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pwlog2trajectory
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pwlog2trajectory
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#!/usr/bin/env python
#****************************************************************************
# Copyright (C) 2013 SUNCAT
# This file is distributed under the terms of the
# GNU General Public License. See the file `COPYING'
# in the root directory of the present distribution,
# or http://www.gnu.org/copyleft/gpl.txt .
#****************************************************************************
from sys import argv, exit, stderr
if len(argv) != 3:
print >>stderr, 'usage: ' + argv[0] + ' pw-log output.traj'
exit(1)
import numpy as np
from ase.io import PickleTrajectory
from ase import Atoms
from os import popen
import ase.units
hartree = ase.units.Hartree
rydberg = ase.units.Rydberg
bohr = ase.units.Bohr
def get_total_energy(s):
a = s.readline()
while a != '' and a[:17] != '! total energy':
a = s.readline()
if a == '':
return None
energy = float(a.split()[-2]) * rydberg
for i in range(11):
a = s.readline()
if ' smearing contrib.' in a:
break
# correct for finite temperature entropy term
# in case of finite temp. smearing
if a[:22] == ' smearing contrib.':
energy -= 0.5 * float(a.split()[-2]) * rydberg
return energy
# dummy calculator
class calculator:
def set_energy(self, e):
self.energy = e
def get_potential_energy(self):
return self.energy
def get_calculator(self):
return self
def notimpl(self, apply_constraint=False):
raise NotImplementedError
p = popen('grep -n Giannozzi ' + argv[1] + ' 2>/dev/null | tail -1', 'r')
try:
n = int(p.readline().split()[0].strip(':'))
except:
print >>stderr, 'No valid pw-log at ' + argv[1] + ' found.'
p.close()
exit(2)
p.close()
calc = calculator()
s = open(argv[1], 'r')
# skip over previous runs in log in case the current log has been
# appended to old ones
for i in range(n):
s.readline()
a = s.readline()
while a[:11] != ' celldm':
a = s.readline()
alat = float(a.split()[1]) / 1.889726
a = s.readline()
while a[:12] != ' crystal':
a = s.readline()
cell = []
for i in range(3):
cell.append([float(x) for x in s.readline().split()[3:6]])
cell = np.array(cell)
a = s.readline()
while a[:12] != ' site n.':
a = s.readline()
pos = []
syms = ''
y = s.readline().split()
while len(y) > 0:
nf = len(y)
pos.append([float(x) for x in y[nf - 4:nf - 1]])
syms += y[1].strip('0123456789')
y = s.readline().split()
pos = np.array(pos) * alat
natoms = len(pos)
# create atoms object with coordinates and unit cell
# as specified in the initial ionic step in log
atoms = Atoms(syms, pos, cell=cell * alat, pbc=(1, 1, 1))
atoms.get_calculator = calc.get_calculator
atoms.get_potential_energy = calc.get_potential_energy
atoms.get_forces = calc.notimpl
atoms.get_stress = calc.notimpl
atoms.get_charges = calc.notimpl
# get total energy at first ionic step
en = get_total_energy(s)
if en is not None:
calc.set_energy(en)
else:
print >>stderr, 'no total energy found'
exit(3)
print(atoms)
traj = PickleTrajectory(argv[2], 'w')
traj.write(atoms)
a = s.readline()
while a != '':
while a[:7] != 'CELL_PA' and a[:7] != 'ATOMIC_' and a != '':
a = s.readline()
if a == '':
break
if a[0] == 'A':
coord = a.split('(')[-1]
for i in range(natoms):
pos[i][:] = s.readline().split()[1:4]
if coord == 'alat)':
atoms.set_positions(pos * alat)
elif coord == 'bohr)':
atoms.set_positions(pos * bohr)
elif coord == 'angstrom)':
atoms.set_positions(pos)
else:
atoms.set_scaled_positions(pos)
# get total energy at 2nd,3rd,...nth ionic step
en = get_total_energy(s)
calc.set_energy(en)
if en is not None:
traj.write(atoms)
else:
break
else:
for i in range(3):
cell[i][:] = s.readline().split()
atoms.set_cell(cell * alat, scale_atoms=False)
a = s.readline()