import SinglePointCalculator
from ase import Atoms, Atom
try: # try to read constraints, first from CONTCAR, then from POSCAR
constr = read_vasp('CONTCAR').constraints
except Exception:
try:
constr = read_vasp('POSCAR').constraints
except Exception:
constr = None
if isinstance(filename, str):
f = open(filename)
else: # Assume it's a file-like object
f = filename
data = f.readlines()
natoms = 0
images = []
atoms = Atoms(pbc=True, constraint=constr)
energy = 0
species = []
species_num = []
symbols = []
ecount = 0
poscount = 0
magnetization = []
for n, line in enumerate(data):
if 'POTCAR:' in line:
temp = line.split()[2]
for c in ['.', '_', '1']:
if c in temp:
temp = temp[0:temp.find(c)]
species += [temp]
if 'ions per type' in line:
species = species[:len(species) // 2]
temp = line.split()
for ispecies in range(len(species)):
species_num += [int(temp[ispecies + 4])]
natoms += species_num[-1]
for iatom in range(species_num[-1]):
symbols += [species[ispecies]]
if 'direct lattice vectors' in line:
cell = []
for i in range(3):
temp = data[n + 1 + i].split()
cell += [[float(temp[0]), float(temp[1]), float(temp[2])]]
atoms.set_cell(cell)
if 'FREE ENERGIE OF THE ION-ELECTRON SYSTEM' in line:
# choose between energy wigh smearing extrapolated to zero
# or free energy (latter is consistent with forces)
energy_zero = float(data[n + 4].split()[6])
energy_free = float(data[n + 2].split()[4])
energy = energy_zero
if force_consistent:
energy = energy_free
if ecount < poscount:
# reset energy for LAST set of atoms, not current one -
# VASP 5.11? and up
images[-1].calc.results['energy'] = energy
images[-1].calc.set(energy=energy)
ecount += 1
if 'magnetization (x)' in line:
magnetization = []
for i in range(natoms):
magnetization += [float(data[n + 4 + i].split()[4])]
if 'POSITION ' in line:
forces = []
positions = []
for iatom in range(natoms):
temp = data[n + 2 + iatom].split()
atoms += Atom(symbols[iatom],
[float(temp[0]), float(temp[1]), float(temp[2])])
forces += [[float(temp[3]), float(temp[4]), float(temp[5])]]
positions += [[float(temp[0]), float(temp[1]), float(temp[2])]]
atoms.set_calculator(SinglePointCalculator(atoms,
energy=energy,
forces=forces))
images += [atoms]
if len(magnetization) > 0:
images[-1].calc.magmoms = np.array(magnetization, float)
atoms = Atoms(pbc=True, constraint=constr)
poscount += 1
# return requested images, code borrowed from ase/io/trajectory.py
if isinstance(index, int):
return images[index]
else:
step = index.step or 1
if step > 0:
start = index.start or 0
if start < 0:
start += len(images)
stop = index.stop or len(images)
if stop < 0:
stop += len(images)
else:
if index.start is None:
start = len(images) - 1
else:
start = index.start
if start < 0:
start += len(images)
if index.stop is None:
stop = -1
else:
stop = index.stop
if stop < 0:
stop += len(images)
return [images[i] for i in range(start, stop, step)]
def read_vasp_xdatcar(filename, index=-1):
"""Import XDATCAR file
Reads all positions from the XDATCAR and returns a list of
Atoms objects. Useful for viewing optimizations runs
from VASP5.x
Constraints ARE NOT stored in the XDATCAR, and as such, Atoms
objects retrieved from the XDATCAR will not have constraints set.
"""
import numpy as np
from ase import Atoms
images = list()
cell = np.eye(3)
atomic_formula = str()
with open(filename, 'r') as xdatcar:
while True:
comment_line = xdatcar.readline()
if "Direct configuration=" not in comment_line:
try:
lattice_constant = float(xdatcar.readline())
except:
break
xx = [float(x) for x in xdatcar.readline().split()]
yy = [float(y) for y in xdatcar.readline().split()]
zz = [float(z) for z in xdatcar.readline().split()]
cell = np.array([xx, yy, zz]) * lattice_constant
symbols = xdatcar.readline().split()
numbers = [int(n) for n in xdatcar.readline().split()]
total = sum(numbers)
atomic_formula = str()
for n, sym in enumerate(symbols):
atomic_formula += '%s%s' % (sym, numbers[n])
xdatcar.readline()
coords = [np.array(xdatcar.readline().split(), np.float)
for ii in range(total)]
image = Atoms(atomic_formula, cell=cell, pbc=True)
image.set_scaled_positions(np.array(coords))
images.append(image)
if not index:
return images
else:
return images[index]
def __get_xml_parameter(par):
"""An auxillary function that enables convenient extraction of
parameter values from a vasprun.xml file with proper type
handling.
