def _cubic_bulk(name, x, a):
if x == 'fcc':
atoms = Atoms(4 * name,
cell=(a, a, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0, 0.5, 0.5),
(0.5, 0, 0.5), (0.5, 0.5, 0)])
elif x == 'diamond':
atoms = _cubic_bulk(2 * name, 'zincblende', a)
elif x == 'zincblende':
atoms = Atoms(4 * name,
cell=(a, a, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0.25, 0.25, 0.25),
(0, 0.5, 0.5), (0.25, 0.75, 0.75),
(0.5, 0, 0.5), (0.75, 0.25, 0.75),
(0.5, 0.5, 0), (0.75, 0.75, 0.25)])
elif x == 'rocksalt':
atoms = Atoms(4 * name,
cell=(a, a, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0.5, 0, 0), (0, 0.5, 0.5),
(0.5, 0.5, 0.5), (0.5, 0, 0.5),
(0, 0, 0.5), (0.5, 0.5, 0),
(0, 0.5, 0)])
else:
raise RuntimeError
return atoms
def read_pdb(fileobj, index=-1):
"""Read PDB files.
The format is assumed to follow the description given in
http://www.wwpdb.org/documentation/format32/sect9.html."""
if isinstance(fileobj, str):
fileobj = open(fileobj)
atoms = Atoms()
positions = []
symbols = []
for line in fileobj.readlines():
if line.startswith('ATOM') or line.startswith('HETATM'):
try:
symbol = line[12:16].strip()
# we assume that the second character is a label
# in case that it is upper case
if len(symbol) > 1 and symbol[1].isupper():
symbol = symbol[0]
words = line[30:55].split()
#charges.append(float(c))
symbols.append(symbol)
positions.append(
np.array(
[float(words[0]),
float(words[1]),
float(words[2])]))
except:
print("Couldn't read entry in pdb")
pass
return Atoms(symbols=symbols, positions=positions)
def read_dacapo(filename):
from ase_ext.io.pupynere import NetCDFFile
nc = NetCDFFile(filename)
dims = nc.dimensions
vars = nc.variables
cell = vars['UnitCell'][-1]
try:
magmoms = vars['InitialAtomicMagneticMoment'][:]
except KeyError:
magmoms = None
try:
tags = vars['AtomTags'][:]
except KeyError:
tags = None
atoms = Atoms(scaled_positions=vars['DynamicAtomPositions'][-1],
symbols=[(a + b).strip()
for a, b in vars['DynamicAtomSpecies'][:]],
cell=cell,
magmoms=magmoms,
tags=tags,
pbc=True)
try:
energy = vars['TotalEnergy'][-1]
force = vars['DynamicAtomForces'][-1]
except KeyError:
energy = None
force = None
calc = SinglePointCalculator(energy, force, None, None,
atoms) ### Fixme magmoms
atoms.set_calculator(calc)
return atoms
def read_xsf(fileobj, index=-1):
if isinstance(fileobj, str):
fileobj = open(fileobj)
readline = fileobj.readline
line = readline()
if line.startswith('ANIMSTEPS'):
nimages = int(line.split()[1])
line = readline()
else:
nimages = 1
if line.startswith('CRYSTAL'):
pbc = True
elif line.startswith('SLAB'):
pbc = (True, True, Flase)
elif line.startswith('POLYMER'):
pbc = (True, False, Flase)
else:
pbc = False
images = []
for n in range(nimages):
cell = None
if pbc:
line = readline()
assert line.startswith('PRIMVEC')
cell = []
for i in range(3):
cell.append([float(x) for x in readline().split()])
line = readline()
assert line.startswith('PRIMCOORD')
natoms = int(readline().split()[0])
numbers = []
positions = []
for a in range(natoms):
line = readline().split()
numbers.append(int(line[0]))
positions.append([float(x) for x in line[1:]])
positions = np.array(positions)
if len(positions[0]) == 3:
forces = None
else:
positions = positions[:, :3]
forces = positions[:, 3:] * Hartree
image = Atoms(numbers, positions, cell=cell, pbc=pbc)
if forces is not None:
image.set_calculator(SinglePointCalculator(None, forces, None,
None, image))
images.append(image)
return images[index]
def read_xyz(fileobj, index=-1):
if isinstance(fileobj, str):
fileobj = open(fileobj)
lines = fileobj.readlines()
L1 = lines[0].split()
if len(L1) == 1:
# del lines[:2]
natoms = int(L1[0])
else:
natoms = len(lines)
energy=0
images = []
while len(lines) >= natoms:
positions = []
symbols = []
forces = []
charges = []
L2 = lines[1].split()
for line in lines[2:natoms+2]:
linesplit = line.split()
if len(linesplit)==5:
symbol, x, y, z, c = linesplit[:5]
charges.append(c)
else:
symbol, x, y, z = linesplit[:4]
symbols.append(symbol)
positions.append([float(x), float(y), float(z)])
if len(linesplit) > 9:
fx,fy,fz = linesplit[7:10]
forces.append([float(fx), float(fy), float(fz)])
cell=[]
if forces==[]:
forces=None
if len(lines[1].split())>0:
if len(lines[1].split("\""))>1:
L = lines[1].split("\"")[1].split()
else:
L = lines[1].split()
if len(L)>9:
energy=float(L[9])
try:
cell = ((float(L[0]),float(L[1]),float(L[2])),(float(L[3]),float(L[4]),float(L[5])),(float(L[6]),float(L[7]),float(L[8])))
except ValueError:
cell = ((0,0,0),(0,0,0),(0,0,0))
images.append(Atoms(symbols=symbols, positions=positions,forces=forces, energy=energy,cell=cell))
else:
images.append(Atoms(symbols=symbols, positions=positions,forces=forces, energy=energy))
if len(charges)>0:
images[-1].set_charges(charges)
del lines[:natoms + 2]
if ((len(lines)>0) and (len(lines[0].split())>0)):
natoms = int(lines[0].split()[0])
#return images[index]
return images
def read_turbomole(filename='coord'):
"""Method to read turbomole coord file
coords in bohr, atom types in lowercase, format:
$coord
x y z atomtype
x y z atomtype f
$end
Above 'f' means a fixed atom.
