def get_magnetizations(mydir, ion_list):
data = []
max_row = 0
for (parent, subdirs, files) in os.walk(mydir):
for f in files:
if re.match("OUTCAR*", f):
try:
row = []
fullpath = os.path.join(parent, f)
outcar = Outcar(fullpath)
mags = outcar.magnetization
mags = [m["tot"] for m in mags]
all_ions = xrange(len(mags))
row.append(fullpath.lstrip("./"))
if ion_list:
all_ions = ion_list
for ion in all_ions:
row.append(str(mags[ion]))
data.append(row)
if len(all_ions) > max_row:
max_row = len(all_ions)
except:
pass
for d in data:
if len(d) < max_row + 1:
d.extend([""] * (max_row + 1 - len(d)))
headers = ["Filename"]
for i in xrange(max_row):
headers.append(str(i))
print str_aligned(data, headers)
def get_energies(rootdir, reanalyze, verbose, pretty, detailed, sort):
if verbose:
FORMAT = "%(relativeCreated)d msecs : %(message)s"
logging.basicConfig(level=logging.INFO, format=FORMAT)
if not detailed:
drone = SimpleVaspToComputedEntryDrone(inc_structure=True)
else:
drone = VaspToComputedEntryDrone(inc_structure=True,
data=["filename",
"initial_structure"])
ncpus = multiprocessing.cpu_count()
logging.info("Detected {} cpus".format(ncpus))
queen = BorgQueen(drone, number_of_drones=ncpus)
if os.path.exists(save_file) and not reanalyze:
msg = "Using previously assimilated data from {}.".format(save_file) \
+ " Use -f to force re-analysis."
queen.load_data(save_file)
else:
if ncpus > 1:
queen.parallel_assimilate(rootdir)
else:
queen.serial_assimilate(rootdir)
msg = "Analysis results saved to {} for faster ".format(save_file) + \
"subsequent loading."
queen.save_data(save_file)
entries = queen.get_data()
if sort == "energy_per_atom":
entries = sorted(entries, key=lambda x: x.energy_per_atom)
elif sort == "filename":
entries = sorted(entries, key=lambda x: x.data["filename"])
all_data = []
for e in entries:
if not detailed:
delta_vol = "{:.2f}".format(e.data["delta_volume"] * 100)
else:
delta_vol = e.structure.volume / \
e.data["initial_structure"].volume - 1
delta_vol = "{:.2f}".format(delta_vol * 100)
all_data.append((e.data["filename"].replace("./", ""),
re.sub("\s+", "", e.composition.formula),
"{:.5f}".format(e.energy),
"{:.5f}".format(e.energy_per_atom),
delta_vol))
if len(all_data) > 0:
headers = ("Directory", "Formula", "Energy", "E/Atom", "% vol chg")
if pretty:
from prettytable import PrettyTable
t = PrettyTable(headers)
t.set_field_align("Directory", "l")
map(t.add_row, all_data)
print t
else:
print str_aligned(all_data, headers)
print msg
else:
print "No valid vasp run found."
def get_magnetizations(mydir, ion_list):
data = []
max_row = 0
for (parent, subdirs, files) in os.walk(mydir):
for f in files:
if re.match("OUTCAR*", f):
try:
row = []
fullpath = os.path.join(parent, f)
outcar = Outcar(fullpath)
mags = outcar.magnetization
mags = [m["tot"] for m in mags]
all_ions = xrange(len(mags))
row.append(fullpath.lstrip("./"))
if ion_list:
all_ions = ion_list
for ion in all_ions:
row.append(str(mags[ion]))
data.append(row)
if len(all_ions) > max_row:
max_row = len(all_ions)
except:
pass
for d in data:
if len(d) < max_row + 1:
d.extend([""] * (max_row + 1 - len(d)))
headers = ["Filename"]
for i in xrange(max_row):
headers.append(str(i))
print str_aligned(data, headers)
def get_energies(rootdir, reanalyze, verbose, pretty, detailed, sort):
if verbose:
FORMAT = "%(relativeCreated)d msecs : %(message)s"
logging.basicConfig(level=logging.INFO, format=FORMAT)
if not detailed:
drone = SimpleVaspToComputedEntryDrone(inc_structure=True)
else:
drone = VaspToComputedEntryDrone(
inc_structure=True, data=["filename", "initial_structure"])
ncpus = multiprocessing.cpu_count()
logging.info("Detected {} cpus".format(ncpus))
queen = BorgQueen(drone, number_of_drones=ncpus)
if os.path.exists(save_file) and not reanalyze:
msg = "Using previously assimilated data from {}.".format(save_file) \
+ " Use -f to force re-analysis."