"""
def to_bool(b):
if b == 'T':
return True
else:
return False
to_type = {'int': int,
'logical': to_bool,
'string': str,
'float': float}
text = par.text
if text is None:
text = ''
# Float parameters do not have a 'type' attrib
var_type = to_type[par.attrib.get('type', 'float')]
if par.tag == 'v':
return map(var_type, text.split())
else:
return var_type(text.strip())
def read_vasp_xml(filename='vasprun.xml', index=-1):
"""Parse vasprun.xml file.
Reads unit cell, atom positions, energies, forces, and constraints
from vasprun.xml file
"""
import numpy as np
import xml.etree.ElementTree as ET
from ase import Atoms
from ase.constraints import FixAtoms, FixScaled
from ase.calculators.singlepoint import (SinglePointDFTCalculator,
SinglePointKPoint)
from ase.units import GPa
from collections import OrderedDict
tree = ET.iterparse(filename, events=['start', 'end'])
atoms_init = None
calculation = []
ibz_kpts = None
parameters = OrderedDict()
try:
for event, elem in tree:
if event == 'end':
if elem.tag == 'kpoints':
for subelem in elem.iter(tag='generation'):
kpts_params = OrderedDict()
parameters['kpoints_generation'] = kpts_params
for par in subelem.iter():
if par.tag in ['v', 'i']:
parname = par.attrib['name'].lower()
kpts_params[parname] = __get_xml_parameter(par)
kpts = elem.findall("varray[@name='kpointlist']/v")
ibz_kpts = np.zeros((len(kpts), 3))
for i, kpt in enumerate(kpts):
ibz_kpts[i] = [float(val) for val in kpt.text.split()]
elif elem.tag == 'parameters':
for par in elem.iter():
if par.tag in ['v', 'i']:
parname = par.attrib['name'].lower()
parameters[parname] = __get_xml_parameter(par)
elif elem.tag == 'atominfo':
species = []
for entry in elem.find("array[@name='atoms']/set"):
species.append(entry[0].text.strip())
natoms = len(species)
elif (elem.tag == 'structure' and
elem.attrib.get('name') == 'initialpos'):
cell_init = np.zeros((3, 3), dtype=float)
for i, v in enumerate(elem.find(
"crystal/varray[@name='basis']")):
cell_init[i] = np.array([
float(val) for val in v.text.split()])
scpos_init = np.zeros((natoms, 3), dtype=float)
for i, v in enumerate(elem.find(
"varray[@name='positions']")):
scpos_init[i] = np.array([
float(val) for val in v.text.split()])
constraints = []
fixed_indices = []
for i, entry in enumerate(elem.findall(
"varray[@name='selective']/v")):
flags = (np.array(entry.text.split() ==
np.array(['F', 'F', 'F'])))
if flags.all():
fixed_indices.append(i)
elif flags.any():
constraints.append(FixScaled(cell_init, i, flags))
if fixed_indices:
constraints.append(FixAtoms(fixed_indices))
atoms_init = Atoms(species,
cell=cell_init,
scaled_positions=scpos_init,
constraint=constraints,
pbc=True)
elif event == 'start' and elem.tag == 'calculation':
calculation.append(elem)
except ET.ParseError as parse_error:
if atoms_init is None:
raise parse_error
if calculation[-1].find('energy') is None:
calculation = calculation[:-1]
if not calculation:
yield atoms_init
if calculation:
if isinstance(index, int):
steps = [calculation[index]]
else:
steps = calculation[index]
else:
steps = []
for step in steps:
# Workaround for VASP bug, e_0_energy contains the wrong value
# in calculation/energy, but calculation/scstep/energy does not
# include classical VDW corrections. So, first calculate
# e_0_energy - e_fr_energy from calculation/scstep/energy, then
# apply that correction to e_fr_energy from calculation/energy.
lastscf = step.findall('scstep/energy')[-1]
de = (float(lastscf.find('i[@name="e_0_energy"]').text) -
float(lastscf.find('i[@name="e_fr_energy"]').text))
free_energy = float(step.find('energy/i[@name="e_fr_energy"]').text)
energy = free_energy + de
cell = np.zeros((3, 3), dtype=float)
for i, vector in enumerate(step.find(
'structure/crystal/varray[@name="basis"]')):
cell[i] = np.array([float(val) for val in vector.text.split()])
scpos = np.zeros((natoms, 3), dtype=float)
for i, vector in enumerate(step.find(
'structure/varray[@name="positions"]')):
scpos[i] = np.array([float(val) for val in vector.text.split()])
forces = None
fblocks = step.find('varray[@name="forces"]')
if fblocks is not None:
forces = np.zeros((natoms, 3), dtype=float)
for i, vector in enumerate(fblocks):
forces[i] = np.array([float(val)
for val in vector.text.split()])
stress = None
sblocks = step.find('varray[@name="stress"]')
if sblocks is not None:
stress = np.zeros((3, 3), dtype=float)
for i, vector in enumerate(sblocks):
stress[i] = np.array([float(val)
for val in vector.text.split()])
stress *= -0.1 * GPa
stress = stress.reshape(9)[[0, 4, 8, 5, 2, 1]]
efermi = step.find('dos/i[@name="efermi"]')
if efermi is not None:
efermi = float(efermi.text)
kpoints = []
for ikpt in range(1, len(ibz_kpts) + 1):
kblocks = step.findall(
'eigenvalues/array/set/set/set[@comment="kpoint %d"]' % ikpt)
if kblocks is not None:
for i, kpoint in enumerate(kblocks):
eigenvals = kpoint.findall('r')
eps_n = np.zeros(len(eigenvals))
f_n = np.zeros(len(eigenvals))
for j, val in enumerate(eigenvals):
val = val.text.split()
eps_n[j] = float(val[0])
f_n[j] = float(val[1])
if len(kblocks) == 1:
f_n *= 2
kpoints.append(SinglePointKPoint(1, 0, ikpt, eps_n, f_n))
if len(kpoints) == 0:
kpoints = None
atoms = atoms_init.copy()
atoms.set_cell(cell)
atoms.set_scaled_positions(scpos)
atoms.set_calculator(
SinglePointDFTCalculator(atoms, energy=energy, forces=forces,
stress=stress, free_energy=free_energy,
ibz_kpts=ibz_kpts, eFermi=efermi))
atoms.calc.name = 'vasp'
atoms.calc.kpts = kpoints
atoms.calc.parameters = parameters
yield atoms
def write_vasp(filename, atoms, label='', direct=False, sort=None,
symbol_count=None, long_format=True, vasp5=False):
"""Method to write VASP position (POSCAR/CONTCAR) files.