"""
from ase_ext import Atoms, Atom
from ase_ext.constraints import FixAtoms
if isinstance(filename, str):
f = open(filename)
lines = f.readlines()
atoms_pos = []
atom_symbols = []
dollar_count=0
myconstraints=[]
for line in lines:
if ('$' in line):
dollar_count = dollar_count + 1
if (dollar_count >= 2):
break
else:
x, y, z, symbolraw = line.split()[:4]
symbolshort=symbolraw.strip()
symbol=symbolshort[0].upper()+symbolshort[1:].lower()
#print symbol
atom_symbols.append(symbol)
atoms_pos.append([float(x)*Bohr, float(y)*Bohr, float(z)*Bohr])
cols = line.split()
if (len(cols) == 5):
fixedstr = line.split()[4].strip()
if (fixedstr == "f"):
myconstraints.append(True)
else:
myconstraints.append(False)
else:
myconstraints.append(False)
if type(filename) == str:
f.close()
atoms = Atoms(positions = atoms_pos, symbols = atom_symbols, pbc = False)
c = FixAtoms(myconstraints)
atoms.set_constraint(c)
#print c
return atoms
def read_cif(fileobj, index=-1):
if isinstance(fileobj, str):
fileobj = open(fileobj)
def search_key(fobj, key):
for line in fobj:
if key in line:
return line
return None
def get_key(fobj, key, pos=1):
line = search_key(fobj, key)
if line:
return float(line.split()[pos].split('(')[0])
return None
a = get_key(fileobj, '_cell_length_a')
b = get_key(fileobj, '_cell_length_b')
c = get_key(fileobj, '_cell_length_c')
alpha = pi * get_key(fileobj, '_cell_angle_alpha') / 180
beta = pi * get_key(fileobj, '_cell_angle_beta') / 180
gamma = pi * get_key(fileobj, '_cell_angle_gamma') / 180
va = a * np.array([1, 0, 0])
vb = b * np.array([cos(gamma), sin(gamma), 0])
cx = cos(beta)
cy = (cos(alpha) - cos(beta) * cos(gamma)) / sin(gamma)
cz = sqrt(1. - cx*cx - cy*cy)
vc = c * np.array([cx, cy, cz])
cell = np.array([va, vb, vc])
atoms = Atoms(cell=cell)
read = False
for line in fileobj:
if not read:
if '_atom_site_disorder_group' in line:
read = True
else:
word = line.split()
if len(word) < 5:
break
symbol = word[1]
pos = (float(word[2].split('(')[0]) * va +
float(word[3].split('(')[0]) * vb +
float(word[4].split('(')[0]) * vc )
atoms.append(Atom(symbol, pos))
return atoms
def read_vnl(filename):
from io import StringIO
vnl = VNLUnpickler(StringIO(ZipFile(filename).read('0_object'))).load()
conf = vnl.data['__properties__']['Atomic Configuration'].data
numbers = conf['_dataarray_']
positions = conf['_positions_'].data['_dataarray_']
return Atoms(numbers=numbers, positions=positions)
def bind(self, frame):
if not self.ui.get_widget('/MenuBar/ViewMenu/ShowBonds').get_active():
self.bonds = np.empty((0, 5), int)
return
from ase_ext.atoms import Atoms
from ase_ext.calculators.neighborlist import NeighborList
nl = NeighborList(self.images.r * 1.5, skin=0, self_interaction=False)
nl.update(
Atoms(positions=self.images.P[frame],
cell=(self.images.repeat[:, np.newaxis] *
self.images.A[frame]),
pbc=self.images.pbc))
nb = nl.nneighbors + nl.npbcneighbors
self.bonds = np.empty((nb, 5), int)
if nb == 0:
return
n1 = 0
for a in range(self.images.natoms):
indices, offsets = nl.get_neighbors(a)
n2 = n1 + len(indices)
self.bonds[n1:n2, 0] = a
self.bonds[n1:n2, 1] = indices
self.bonds[n1:n2, 2:] = offsets
n1 = n2
i = self.bonds[:n2, 2:].any(1)
self.bonds[n2:, 0] = self.bonds[i, 1]
self.bonds[n2:, 1] = self.bonds[i, 0]
self.bonds[n2:, 2:] = -self.bonds[i, 2:]
def read_iwm(fileobj, index=-1):
if isinstance(fileobj, str):
fileobj = open(fileobj)
lines = fileobj.readlines()
L1 = lines[1].split()
if len(L1) == 1:
del lines[:3]
natoms = int(L1[0])
else:
natoms = len(lines)
images = []
positions = []
symbols = []
for line in lines[:natoms]:
symbol, mass, x, y, z = line.split()[:5]
if symbol in iwm_symbols:
symbols.append(iwm_symbols[symbol])
else:
symbols.append(chemical_symbols[int(symbol)])
positions.append([float(x), float(y), float(z)])
del (lines[natoms:3 * natoms + 3])
cell = []
for line in lines[natoms:natoms + 3]:
x, y, z = line.split()[:3]
cell.append(np.array([float(x), float(y), float(z)]))
images.append(Atoms(symbols=symbols, positions=positions, cell=cell))
return images[index]
def make_test_dft_calculation():
a = b = 2.0
c = 6.0
atoms = Atoms(positions=[(0, 0, c / 2)],
symbols='H',
pbc=(1, 1, 0),
cell=(a, b, c),
calculator=TestCalculator())
return atoms
