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dft_tools/python/vasp/plotools.py

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import itertools as it
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import numpy as np
from proj_group import ProjectorGroup
from proj_shell import ProjectorShell
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np.set_printoptions(suppress=True)
# 'simplejson' is supposed to be faster than 'json' in stdlib.
try:
import simplejson as json
except ImportError:
import json
def issue_warning(message):
"""
Issues a warning.
"""
print
print " !!! WARNING !!!: " + message
print
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################################################################################
# check_data_consistency()
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################################################################################
def check_data_consistency(pars, el_struct):
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"""
Check the consistency of the VASP data.
"""
# Check that ions inside each shell are of the same sort
for sh in pars.shells:
assert max(sh['ion_list']) <= el_struct.natom, "Site index in the projected shell exceeds the number of ions in the structure"
sorts = set([el_struct.type_of_ion[io] for io in sh['ion_list']])
assert len(sorts) == 1, "Each projected shell must contain only ions of the same sort"
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# Check that ion and orbital lists in shells match those of projectors
ion_list = sh['ion_list']
lshell = sh['lshell']
for ion in ion_list:
for par in el_struct.proj_params:
if par['isite'] - 1 == ion and par['l'] == lshell:
break
else:
errmsg = "Projector for isite = %s, l = %s does not match PROJCAR"%(ion + 1, lshell)
raise Exception(errmsg)
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################################################################################
#
# generate_plo()
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#
################################################################################
def generate_plo(conf_pars, el_struct):
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"""
Parameters
----------
conf_pars (dict) : dictionary of input parameters (from conf-file)
el_struct : ElectronicStructure object
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"""
check_data_consistency(conf_pars, el_struct)
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proj_raw = el_struct.proj_raw
try:
efermi = conf_pars.general['efermi']
except (KeyError, AttributeError):
efermi = el_struct.efermi
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# eigvals(nktot, nband, ispin) are defined with respect to the Fermi level
eigvals = el_struct.eigvals - efermi
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nshell = len(conf_pars.shells)
print
print " Generating %i shell%s..."%(nshell, '' if nshell == 1 else 's')
pshells = []
for sh_par in conf_pars.shells:
pshell = ProjectorShell(sh_par, proj_raw, el_struct.proj_params, el_struct.nc_flag)
print
print " Shell : %s"%(pshell.user_index)
print " Orbital l : %i"%(pshell.lorb)
print " Number of ions: %i"%(len(pshell.ion_list))
print " Dimension : %i"%(pshell.ndim)
pshells.append(pshell)
pgroups = []
for gr_par in conf_pars.groups:
pgroup = ProjectorGroup(gr_par, pshells, eigvals)
pgroup.orthogonalize()
print "Density matrix:"
dm_all, ov_all = pshells[pgroup.ishells[0]].density_matrix(el_struct)
nimp = 0.0
for io, dm in enumerate(dm_all[0]):
print " Site %i"%(io + 1)
print dm
ndm = dm.trace()
nimp += ndm
print " trace: ", ndm
print
print " Impurity density:", nimp
print
print "Overlap:"
for io, ov in enumerate(ov_all[0]):
print " Site %i"%(io + 1)
print ov
if 'dosmesh' in conf_pars.general:
print
print "Evaluating DOS..."
mesh_pars = conf_pars.general['dosmesh']
if np.isnan(mesh_pars['emin']):
dos_emin = pgroup.emin
dos_emax = pgroup.emax
else:
dos_emin = mesh_pars['emin']
dos_emax = mesh_pars['emax']
n_points = mesh_pars['n_points']
emesh = np.linspace(dos_emin, dos_emax, n_points)
dos = pshells[pgroup.ishells[0]].density_of_states(el_struct, emesh)
de = emesh[1] - emesh[0]
ntot = (dos[1:,...] + dos[:-1,...]).sum(0) / 2 * de
print " Total number of states:", ntot
for io in xrange(dos.shape[2]):
np.savetxt('pdos_%i.dat'%(io), np.vstack((emesh.T, dos[:, 0, io, :].T)).T)
pgroups.append(pgroup)
return pshells, pgroups
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# TODO: k-points with weights should be stored once and for all
################################################################################
#
# kpoints_output
#
################################################################################
def kpoints_output(basename, el_struct):
"""
Outputs k-point data into a text file.
"""
kmesh = el_struct.kmesh
fname = basename + '.kpoints'
with open(fname, 'wt') as f:
f.write("# Number of k-points: nktot\n")
nktot = kmesh['nktot']
f.write("%i\n"%(nktot))
# TODO: add the output of reciprocal lattice vectors
f.write("# List of k-points with weights\n")
for ik in xrange(nktot):
kx, ky, kz = kmesh['kpoints'][ik, :]
kwght = kmesh['kweights'][ik]
f.write("%15.10f%15.10f%15.10f%20.10f\n"%(kx, ky, kz, kwght))
# Check if there are tetrahedra defined and if they are, output them
try:
ntet = kmesh['ntet']
volt = kmesh['volt']
f.write("\n# Number of tetrahedra and volume: ntet, volt\n")
f.write("%i %s\n"%(ntet, volt))
f.write("# List of tetrahedra: imult, ik1, ..., ik4\n")
for it in xrange(ntet):
f.write(' '.join(map("{0:d}".format, *kmesh['itet'][it, :])) + '\n')
except KeyError:
pass
################################################################################
#
# ctrl_output
#
################################################################################
def ctrl_output(conf_pars, el_struct, ng):
"""
Outputs a ctrl-file.