Writes label, scalefactor, unitcell, # of various kinds of atoms,
positions in cartesian or scaled coordinates (Direct), and constraints
to file. Cartesian coordiantes is default and default label is the
atomic species, e.g. 'C N H Cu'.
"""
import numpy as np
from ase.constraints import FixAtoms, FixScaled, FixedPlane, FixedLine
if isinstance(filename, str):
f = open(filename, 'w')
else: # Assume it's a 'file-like object'
f = filename
if isinstance(atoms, (list, tuple)):
if len(atoms) > 1:
raise RuntimeError('Don\'t know how to save more than ' +
'one image to VASP input')
else:
atoms = atoms[0]
# Write atom positions in scaled or cartesian coordinates
if direct:
coord = atoms.get_scaled_positions()
else:
coord = atoms.get_positions()
if atoms.constraints:
sflags = np.zeros((len(atoms), 3), dtype=bool)
for constr in atoms.constraints:
if isinstance(constr, FixScaled):
sflags[constr.a] = constr.mask
elif isinstance(constr, FixAtoms):
sflags[constr.index] = [True, True, True]
elif isinstance(constr, FixedPlane):
mask = np.all(np.abs(np.cross(constr.dir, atoms.cell)) < 1e-5,
axis=1)
if sum(mask) != 1:
raise RuntimeError(
'VASP requires that the direction of FixedPlane '
'constraints is parallel with one of the cell axis')
sflags[constr.a] = mask
elif isinstance(constr, FixedLine):
mask = np.all(np.abs(np.cross(constr.dir, atoms.cell)) < 1e-5,
axis=1)
if sum(mask) != 1:
raise RuntimeError(
'VASP requires that the direction of FixedLine '
'constraints is parallel with one of the cell axis')
sflags[constr.a] = ~mask
if sort:
ind = np.argsort(atoms.get_chemical_symbols())
symbols = np.array(atoms.get_chemical_symbols())[ind]
coord = coord[ind]
if atoms.constraints:
sflags = sflags[ind]
else:
symbols = atoms.get_chemical_symbols()
# Create a list sc of (symbol, count) pairs
if symbol_count:
sc = symbol_count
else:
sc = []
psym = symbols[0]
count = 0
for sym in symbols:
if sym != psym:
sc.append((psym, count))
psym = sym
count = 1
else:
count += 1
sc.append((psym, count))
# Create the label
if label == '':
for sym, c in sc:
label += '%2s ' % sym
f.write(label + '\n')
# Write unitcell in real coordinates and adapt to VASP convention
# for unit cell
# ase Atoms doesn't store the lattice constant separately, so always
# write 1.0.
f.write('%19.16f\n' % 1.0)
if long_format:
latt_form = ' %21.16f'
else:
latt_form = ' %11.6f'
for vec in atoms.get_cell():
f.write(' ')
for el in vec:
f.write(latt_form % el)
f.write('\n')
# If we're writing a VASP 5.x format POSCAR file, write out the
# atomic symbols
if vasp5:
for sym, c in sc:
f.write(' %3s' % sym)
f.write('\n')
# Numbers of each atom
for sym, count in sc:
f.write(' %3i' % count)
f.write('\n')
if atoms.constraints:
f.write('Selective dynamics\n')
if direct:
f.write('Direct\n')
else:
f.write('Cartesian\n')
if long_format:
cform = ' %19.16f'
else:
cform = ' %9.6f'
for iatom, atom in enumerate(coord):
for dcoord in atom:
f.write(cform % dcoord)
if atoms.constraints:
for flag in sflags[iatom]:
if flag:
s = 'F'
else:
s = 'T'
f.write('%4s' % s)
f.write('\n')
if isinstance(filename, str):
f.close()
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