def read_I_info(fileobj, index=-1):
if isinstance(fileobj, str):
fileobj = open(fileobj)
lines = fileobj.readlines()
del lines[0]
finished = False
s = Atoms()
while not finished:
w = lines.pop(0).split()
if w[0].startswith('"'):
position = Bohr * np.array([float(w[3]), float(w[4]), float(w[5])])
s.append(Atom(w[0].replace('"', ''), position))
else:
finished = True
return s
def read_dacapo_text(fileobj):
if isinstance(fileobj, str):
fileobj = open(fileobj)
lines = fileobj.readlines()
i = lines.index(' Structure: A1 A2 A3\n')
cell = np.array([[float(w) for w in line.split()[2:5]]
for line in lines[i + 1:i + 4]]).transpose()
i = lines.index(' Structure: >> Ionic positions/velocities ' +
'in cartesian coordinates <<\n')
atoms = []
for line in lines[i + 4:]:
words = line.split()
if len(words) != 9:
break
Z, x, y, z = words[2:6]
atoms.append(Atom(int(Z), [float(x), float(y), float(z)]))
atoms = Atoms(atoms, cell=cell.tolist())
try:
i = lines.index(
' DFT: CPU time Total energy\n')
except ValueError:
pass
else:
column = lines[i + 3].split().index('selfcons') - 1
try:
i2 = lines.index(' ANALYSIS PART OF CODE\n', i)
except ValueError:
pass
else:
while i2 > i:
if lines[i2].startswith(' DFT:'):
break
i2 -= 1
energy = float(lines[i2].split()[column])
atoms.set_calculator(
SinglePointCalculator(energy, None, None, None, atoms))
return atoms
def _orthorhombic_bulk(name, x, a, covera=None):
if x == 'fcc':
b = a / sqrt(2)
atoms = Atoms(2 * name,
cell=(b, b, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0.5, 0.5, 0.5)])
elif x == 'bcc':
atoms = Atoms(2 * name,
cell=(a, a, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0.5, 0.5, 0.5)])
elif x == 'hcp':
atoms = Atoms(4 * name,
cell=(a, a * sqrt(3), covera * a),
scaled_positions=[(0, 0, 0), (0.5, 0.5, 0),
(0.5, 1.0 / 6.0, 0.5),
(0, 2.0 / 3.0, 0.5)],
pbc=True)
elif x == 'diamond':
atoms = _orthorhombic_bulk(2 * name, 'zincblende', a)
elif x == 'zincblende':
s1, s2 = string2symbols(name)
b = a / sqrt(2)
atoms = Atoms(2 * name,
cell=(b, b, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0.5, 0, 0.25),
(0.5, 0.5, 0.5), (0, 0.5, 0.75)])
elif x == 'rocksalt':
s1, s2 = string2symbols(name)
b = a / sqrt(2)
atoms = Atoms(2 * name,
cell=(b, b, a),
pbc=True,
scaled_positions=[(0, 0, 0), (0.5, 0.5, 0),
(0.5, 0.5, 0.5), (0, 0, 0.5)])
else:
raise RuntimeError
return atoms
def __getitem__(self, i=-1):
N = len(self.offsets)
if 0 <= i < N:
self.fd.seek(self.offsets[i])
try:
d = pickle.load(self.fd)
except EOFError:
raise IndexError
if i == N - 1:
self.offsets.append(self.fd.tell())
try:
magmoms = d['magmoms']
except KeyError:
magmoms = None
atoms = Atoms(positions=d['positions'],
numbers=self.numbers,
cell=d['cell'],
momenta=d['momenta'],
magmoms=magmoms,
tags=self.tags,
masses=self.masses,
pbc=self.pbc,
constraint=[c.copy() for c in self.constraints])
if 'energy' in d:
calc = SinglePointCalculator(d.get('energy', None),
d.get('forces', None),
d.get('stress', None), magmoms,
atoms)
atoms.set_calculator(calc)
return atoms
if i >= N:
for j in range(N - 1, i + 1):
atoms = self[j]
return atoms
i = len(self) + i
if i < 0:
raise IndexError('Trajectory index out of range.')
return self[i]
def copy(self):
from ase_ext.atoms import Atoms
return Atoms(positions=self.get_positions(),
numbers=self.get_atomic_numbers(),
tags=self.get_tags(),
momenta=self.get_momenta(),
masses=self.get_masses(),
magmoms=self.get_initial_magnetic_moments(),
charges=self.get_charges(),
cell=self.get_cell(),
pbc=self.get_pbc(),
constraint=None,
calculator=None) # Don't copy the calculator
def read_mol(fileobj, index=-1):
if isinstance(fileobj, str):
fileobj = open(fileobj)
lines = fileobj.readlines()
del (lines[:3])
L1 = lines[0].split()
del (lines[0])
natoms = int(L1[0])
positions = []
symbols = []
for line in lines[:natoms]:
x, y, z, symbol = line.split()[:4]
symbols.append(symbol)
positions.append([float(x), float(y), float(z)])
return Atoms(symbols=symbols, positions=positions)
def read_exciting(fileobj, index=-1):
"""Reads structure from exiting xml file.
Parameters
----------
fileobj: file object
Filehandle from which data should be read.
Other parameters
----------------
index: integer -1
Not used in this implementation.