queen.load_data(save_file)
else:
if ncpus > 1:
queen.parallel_assimilate(rootdir)
else:
queen.serial_assimilate(rootdir)
msg = "Analysis results saved to {} for faster ".format(save_file) + \
"subsequent loading."
queen.save_data(save_file)
entries = queen.get_data()
if sort == "energy_per_atom":
entries = sorted(entries, key=lambda x: x.energy_per_atom)
elif sort == "filename":
entries = sorted(entries, key=lambda x: x.data["filename"])
all_data = []
for e in entries:
if not detailed:
delta_vol = "{:.2f}".format(e.data["delta_volume"] * 100)
else:
delta_vol = e.structure.volume / \
e.data["initial_structure"].volume - 1
delta_vol = "{:.2f}".format(delta_vol * 100)
all_data.append(
(e.data["filename"].replace("./", ""),
re.sub("\s+", "",
e.composition.formula), "{:.5f}".format(e.energy),
"{:.5f}".format(e.energy_per_atom), delta_vol))
if len(all_data) > 0:
headers = ("Directory", "Formula", "Energy", "E/Atom", "% vol chg")
if pretty:
from prettytable import PrettyTable
t = PrettyTable(headers)
t.set_field_align("Directory", "l")
map(t.add_row, all_data)
print t
else:
print str_aligned(all_data, headers)
print msg
else:
print "No valid vasp run found."
def test_str_aligned_delimited(self):
data = [["a", "bb"], ["ccc", "dddd"]]
ans = """ a bb
ccc dddd"""
self.assertEqual(str_aligned(data), ans)
self.assertEqual(str_aligned(data, header=["X", "Y"]),
' X Y\n----------\n a bb\nccc dddd')
self.assertEqual(str_delimited(data), 'a\tbb\nccc\tdddd')
def test_str_aligned_delimited(self):
data = [["a", "bb"], ["ccc", "dddd"]]
ans = """ a bb
ccc dddd"""
self.assertEqual(str_aligned(data), ans)
self.assertEqual(str_aligned(data, header=["X", "Y"]),
' X Y\n----------\n a bb\nccc dddd')
self.assertEqual(str_delimited(data), 'a\tbb\nccc\tdddd')
def get_string(self, pretty=False):
"""
Returns a string representation of self. The reason why this
method is different from the __str__ method is to provide options for pretty printing.
Args:
pretty:
Set to True for pretty aligned output.
"""
lines = []
app = lines.append
# Write the Abinit objects first.
for obj in self.abiobjects:
app([80*"#", ""])
app(["#", "%s" % obj.__class__.__name__])
app([80*"#", ""])
for (k, v) in obj.to_abivars().items():
app(self._format_kv(k, v))
# Extra variables.
if self.extra_abivars:
app([80*"#", ""])
app(["#", "Extra_Abivars"])
app([80*"#", ""])
for (k, v) in self.extra_abivars.items():
app(self._format_kv(k, v))
if pretty:
return str_aligned(lines, header=None)
else:
return str_delimited(lines, header=None, delimiter=5*" ")
def get_string(self, sort_keys=False, pretty=False):
"""
Returns a string representation of the INCAR. The reason why this
method is different from the __str__ method is to provide options for
pretty printing.
Args:
sort_keys:
Set to True to sort the INCAR parameters alphabetically.
Defaults to False.
pretty:
Set to True for pretty aligned output. Defaults to False.
"""
keys = self.keys()
if sort_keys:
keys = sorted(keys)
lines = []
for k in keys:
if k == "MAGMOM" and isinstance(self[k], list):
value = []
for m, g in itertools.groupby(self[k]):
value.append("{}*{}".format(len(tuple(g)), m))
lines.append([k, " ".join(value)])
elif isinstance(self[k], list):
lines.append([k, " ".join([str(i) for i in self[k]])])
else:
lines.append([k, self[k]])
if pretty:
return str_aligned(lines)
else:
return str_delimited(lines, None, " = ")
def get_string(self, sort_keys=True, pretty=True):
"""
Returns a string representation of the Feff_tag file. The reason why
this method is different from the __str__ method is to provide options
for pretty printing.