"""
ctrl_fname = conf_pars.general['basename'] + '.ctrl'
head_dict = {}
# TODO: Add output of tetrahedra
# Construct the header dictionary
head_dict['ngroups'] = ng
head_dict['nk'] = el_struct.kmesh['nktot']
head_dict['ns'] = el_struct.nspin
head_dict['nc_flag'] = 1 if el_struct.nc_flag else 0
# head_dict['efermi'] = conf_pars.general['efermi'] # We probably don't need Efermi
header = json.dumps(head_dict, indent=4, separators=(',', ': '))
print " Storing ctrl-file..."
with open(ctrl_fname, 'wt') as f:
f.write(header + "\n")
f.write("#END OF HEADER\n")
f.write("# k-points and weights\n")
labels = ['kx', 'ky', 'kz', 'kweight']
out = "".join(map(lambda s: s.center(15), labels))
f.write("#" + out + "\n")
for ik, kp in enumerate(el_struct.kmesh['kpoints']):
tmp1 = "".join(map("{0:15.10f}".format, kp))
out = tmp1 + "{0:16.10f}".format(el_struct.kmesh['kweights'][ik])
f.write(out + "\n")
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################################################################################
#
# plo_output
#
################################################################################
def plo_output(conf_pars, el_struct, pshells, pgroups):
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"""
Outputs PLO groups into text files.
Filenames are defined by <basename> that is passed from config-file.
All necessary general parameters are stored in a file '<basename>.ctrl'.
Each group is stored in a '<basename>.plog<Ng>' file. The format is the
following:
# Energy window: emin, emax
ib_min, ib_max
nelect
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# Eigenvalues
isp, ik1, kx, ky, kz, kweight
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ib1, ib2
eig1
eig2
...
eigN
ik2, kx, ky, kz, kweight
...
# Projected shells
Nshells
# Shells: <shell indices>
# Shell <1>
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Shell 1
ndim
# complex arrays: plo(ns, nion, ndim, nb)
...
# Shells: <shell indices>
# Shell <2>
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Shell 2
...
"""
for ig, pgroup in enumerate(pgroups):
plo_fname = conf_pars.general['basename'] + '.pg%i'%(ig + 1)
print " Storing PLO-group file '%s'..."%(plo_fname)
head_dict = {}
head_dict['ewindow'] = (pgroup.emin, pgroup.emax)
head_dict['nb_max'] = pgroup.nb_max
# Number of electrons within the window
head_dict['nelect'] = pgroup.nelect_window(el_struct)
print " Density within window:", head_dict['nelect']
head_shells = []
for ish in pgroup.ishells:
shell = pgroup.shells[ish]
sh_dict = {}
sh_dict['shell_index'] = ish
sh_dict['lorb'] = shell.lorb
sh_dict['ndim'] = shell.ndim
# Convert ion indices from the internal representation (starting from 0)
# to conventional VASP representation (starting from 1)
ion_output = [io + 1 for io in shell.ion_list]
sh_dict['ion_list'] = ion_output
sh_dict['ion_sort'] = el_struct.type_of_ion[shell.ion_list[0]]
# TODO: add the output of transformation matrices
head_shells.append(sh_dict)
head_dict['shells'] = head_shells
header = json.dumps(head_dict, indent=4, separators=(',', ': '))
with open(plo_fname, 'wt') as f:
f.write(header + "\n")
f.write("#END OF HEADER\n")
# Eigenvalues within the window
f.write("# Eigenvalues within the energy window: %s, %s\n"%(pgroup.emin, pgroup.emax))
nk, nband, ns_band = el_struct.eigvals.shape
for isp in xrange(ns_band):
f.write("# is = %i\n"%(isp + 1))
for ik in xrange(nk):
ib1, ib2 = pgroup.ib_win[ik, isp, 0], pgroup.ib_win[ik, isp, 1]
f.write(" %i %i\n"%(ib1, ib2))
for ib in xrange(ib1, ib2 + 1):
eigv_ef = el_struct.eigvals[ik, ib, isp] - el_struct.efermi
f_weight = el_struct.ferw[isp, ik, ib]
f.write("%13.8f %12.7f\n"%(eigv_ef, f_weight))
# Projected shells
f.write("# Projected shells\n")
f.write("# Shells: %s\n"%(pgroup.ishells))
for ish in pgroup.ishells:
shell = pgroup.shells[ish]
f.write("# Shell %i\n"%(ish))
nion, ns, nk, nlm, nb = shell.proj_win.shape
for isp in xrange(ns):
f.write("# is = %i\n"%(isp + 1))
for ik in xrange(nk):
f.write("# ik = %i\n"%(ik + 1))
for ion in xrange(nion):
for ilm in xrange(nlm):
ib1, ib2 = pgroup.ib_win[ik, isp, 0], pgroup.ib_win[ik, isp, 1]
ib_win = ib2 - ib1 + 1
for ib in xrange(ib_win):
p = shell.proj_win[ion, isp, ik, ilm, ib]
f.write("{0:16.10f}{1:16.10f}\n".format(p.real, p.imag))
f.write("\n")
################################################################################
#
# output_as_text
#
################################################################################
def output_as_text(pars, el_struct, pshells, pgroups):
"""
Output all information necessary for the converter as text files.
"""
ctrl_output(pars, el_struct, len(pgroups))
plo_output(pars, el_struct, pshells, pgroups)