"""
from lxml import etree as ET
#parse file into element tree
doc = ET.parse(fileobj)
root = doc.getroot()
speciesnodes = root.find('structure').getiterator('species')
symbols = []
positions = []
basevects = []
atoms = None
#collect data from tree
for speciesnode in speciesnodes:
symbol = speciesnode.get('speciesfile').split('.')[0]
natoms = speciesnode.getiterator('atom')
for atom in natoms:
x, y, z = atom.get('coord').split()
positions.append([float(x), float(y), float(z)])
symbols.append(symbol)
basevectsn = doc.xpath('//basevect/text()')
for basevect in basevectsn:
x, y, z = basevect.split()
basevects.append([float(x) * Bohr, float(y) * Bohr, float(z) * Bohr])
atoms = Atoms(symbols=symbols, cell=basevects)
atoms.set_scaled_positions(positions)
if 'molecule' in list(root.find('structure').attrib.keys()):
if root.find('structure').attrib['molecule']:
atoms.set_pbc(False)
else:
atoms.set_pbc(True)
return atoms
def read_sdf(fileobj):
if isinstance(fileobj, str):
fileobj = open(fileobj)
lines = fileobj.readlines()
# first three lines header
del lines[:3]
#
L1 = lines.pop(0).split()
natoms = int(L1[0])
positions = []
symbols = []
for line in lines[:natoms]:
x, y, z, symbol = line.split()[:4]
symbols.append(symbol)
positions.append([float(x), float(y), float(z)])
return Atoms(symbols=symbols, positions=positions)
def run(opt, args):
images = Images()
if opt.aneb:
opt.image_number = '-1'
if len(args) > 0:
from ase_ext.io import string2index
images.read(args, string2index(opt.image_number))
else:
images.initialize([Atoms()])
if opt.interpolate:
images.interpolate(opt.interpolate)
if opt.aneb:
images.aneb()
if opt.repeat != '1':
r = opt.repeat.split(',')
if len(r) == 1:
r = 3 * r
images.repeat_images([int(c) for c in r])
if opt.output is not None:
images.write(opt.output, rotations=opt.rotations,
show_unit_cell=opt.show_unit_cell)
opt.terminal = True
if opt.terminal:
if opt.graph is not None:
data = images.graph(opt.graph)
for line in data.T:
for x in line:
print(x, end=' ')
print()
else:
from ase_ext.gui.gui import GUI
gui = GUI(images, opt.rotations, opt.show_unit_cell, opt.bonds)
gui.run(opt.graph)
def read_cube(fileobj, index=-1, read_data=False):
if isinstance(fileobj, str):
fileobj = open(fileobj)
readline = fileobj.readline
readline()
axes = ['XYZ'.index(s[0]) for s in readline().split()[2::3]]
if axes == []:
axes = [0, 1, 2]
line = readline().split()
natoms = int(line[0])
corner = [Bohr * float(x) for x in line[1:]]
cell = np.empty((3, 3))
shape = []
for i in range(3):
n, x, y, z = [float(s) for s in readline().split()]
shape.append(n)
if n % 2 == 1:
n += 1
cell[i] = n * Bohr * np.array([x, y, z])
numbers = np.empty(natoms, int)
positions = np.empty((natoms, 3))
for i in range(natoms):
line = readline().split()
numbers[i] = int(line[0])
positions[i] = [float(s) for s in line[2:]]
positions *= Bohr
atoms = Atoms(numbers=numbers, positions=positions, cell=cell)
if read_data:
data = np.array([float(s)
for s in fileobj.read().split()]).reshape(shape)
if axes != [0, 1, 2]:
data = data.transpose(axes).copy()
return data, atoms
return atoms
def get_atoms(self, frame):
atoms = Atoms(positions=self.P[frame],
numbers=self.Z,
magmoms=self.M[0],
tags=self.T,
cell=self.A[frame],
pbc=self.pbc)
# check for constrained atoms and add them accordingly:
if not self.dynamic.all():
atoms.set_constraint(FixAtoms(mask=1 - self.dynamic))
atoms.set_calculator(
SinglePointCalculator(self.E[frame], self.F[frame], None, None,
atoms))
return atoms
def bulk(name,
crystalstructure,
a=None,
c=None,
covera=None,
orthorhombic=False,
cubic=False):
"""Helper function for creating bulk systems.
name: str
Chemical symbol or symbols as in 'MgO' or 'NaCl'.
crystalstructure: str
Must be one of sc, fcc, bcc, hcp, diamond, zincblende or
rocksalt.
a: float
Lattice constant.
c: float
Lattice constant.
covera: float
c/a raitio used for hcp. Defaults to ideal ratio.
orthorhombic: bool
Construct orthorhombic unit cell instead of primitive cell
which is the default.
cubic: bool
Construct cubic unit cell.
"""
if covera is not None and c is not None:
raise ValueError("Don't specify both c and c/a!")
if covera is None and c is None:
covera = sqrt(8.0 / 3.0)
if a is None:
a = estimate_lattice_constant(name, crystalstructure, covera)
if covera is None and c is not None:
covera = c / a
x = crystalstructure.lower()
if orthorhombic and x != 'sc':
return _orthorhombic_bulk(name, x, a, covera)
if cubic and x == 'bcc':
return _orthorhombic_bulk(name, x, a, covera)
if cubic and x != 'sc':
return _cubic_bulk(name, x, a)
if x == 'sc':
atoms = Atoms(name, cell=(a, a, a), pbc=True)
elif x == 'fcc':
b = a / 2
atoms = Atoms(name, cell=[(0, b, b), (b, 0, b), (b, b, 0)], pbc=True)
elif x == 'bcc':
b = a / 2
atoms = Atoms(name,
cell=[(-b, b, b), (b, -b, b), (b, b, -b)],
pbc=True)
elif x == 'hcp':
atoms = Atoms(2 * name,
scaled_positions=[(0, 0, 0),
(1.0 / 3.0, 1.0 / 3.0, 0.5)],
cell=[(a, 0, 0), (a / 2, a * sqrt(3) / 2, 0),
(0, 0, covera * a)],
pbc=True)
elif x == 'diamond':
atoms = bulk(2 * name, 'zincblende', a)
elif x == 'zincblende':
s1, s2 = string2symbols(name)
atoms = bulk(s1, 'fcc', a) + bulk(s2, 'fcc', a)
atoms.positions[1] += a / 4
elif x == 'rocksalt':
s1, s2 = string2symbols(name)
atoms = bulk(s1, 'fcc', a) + bulk(s2, 'fcc', a)
atoms.positions[1, 0] += a / 2
else:
raise ValueError('Unknown crystal structure: ' + crystalstructure)
return atoms
def nanotube(n, m, length=1, bond=1.42, symbol='C', verbose=False):
if n < m:
m, n = n, m
nk = 6000
sq3 = sqrt(3.0)
a = sq3 * bond
l2 = n * n + m * m + n * m
l = sqrt(l2)
dt = a * l / np.pi
nd = gcd(n, m)
if (n - m) % (3 * nd) == 0:
ndr = 3 * nd
else:
ndr = nd
nr = (2 * m + n) / ndr
ns = -(2 * n + m) / ndr
nt2 = 3 * l2 / ndr / ndr
nt = np.floor(sqrt(nt2))
nn = 2 * l2 / ndr
ichk = 0
if nr == 0:
n60 = 1
else:
n60 = nr * 4
absn = abs(n60)
nnp = []
nnq = []
for i in range(-absn, absn + 1):
for j in range(-absn, absn + 1):
j2 = nr * j - ns * i
if j2 == 1:
j1 = m * i - n * j
if j1 > 0 and j1 < nn:
ichk += 1
nnp.append(i)
nnq.append(j)
if ichk == 0:
raise RuntimeError('not found p, q strange!!')