Args:
sort_keys: Set to True to sort the Feff parameters alphabetically.
Defaults to False.
pretty: Set to True for pretty aligned output, False for no.
Returns:
String representation of FeffTags.
"""
keys = self.keys()
if sort_keys:
keys = sorted(keys)
lines = []
for k in keys:
if isinstance(self[k], list):
lines.append([k, " ".join([str(i) for i in self[k]])])
else:
lines.append([k, self[k]])
if pretty:
return str_aligned(lines)
else:
return str_delimited(lines, None, " ")
def get_string(self, pretty=False):
"""
Returns a string representation of self. The reason why this
method is different from the __str__ method is to provide options for pretty printing.
Args:
pretty:
Set to True for pretty aligned output.
"""
lines = []
app = lines.append
# Write the Abinit objects first.
for obj in self.abiobjects:
app([80 * "#", ""])
app(["#", "%s" % obj.__class__.__name__])
app([80 * "#", ""])
for (k, v) in obj.to_abivars().items():
app(self._format_kv(k, v))
# Extra variables.
if self.extra_abivars:
app([80 * "#", ""])
app(["#", "Extra_Abivars"])
app([80 * "#", ""])
for (k, v) in self.extra_abivars.items():
app(self._format_kv(k, v))
if pretty:
return str_aligned(lines, header=None)
else:
return str_delimited(lines, header=None, delimiter=5 * " ")
def get_string(self, sort_keys=True, pretty=True):
"""
Returns a string representation of the Feff_tag file. The reason why
this method is different from the __str__ method is to provide options
for pretty printing.
Args:
sort_keys: Set to True to sort the Feff parameters alphabetically.
Defaults to False.
pretty: Set to True for pretty aligned output, False for no.
Returns:
String representation of FeffTags.
"""
keys = self.keys()
if sort_keys:
keys = sorted(keys)
lines = []
for k in keys:
if isinstance(self[k], list):
lines.append([k, " ".join([str(i) for i in self[k]])])
else:
lines.append([k, self[k]])
if pretty:
return str_aligned(lines)
else:
return str_delimited(lines, None, " ")
def get_energies(rootdir, reanalyze):
FORMAT = "%(relativeCreated)d msecs : %(message)s"
logging.basicConfig(level=logging.INFO, format=FORMAT)
drone = VaspToComputedEntryDrone(inc_structure=True, data=['filename'])
ncpus = multiprocessing.cpu_count()
logging.info('Detected {} cpus'.format(ncpus))
queen = BorgQueen(drone, number_of_drones=ncpus)
if os.path.exists('vasp_analyzer_data.gz') and not reanalyze:
logging.info('Using previously assimilated data file vasp_analyzer_data.gz. Use -f to force re-analysis')
queen.load_data('vasp_analyzer_data.gz')
else:
queen.parallel_assimilate(rootdir)
queen.save_data('vasp_analyzer_data.gz')
entries = queen.get_assimilated_data()
entries = sorted(entries, key=lambda x:x.data['filename'])
all_data = [(e.data['filename'].replace("./", ""), e.composition.formula, "{:.5f}".format(e.energy), "{:.5f}".format(e.energy_per_atom), "{:.2f}".format(e.structure.volume)) for e in entries]
print str_aligned(all_data, ("Directory", "Formula", "Energy", "E/Atom", "Vol"))
def get_energies(rootdir, reanalyze, verbose, pretty):
if verbose:
FORMAT = "%(relativeCreated)d msecs : %(message)s"
logging.basicConfig(level=logging.INFO, format=FORMAT)
drone = GaussianToComputedEntryDrone(inc_structure=True,
parameters=['filename'])
ncpus = multiprocessing.cpu_count()
logging.info('Detected {} cpus'.format(ncpus))
queen = BorgQueen(drone, number_of_drones=ncpus)
if os.path.exists(save_file) and not reanalyze:
msg = 'Using previously assimilated data from {}. ' + \
'Use -f to force re-analysis'.format(save_file)
queen.load_data(save_file)
else:
queen.parallel_assimilate(rootdir)
msg = 'Results saved to {} for faster reloading.'.format(save_file)
queen.save_data(save_file)
entries = queen.get_data()
entries = sorted(entries, key=lambda x: x.parameters['filename'])
all_data = [(e.parameters['filename'].replace("./", ""),
re.sub("\s+", "", e.composition.formula),
"{}".format(e.parameters['charge']),
"{}".format(e.parameters['spin_mult']),
"{:.5f}".format(e.energy), "{:.5f}".format(e.energy_per_atom),
) for e in entries]
headers = ("Directory", "Formula", "Charge", "Spin Mult.", "Energy",
"E/Atom")
if pretty:
from prettytable import PrettyTable
t = PrettyTable(headers)
t.set_field_align("Directory", "l")
map(t.add_row, all_data)
print t
else:
print str_aligned(all_data, headers)
print msg
def get_string(self, radius=10.):
"""
Returns a string representation of atomic shell coordinates to be used
in the feff.inp file.