if ichk >= 2:
raise RuntimeError('more than 1 pair p, q strange!!')
nnnp = nnp[0]
nnnq = nnq[0]
if verbose:
print('the symmetry vector is', nnnp, nnnq)
lp = nnnp * nnnp + nnnq * nnnq + nnnp * nnnq
r = a * sqrt(lp)
c = a * l
t = sq3 * c / ndr
if 2 * nn > nk:
raise RuntimeError('parameter nk is too small!')
rs = c / (2.0 * np.pi)
if verbose:
print('radius=', rs, t)
q1 = np.arctan((sq3 * m) / (2 * n + m))
q2 = np.arctan((sq3 * nnnq) / (2 * nnnp + nnnq))
q3 = q1 - q2
q4 = 2.0 * np.pi / nn
q5 = bond * np.cos((np.pi / 6.0) - q1) / c * 2.0 * np.pi
h1 = abs(t) / abs(np.sin(q3))
h2 = bond * np.sin((np.pi / 6.0) - q1)
ii = 0
x, y, z = [], [], []
for i in range(nn):
x1, y1, z1 = 0, 0, 0
k = np.floor(i * abs(r) / h1)
x1 = rs * np.cos(i * q4)
y1 = rs * np.sin(i * q4)
z1 = (i * abs(r) - k * h1) * np.sin(q3)
kk2 = abs(np.floor((z1 + 0.0001) / t))
if z1 >= t - 0.0001:
z1 -= t * kk2
elif z1 < 0:
z1 += t * kk2
ii += 1
x.append(x1)
y.append(y1)
z.append(z1)
z3 = (i * abs(r) - k * h1) * np.sin(q3) - h2
ii += 1
if z3 >= 0 and z3 < t:
x2 = rs * np.cos(i * q4 + q5)
y2 = rs * np.sin(i * q4 + q5)
z2 = (i * abs(r) - k * h1) * np.sin(q3) - h2
x.append(x2)
y.append(y2)
z.append(z2)
else:
x2 = rs * np.cos(i * q4 + q5)
y2 = rs * np.sin(i * q4 + q5)
z2 = (i * abs(r) - (k + 1) * h1) * np.sin(q3) - h2
kk = abs(np.floor(z2 / t))
if z2 >= t - 0.0001:
z2 -= t * kk
elif z2 < 0:
z2 += t * kk
x.append(x2)
y.append(y2)
z.append(z2)
ntotal = 2 * nn
X = []
for i in range(ntotal):
X.append([x[i], y[i], z[i]])
if length > 1:
xx = X[:]
for mnp in range(2, length + 1):
for i in range(len(xx)):
X.append(xx[i][:2] + [xx[i][2] + (mnp - 1) * t])
TransVec = t
NumAtom = ntotal * length
Diameter = rs * 2
ChiralAngle = np.arctan((sq3 * n) / (2 * m + n)) / (np.pi * 180)
cell = [Diameter * 2, Diameter * 2, length * t]
atoms = Atoms(symbol + str(NumAtom),
positions=X,
cell=cell,
pbc=[False, False, True])
atoms.center()
if verbose:
print('translation vector =', TransVec)
print('diameter = ', Diameter)
print('chiral angle = ', ChiralAngle)
return atoms
def surface(symbol, structure, face, size, a, c, vacuum, orthogonal=True):
"""Function to build often used surfaces.
Don't call this function directly - use fcc100, fcc110, bcc111, ..."""
Z = atomic_numbers[symbol]
if a is None:
sym = reference_states[Z]['symmetry'].lower()
if sym != structure:
raise ValueError("Can't guess lattice constant for %s-%s!" %
(structure, symbol))
a = reference_states[Z]['a']
if structure == 'hcp' and c is None:
if reference_states[Z]['symmetry'].lower() == 'hcp':
c = reference_states[Z]['c/a'] * a
else:
c = sqrt(8 / 3.0) * a
positions = np.empty((size[2], size[1], size[0], 3))
positions[..., 0] = np.arange(size[0]).reshape((1, 1, -1))
positions[..., 1] = np.arange(size[1]).reshape((1, -1, 1))
positions[..., 2] = np.arange(size[2]).reshape((-1, 1, 1))
numbers = np.ones(size[0] * size[1] * size[2], int) * Z
tags = np.empty((size[2], size[1], size[0]), int)
tags[:] = np.arange(size[2], 0, -1).reshape((-1, 1, 1))
slab = Atoms(numbers,
tags=tags.ravel(),
pbc=(True, True, False),
cell=size)
surface_cell = None
sites = {'ontop': (0, 0)}
surf = structure + face
if surf == 'fcc100':
cell = (sqrt(0.5), sqrt(0.5), 0.5)
positions[-2::-2, ..., :2] += 0.5
sites.update({'hollow': (0.5, 0.5), 'bridge': (0.5, 0)})
elif surf == 'fcc110':
cell = (1.0, sqrt(0.5), sqrt(0.125))
positions[-2::-2, ..., :2] += 0.5
sites.update({'hollow': (0.5, 0.5), 'longbridge': (0.5, 0),
'shortbridge': (0, 0.5)})
elif surf == 'bcc100':
cell = (1.0, 1.0, 0.5)
positions[-2::-2, ..., :2] += 0.5
sites.update({'hollow': (0.5, 0.5), 'bridge': (0.5, 0)})
else:
if orthogonal and size[1] % 2 == 1:
raise ValueError(("Can't make orthorhombic cell with size=%r. " %
(tuple(size),)) +
'Second number in size must be even.')
if surf == 'fcc111':
cell = (sqrt(0.5), sqrt(0.375), 1 / sqrt(3))
if orthogonal:
positions[-1::-3, 1::2, :, 0] += 0.5
positions[-2::-3, 1::2, :, 0] += 0.5
positions[-3::-3, 1::2, :, 0] -= 0.5
positions[-2::-3, ..., :2] += (0.0, 2.0 / 3)
positions[-3::-3, ..., :2] += (0.5, 1.0 / 3)
else:
positions[-2::-3, ..., :2] += (-1.0 / 3, 2.0 / 3)
positions[-3::-3, ..., :2] += (1.0 / 3, 1.0 / 3)
sites.update({'bridge': (0.5, 0), 'fcc': (1.0 / 3, 1.0 / 3),
'hcp': (2.0 / 3, 2.0 / 3)})
elif surf == 'hcp0001':
cell = (1.0, sqrt(0.75), 0.5 * c / a)
if orthogonal:
positions[:, 1::2, :, 0] += 0.5
positions[-2::-2, ..., :2] += (0.0, 2.0 / 3)
else:
positions[-2::-2, ..., :2] += (-1.0 / 3, 2.0 / 3)
sites.update({'bridge': (0.5, 0), 'fcc': (1.0 / 3, 1.0 / 3),
'hcp': (2.0 / 3, 2.0 / 3)})
elif surf == 'bcc110':
cell = (1.0, sqrt(0.5), sqrt(0.5))
if orthogonal:
positions[:, 1::2, :, 0] += 0.5
positions[-2::-2, ..., :2] += (0.0, 1.0)
else:
positions[-2::-2, ..., :2] += (-0.5, 1.0)
sites.update({'shortbridge': (0, 0.5),
'longbridge': (0.5, 0),
'hollow': (0.375, 0.25)})
elif surf == 'bcc111':
cell = (sqrt(2), sqrt(1.5), sqrt(3) / 6)
if orthogonal:
positions[-1::-3, 1::2, :, 0] += 0.5
positions[-2::-3, 1::2, :, 0] += 0.5
positions[-3::-3, 1::2, :, 0] -= 0.5
positions[-2::-3, ..., :2] += (0.0, 2.0 / 3)
positions[-3::-3, ..., :2] += (0.5, 1.0 / 3)
else:
positions[-2::-3, ..., :2] += (-1.0 / 3, 2.0 / 3)
positions[-3::-3, ..., :2] += (1.0 / 3, 1.0 / 3)
sites.update({'hollow': (1.0 / 3, 1.0 / 3)})
surface_cell = a * np.array([(cell[0], 0),
(cell[0] / 2, cell[1])])
if not orthogonal:
cell = np.array([(cell[0], 0, 0),
(cell[0] / 2, cell[1], 0),
(0, 0, cell[2])])
if surface_cell is None:
surface_cell = a * np.diag(cell[:2])
if isinstance(cell, tuple):
cell = np.diag(cell)
slab.set_positions(positions.reshape((-1, 3)))
slab.set_cell([a * v * n for v, n in zip(cell, size)], scale_atoms=True)
if vacuum is not None:
slab.center(vacuum=vacuum, axis=2)
slab.adsorbate_info['cell'] = surface_cell
slab.adsorbate_info['sites'] = sites
return slab
def read_dftb(filename='dftb_in.hsd'):
"""Method to read coordinates form DFTB+ input file dftb_in.hsd
additionally read information about fixed atoms
and periodic boundary condition
"""
from ase_ext import Atoms, Atom
from ase_ext.constraints import FixAtoms
import sys, string
if isinstance(filename, str):
f = open(filename)
lines = f.readlines()
atoms_pos = []
atom_symbols = []
type_names = []
my_pbc = False
myconstraints = []
moved_atoms_found = False
range_found = False
moved_atoms = []
for line in lines:
if (line.strip().startswith('#')):
pass
else:
if ('TypeNames' in line):
col = line.split()
for i in range(3, len(col) - 1):
type_names.append(col[i].strip("\""))
elif ('Periodic' in line):
if ('Yes' in line):
my_pbc = True
else:
pass
start_reading_coords = False
stop_reading_coords = False
for line in lines:
if (line.strip().startswith('#')):
pass
else:
if ('TypesAndCoordinates' in line):
start_reading_coords = True
if start_reading_coords:
if ('}' in line):
stop_reading_coords = True
if (start_reading_coords and not (stop_reading_coords)
and not 'TypesAndCoordinates' in line):
typeindexstr, x, y, z = line.split()[:4]
typeindex = int(typeindexstr)
symbol = type_names[typeindex - 1]
atom_symbols.append(symbol)
atoms_pos.append([float(x), float(y), float(z)])
if type(filename) == str:
f.close()
atoms = Atoms(positions=atoms_pos, symbols=atom_symbols, pbc=my_pbc)
return atoms
def read(filename, index=-1, format=None):
"""Read Atoms object(s) from file.
filename: str
Name of the file to read from.
index: int or slice
If the file contains several configurations, the last configuration
will be returned by default. Use index=n to get configuration
number n (counting from zero).
format: str
Used to specify the file-format. If not given, the
file-format will be guessed by the *filetype* function.