Args:
radius:
Maximum atomic shell radius to include in atoms list
Returns:
String representation of Atomic Coordinate Shells.
"""
nopts = len(self.struct.species)
ptatoms = []
for i in range(0, nopts):
ptatoms.append(self.struct.species[i].symbol)
index = ptatoms.index(self.central_atom)
pt = self.struct.cart_coords[index]
sphere = Structure.get_sites_in_sphere(self.struct, pt, radius)
xshift = pt[0]
yshift = pt[1]
zshift = pt[2]
end = len(sphere)
row = []
for i in range(end):
atom = sphere[i][0]
atm = re.sub(r"[^aA-zZ]+", "", atom.species_string)
ipot = self.pot_dict[atm]
x = atom.coords[0] - xshift
y = atom.coords[1] - yshift
z = atom.coords[2] - zshift
distance = sphere[i][1]
row.append(["{:f}".format(x), "{:f}".format(y), "{:f}".format(z),
ipot, atm, "{:f}".format(distance), i])
row_sorted = sorted(row, key=itemgetter(5))
row_sorted[0][3] = 0
for i in range(end):
row_sorted[i][6] = i
row_sorted = str_aligned(row_sorted, ["* x", "y", "z", "ipot",
"Atom", "Distance", "Number"])
atom_list = row_sorted.replace("--", "**")
return ''.join(["ATOMS\n", atom_list, "\nEND\n"])
def __str__(self):
"""
Returns a string representation of potential parameters to be used in
the feff.inp file,
determined from structure object.
The lines are arranged as follows:
ipot Z element lmax1 lmax2 stoichometry spinph
Returns:
String representation of Atomic Coordinate Shells.
"""
noelements = len(self.struct.composition.items())
nopts = len(self.struct.species)
ptatoms = []
for i in range(0, nopts):
ptatoms.append(self.struct.species[i].symbol)
index = ptatoms.index(self.central_atom)
center = self.struct.species[index]
cs = center.symbol
cz = center.Z
ipotrow = [[0, cz, cs, -1, -1, .0001, 0]]
for i in range(0, noelements):
center = list(self.struct.composition.items())[i][0]
cs = center.symbol
cz = center.Z
ipot = self.pot_dict[cs]
stoic = list(self.struct.composition.items())[i][1]
ipotrow.append([ipot, cz, cs, -1, -1, stoic, 0])
ipot_sorted = sorted(ipotrow, key=itemgetter(0))
ipotrow = str_aligned(ipot_sorted, [
"*ipot", "Z", "tag", "lmax1", "lmax2", "xnatph(stoichometry)",
"spinph"
])
ipotlist = ipotrow.replace("--", "**")
ipotlist = ''.join(["POTENTIALS\n", ipotlist])
return ipotlist
def get_string(self, pretty=False):
"""
Returns a string representation of self. The reason why this
method is different from the __str__ method is to provide options for pretty printing.
Args:
pretty: Set to True for pretty aligned output.