Known formats:
========================= ===========
format short name
========================= ===========
GPAW restart-file gpw
Dacapo netCDF output file dacapo
Old ASE netCDF trajectory nc
Virtual Nano Lab file vnl
ASE pickle trajectory traj
GPAW text output gpaw-text
CUBE file cube
XCrySDen Structure File xsf
Dacapo text output dacapo-text
XYZ-file xyz
VASP POSCAR/CONTCAR file vasp
VASP OUTCAR file vasp_out
Protein Data Bank pdb
FHI-aims geometry file aims
FHI-aims output file aims_out
VTK XML Image Data vti
VTK XML Structured Grid vts
VTK XML Unstructured Grid vtu
TURBOMOLE coord file tmol
exciting input exi
AtomEye configuration cfg
WIEN2k structure file struct
DftbPlus input file dftb
SYBYL mol file mol2
========================= ===========
"""
if isinstance(filename, str):
p = filename.rfind('@')
if p != -1:
try:
index = string2index(filename[p + 1:])
except ValueError:
pass
else:
filename = filename[:p]
if isinstance(index, str):
index = string2index(index)
if format is None:
format = filetype(filename)
if format.startswith('gpw'):
import gpaw
r = gpaw.io.open(filename, 'r')
positions = r.get('CartesianPositions') * Bohr
numbers = r.get('AtomicNumbers')
cell = r.get('UnitCell') * Bohr
pbc = r.get('BoundaryConditions')
tags = r.get('Tags')
magmoms = r.get('MagneticMoments')
atoms = Atoms(positions=positions, numbers=numbers, cell=cell, pbc=pbc)
if tags.any():
atoms.set_tags(tags)
if magmoms.any():
atoms.set_initial_magnetic_moments(magmoms)
return atoms
if format == 'exi':
from ase_ext.io.exciting import read_exciting
return read_exciting(filename, index)
if format == 'mol2':
from ase_ext.io.mol2 import read_mol2
return read_mol2(filename, index)
if format == 'xyz':
from ase_ext.io.xyz import read_xyz
return read_xyz(filename, index)
if format == 'quipxyz':
from ase_ext.io.quipxyz import read_xyz
return read_xyz(filename, index)
if format == 'traj':
from ase_ext.io.trajectory import read_trajectory
return read_trajectory(filename, index)
if format == 'cube':
from ase_ext.io.cube import read_cube
return read_cube(filename, index)
if format == 'nc':
from ase_ext.io.netcdf import read_netcdf
return read_netcdf(filename, index)
if format == 'gpaw-text':
from ase_ext.io.gpawtext import read_gpaw_text
return read_gpaw_text(filename, index)
if format == 'dacapo-text':
from ase_ext.io.dacapo import read_dacapo_text
return read_dacapo_text(filename)
if format == 'dacapo':
from ase_ext.io.dacapo import read_dacapo
return read_dacapo(filename)
if format == 'xsf':
from ase_ext.io.xsf import read_xsf
return read_xsf(filename, index)
if format == 'vasp':
from ase_ext.io.vasp import read_vasp
return read_vasp(filename)
if format == 'vasp_out':
from ase_ext.io.vasp import read_vasp_out
return read_vasp_out(filename, index)
if format == 'mol':
from ase_ext.io.mol import read_mol
return read_mol(filename)
if format == 'pdb':
from ase_ext.io.pdb import read_pdb
return read_pdb(filename)
if format == 'cif':
from ase_ext.io.cif import read_cif
return read_cif(filename)
if format == 'struct':
from ase_ext.io.wien2k import read_struct
return read_struct(filename)
if format == 'vti':
from ase_ext.io.vtkxml import read_vti
return read_vti(filename)
if format == 'vts':
from ase_ext.io.vtkxml import read_vts
return read_vts(filename)
if format == 'vtu':
from ase_ext.io.vtkxml import read_vtu
return read_vtu(filename)
if format == 'aims':
from ase_ext.io.aims import read_aims
return read_aims(filename)
if format == 'aims_out':
from ase_ext.io.aims import read_aims_output
return read_aims_output(filename, index)
if format == 'iwm':
from ase_ext.io.iwm import read_iwm
return read_iwm(filename)
if format == 'Cmdft':
from ase_ext.io.cmdft import read_I_info
return read_I_info(filename)
if format == 'tmol':
from ase_ext.io.turbomole import read_turbomole
return read_turbomole(filename)
if format == 'cfg':
from ase_ext.io.cfg import read_cfg
return read_cfg(filename)
if format == 'dftb':
from ase_ext.io.dftb import read_dftb
return read_dftb(filename)
if format == 'sdf':
from ase_ext.io.sdf import read_sdf
return read_sdf(filename)
raise RuntimeError('File format descriptor ' + format + ' not recognized!')
def read_netcdf(filename, index=-1):
nc = NetCDFFile(filename)
dims = nc.dimensions
vars = nc.variables
positions = vars['CartesianPositions']
numbers = vars['AtomicNumbers'][:]
pbc = vars['BoundaryConditions'][:]
cell = vars['UnitCell']
tags = vars['Tags'][:]
if not tags.any():
tags = None
magmoms = vars['MagneticMoments'][:]
if not magmoms.any():
magmoms = None
nimages = positions.shape[0]
attach_calculator = False
if 'PotentialEnergy' in vars:
energy = vars['PotentialEnergy']
attach_calculator = True
else:
energy = nimages * [None]
if 'CartesianForces' in vars:
forces = vars['CartesianForces']
attach_calculator = True
else:
forces = nimages * [None]
if 'Stress' in vars:
stress = vars['Stress']
attach_calculator = True
else:
stress = nimages * [None]
if isinstance(index, int):
indices = [index]
else:
indices = list(range(nimages))[index]
images = []
for i in indices:
atoms = Atoms(positions=positions[i],
numbers=numbers,
cell=cell[i],
pbc=pbc,
tags=tags,
magmoms=magmoms)
if attach_calculator:
calc = SinglePointCalculator(energy[i], forces[i], stress[i], None,
atoms) ### Fixme magmoms
atoms.set_calculator(calc)
images.append(atoms)
if isinstance(index, int):
return images[0]
else:
return images
def graphene_nanoribbon(n,
m,
side='zigzag',
saturated="no",
C_H=1.09,
C_C=1.42,
vacc=5.,
magnetic=None,
initial_mag=1.12,
sheet=False,
main_element='C',
satur_element='H'):
"""Create a graphene nanoribbon.
Creates a graphene nanoribbon in the x-z plane, with the nanoribbon
running along the z axis.
Parameters:
n: The width of the nanoribbon
m: The length of the nanoribbon.
side ('zigzag'): The orientation of the ribbon. Must be either 'zigzag'
or 'armchair'.
saturated (no/yes/side): If yes, hydrogen atoms are placed along the edges. If side, then only 2 sides are saturated.
C_H: Carbon-hydrogen bond length. Default: 1.09 Angstrom
C_C: Carbon-carbon bond length. Default: 1.42 Angstrom.
vacc: Amount of vacuum. Default 5 Angstrom.
magnetic: Make the edges magnetic.
initial_mag: Magnitude of magnetic moment if magnetic=True.
sheet: If true, make an infinite sheet instead of a ribbon.