"""
lines = []
app = lines.append
# extra_abivars can contain variables that are already defined
# in the object. In this case, the value in extra_abivars is used
# TODO: Should find a more elegant way to avoid collission between objects
# and extra_abivars
extra_abivars = self.extra_abivars.copy()
# Write the Abinit objects first.
for obj in self.abiobjects:
#print(obj)
app([80*"#", ""])
app(["#", "%s" % obj.__class__.__name__])
app([80*"#", ""])
for (k, v) in obj.to_abivars().items():
v = extra_abivars.pop(k, v)
app(self._format_kv(k, v))
# Extra variables.
if self.extra_abivars:
app([80*"#", ""])
app(["#", "Extra_Abivars"])
app([80*"#", ""])
for (k, v) in extra_abivars.items():
app(self._format_kv(k, v))
#lines = self._cut_lines(lines)
if pretty:
return str_aligned(lines, header=None)
else:
return str_delimited(lines, header=None, delimiter=5*" ")
def __str__(self):
"""
Returns a string representation of potential parameters to be used in
the feff.inp file,
determined from structure object.
The lines are arranged as follows:
ipot Z element lmax1 lmax2 stoichometry spinph
Returns:
String representation of Atomic Coordinate Shells.
"""
noelements = len(self.struct.composition.items())
nopts = len(self.struct.species)
ptatoms = []
for i in range(0, nopts):
ptatoms.append(self.struct.species[i].symbol)
index = ptatoms.index(self.central_atom)
center = self.struct.species[index]
cs = center.symbol
cz = center.Z
ipotrow = [[0, cz, cs, -1, -1, .0001, 0]]
for i in range(0, noelements):
center = self.struct.composition.items()[i][0]
cs = center.symbol
cz = center.Z
ipot = self.pot_dict[cs]
stoic = self.struct.composition.items()[i][1]
ipotrow.append([ipot, cz, cs, -1, -1, stoic, 0])
ipot_sorted = sorted(ipotrow, key=itemgetter(0))
ipotrow = str_aligned(ipot_sorted, ["*ipot", "Z", "tag", "lmax1",
"lmax2", "xnatph(stoichometry)",
"spinph"])
ipotlist = ipotrow.replace("--", "**")
ipotlist = ''.join(["POTENTIALS\n", ipotlist])
return ipotlist
Last updated: Oct 26 2011''')
parser.add_argument('incar_file', metavar='filename', type=str, nargs=2,
help='files to process')
args = parser.parse_args()
filepath1 = args.incar_file[0]
filepath2 = args.incar_file[1]
incar1 = Incar.from_file(filepath1)
incar2 = Incar.from_file(filepath2)
def format_lists(v):
if isinstance(v, (tuple, list)):
return " ".join(["%d*%.2f" % (len(tuple(group)), i)
for (i, group) in itertools.groupby(v)])
return v
d = incar1.diff(incar2)
output = [['SAME PARAMS', '', '']]
output.append(['---------------', '', ''])
output.extend([(k, format_lists(d['Same'][k]), format_lists(d['Same'][k]))
for k in sorted(d['Same'].keys()) if k != "SYSTEM"])
output.append(['', '', ''])
output.append(['DIFFERENT PARAMS', '', ''])
output.append(['----------------', '', ''])
output.extend([(k, format_lists(d['Different'][k]['INCAR1']),
format_lists(d['Different'][k]['INCAR2']))
for k in sorted(d['Different'].keys()) if k != "SYSTEM"])
print str_aligned(output, ['', filepath1, filepath2])
args = parser.parse_args()
filepath1 = args.incar_file[0]
filepath2 = args.incar_file[1]
incar1 = Incar.from_file(filepath1)
incar2 = Incar.from_file(filepath2)
def format_lists(v):
if isinstance(v, (tuple, list)):
return " ".join([
"%d*%.2f" % (len(tuple(group)), i)
for (i, group) in itertools.groupby(v)
])
return v
d = incar1.diff(incar2)
output = [['SAME PARAMS', '', '']]
output.append(['---------------', '', ''])
output.extend([(k, format_lists(d['Same'][k]), format_lists(d['Same'][k]))
for k in sorted(d['Same'].keys()) if k != "SYSTEM"])
output.append(['', '', ''])
output.append(['DIFFERENT PARAMS', '', ''])
output.append(['----------------', '', ''])
output.extend([(k, format_lists(d['Different'][k]['INCAR1']),
format_lists(d['Different'][k]['INCAR2']))
for k in sorted(d['Different'].keys()) if k != "SYSTEM"])
print str_aligned(output, ['', filepath1, filepath2])
def get_string(self, radius=10.):
"""
Returns a string representation of atomic shell coordinates to be used
in the feff.inp file.
Args:
radius: Maximum atomic shell radius to include in atoms list
Returns:
String representation of Atomic Coordinate Shells.
"""
#Internal variables:
#
#nopts = number of potentials in unit cell used
#ptatoms = list of atom potential atom symbols in unit cell
#index = index number of absorbing atom in list
#pt = coordinates of absorbing atom
#sphere = sites around absorbing atom within radius
#x,y,zshift = coordinate shift to place absorbing atom at (0,0,0)
#atom = site in sphere
#atm = atomic symbol string for atom at atom site
#ipot = index for that atom symbol in potential dictionary
#distance = distance of that atom site from absorbing atom
nopts = len(self.struct.species)
ptatoms = [self.struct.species[i].symbol for i in range(nopts)]
index = ptatoms.index(self.central_atom)
pt = self.struct.cart_coords[index]
sphere = Structure.get_sites_in_sphere(self.struct, pt, radius)
xshift = pt[0]
yshift = pt[1]
zshift = pt[2]
end = len(sphere)
row = []
for i in range(end):
atom = sphere[i][0]
atm = re.sub(r"[^aA-zZ]+", "", atom.species_string)
ipot = self.pot_dict[atm]
x = atom.coords[0] - xshift
y = atom.coords[1] - yshift
z = atom.coords[2] - zshift
distance = sphere[i][1]
row.append([
"{:f}".format(x), "{:f}".format(y), "{:f}".format(z), ipot,
atm, "{:f}".format(distance), i
])
#after this point table is built
row_sorted = sorted(row, key=itemgetter(5))
row_sorted[0][3] = 0
for i in range(end):
row_sorted[i][6] = i
row_sorted = str_aligned(
row_sorted,
["* x", "y", "z", "ipot", "Atom", "Distance", "Number"])
atom_list = row_sorted.replace("--", "**")
return ''.join(["ATOMS\n", atom_list, "\nEND\n"])
def get_string(self, radius=10.):
"""
Returns a string representation of atomic shell coordinates to be used
in the feff.inp file.
Args:
radius: Maximum atomic shell radius to include in atoms list
Returns:
String representation of Atomic Coordinate Shells.
"""
#Internal variables:
#
#nopts = number of potentials in unit cell used
#ptatoms = list of atom potential atom symbols in unit cell
#index = index number of absorbing atom in list
#pt = coordinates of absorbing atom
#sphere = sites around absorbing atom within radius
#x,y,zshift = coordinate shift to place absorbing atom at (0,0,0)
#atom = site in sphere
#atm = atomic symbol string for atom at atom site
#ipot = index for that atom symbol in potential dictionary
#distance = distance of that atom site from absorbing atom
nopts = len(self.struct.species)
ptatoms = [self.struct.species[i].symbol for i in range(nopts)]
index = ptatoms.index(self.central_atom)
pt = self.struct.cart_coords[index]
sphere = Structure.get_sites_in_sphere(self.struct, pt, radius)
xshift = pt[0]
yshift = pt[1]
zshift = pt[2]
end = len(sphere)
row = []
for i in range(end):
atom = sphere[i][0]
atm = re.sub(r"[^aA-zZ]+", "", atom.species_string)
ipot = self.pot_dict[atm]
x = atom.coords[0] - xshift
y = atom.coords[1] - yshift
z = atom.coords[2] - zshift
distance = sphere[i][1]
row.append(["{:f}".format(x), "{:f}".format(y), "{:f}".format(z),
ipot, atm, "{:f}".format(distance), i])
#after this point table is built
row_sorted = sorted(row, key=itemgetter(5))
row_sorted[0][3] = 0
for i in range(end):
row_sorted[i][6] = i
row_sorted = str_aligned(row_sorted, ["* x", "y", "z", "ipot",
"Atom", "Distance", "Number"])
atom_list = row_sorted.replace("--", "**")
return ''.join(["ATOMS\n", atom_list, "\nEND\n"])