"""
#This function creates the coordinates for a graphene nanoribbon,
#n is width, m is length
b = sqrt(3) * C_C / 4
arm_unit = Atoms(main_element + '4',
pbc=(1, 0, 1),
cell=[4 * b, vacc, 3 * C_C])
arm_unit.positions = [[0, 0, 0], [b * 2, 0, C_C / 2.],
[b * 2, 0, 3 * C_C / 2.], [0, 0, 2 * C_C]]
zz_unit = Atoms(main_element + '2',
pbc=(1, 0, 1),
cell=[3 * C_C / 2., vacc, b * 4])
zz_unit.positions = [[0, 0, 0], [C_C / 2., 0, b * 2]]
atoms = Atoms()
tol = 1e-4
if sheet:
vacc2 = 0.0
else:
vacc2 = vacc
if side == 'zigzag':
edge_index0 = np.arange(m) * 2 + 1
edge_index1 = (n - 1) * m * 2 + np.arange(m) * 2
edge_index2 = []
edge_index3 = []
for i in range(0, n, 2):
edge_index2.append(i * m * 2)
edge_index3.append((i + 1) * m * 2 - 1)
if i > 1:
edge_index2.append(i * m * 2 - 1)
edge_index3.append(i * m * 2 - 2)
edge_index2 = np.array(edge_index2)
edge_index3 = np.array(edge_index3)
if magnetic:
mms = np.zeros(m * n * 2)
for i in edge_index0:
mms[i] = initial_mag
for i in edge_index1:
mms[i] = -initial_mag
for i in range(n):
layer = zz_unit.repeat((1, 1, m))
layer.positions[:, 0] -= 3 * C_C / 2 * i
if i % 2 == 1:
layer.positions[:, 2] += 2 * b
layer[-1].position[2] -= b * 4 * m
atoms += layer
if magnetic:
atoms.set_initial_magnetic_moments(mms)
if saturated != "no":
H_atoms0 = Atoms(satur_element + str(m))
H_atoms0.positions = atoms[edge_index0].positions
H_atoms0.positions[:, 0] += C_H
H_atoms1 = Atoms(satur_element + str(m))
H_atoms1.positions = atoms[edge_index1].positions
H_atoms1.positions[:, 0] -= C_H
H_atoms2 = Atoms(satur_element + str(n))
H_atoms2.positions = atoms[edge_index2].positions
H_atoms2.positions[:, 2] -= C_H
H_atoms3 = Atoms(satur_element + str(n))
H_atoms3.positions = atoms[edge_index3].positions
H_atoms3.positions[:, 2] += C_H
if saturated == "yes":
atoms += H_atoms0 + H_atoms1 + H_atoms2 + H_atoms3
if saturated == "side":
atoms += H_atoms0 + H_atoms1
atoms.cell = [n * 3 * C_C / 2 + vacc2, vacc + 5.0, m * 4 * b]
elif side == 'armchair':
for i in range(n):
layer = arm_unit.repeat((1, 1, m))
layer.positions[:, 0] -= 4 * b * i
atoms += layer
atoms.cell = [b * 4 * n + vacc2, vacc, 3 * C_C * m]
atoms.center()
atoms.set_pbc([sheet, False, True])
return atoms
def add_adsorbate(slab, adsorbate, height, position=(0, 0), offset=None,
mol_index=0):
"""Add an adsorbate to a surface.
This function adds an adsorbate to a slab. If the slab is
produced by one of the utility functions in ase_ext.lattice.surface, it
is possible to specify the position of the adsorbate by a keyword
(the supported keywords depend on which function was used to
create the slab).
If the adsorbate is a molecule, the atom indexed by the mol_index
optional argument is positioned on top of the adsorption position
on the surface, and it is the responsibility of the user to orient
the adsorbate in a sensible way.
This function can be called multiple times to add more than one
adsorbate.
Parameters:
slab: The surface onto which the adsorbate should be added.
adsorbate: The adsorbate. Must be one of the following three types:
A string containing the chemical symbol for a single atom.
An atom object.
An atoms object (for a molecular adsorbate).
height: Height above the surface.
position: The x-y position of the adsorbate, either as a tuple of
two numbers or as a keyword (if the surface is produced by one
of the functions in ase_ext.lattice.surfaces).
offset (default: None): Offsets the adsorbate by a number of unit
cells. Mostly useful when adding more than one adsorbate.
mol_index (default: 0): If the adsorbate is a molecule, index of
the atom to be positioned above the location specified by the
position argument.
Note *position* is given in absolute xy coordinates (or as
a keyword), whereas offset is specified in unit cells. This
can be used to give the positions in units of the unit cell by
using *offset* instead.
"""
info = slab.adsorbate_info
if 'cell' not in info:
info['cell'] = slab.get_cell()[:2,:2]
pos = np.array([0.0, 0.0]) # (x, y) part
spos = np.array([0.0, 0.0]) # part relative to unit cell
if offset is not None:
spos += np.asarray(offset, float)
if isinstance(position, str):
# A site-name:
if 'sites' not in info:
raise TypeError('If the atoms are not made by an ' +
'ase.lattice.surface function, ' +
'position cannot be a name.')
if position not in info['sites']:
raise TypeError('Adsorption site %s not supported.' % position)
spos += info['sites'][position]
else:
pos += position
pos += np.dot(spos, info['cell'])
# Convert the adsorbate to an Atoms object
if isinstance(adsorbate, Atoms):
ads = adsorbate
elif isinstance(adsorbate, Atom):
ads = Atoms([adsorbate])
else:
# Hope it is a useful string or something like that
ads = Atoms(adsorbate)
# Get the z-coordinate:
try:
a = info['top layer atom index']
except KeyError:
a = slab.positions[:, 2].argmax()
info['top layer atom index']= a
z = slab.positions[a, 2] + height
# Move adsorbate into position
ads.translate([pos[0], pos[1], z] - ads.positions[mol_index])
# Attach the adsorbate
slab.extend(ads)
