def start(self, name):
Timer.start(self, name)
if name in self.regions:
id = self.regions[name]
else:
id = self.region_id
self.regions[name] = id
self.region_id += 1
self.craypat_region_begin(id, name)
def start(self, name):
Timer.start(self, name)
if name in self.regions:
id = self.regions[name]
else:
id = self.region_id
self.regions[name] = id
self.region_id += 1
self.craypat_region_begin(id, name)
def test_inv_speed(self):
full_mat = self.recover()
timer = Timer()
timer.start('full_numpy')
tmp0 = np.linalg.inv(full_mat)
timer.stop('full_numpy')
timer.start('full_lapack')
inverse_general(full_mat)
timer.stop('full_lapack')
timer.start('sparse_lapack')
self.inv_eq()
timer.stop('sparse_lapack')
timer.start('sparse_lapack_ne')
self.inv_ne()
timer.stop('sparse_lapack_ne')
times = []
methods = ['full_numpy', 'full_lapack', 'sparse_lapack']
for name in methods:
time = timer.timers[name,]
print(name, time)
times.append(time)
mintime = np.min(times)
self.inv_method = methods[np.argmin(times)]
print('mintime', mintime)
print('sparse_lapack_ne', timer.timers['sparse_lapack_ne',])
def start(self, name):
Timer.start(self, name)
self.tau_timers[name] = self.pytau.profileTimer(name)
self.pytau.start(self.tau_timers[name])
class GPAW(Calculator, PAW):
"""This is the ASE-calculator frontend for doing a PAW calculation."""
implemented_properties = [
'energy', 'forces', 'stress', 'dipole', 'magmom', 'magmoms'
]
default_parameters = {
'mode': 'fd',
'xc': 'LDA',
'occupations': None,
'poissonsolver': None,
'h': None, # Angstrom
'gpts': None,
'kpts': [(0.0, 0.0, 0.0)],
'nbands': None,
'charge': 0,
'setups': {},
'basis': {},
'spinpol': None,
'fixdensity': False,
'filter': None,
'mixer': None,
'eigensolver': None,
'background_charge': None,
'external': None,
'random': False,
'hund': False,
'maxiter': 333,
'idiotproof': True,
'symmetry': {
'point_group': True,
'time_reversal': True,
'symmorphic': True,
'tolerance': 1e-7
},
'convergence': {
'energy': 0.0005, # eV / electron
'density': 1.0e-4,
'eigenstates': 4.0e-8, # eV^2
'bands': 'occupied',
'forces': np.inf
}, # eV / Ang
'dtype': None, # Deprecated
'width': None, # Deprecated
'verbose': 0
}
default_parallel = {
'kpt': None,
'domain': gpaw.parsize_domain,
'band': gpaw.parsize_bands,
'order': 'kdb',
'stridebands': False,
'augment_grids': gpaw.augment_grids,
'sl_auto': False,
'sl_default': gpaw.sl_default,
'sl_diagonalize': gpaw.sl_diagonalize,
'sl_inverse_cholesky': gpaw.sl_inverse_cholesky,
'sl_lcao': gpaw.sl_lcao,
'sl_lrtddft': gpaw.sl_lrtddft,
'buffer_size': gpaw.buffer_size
}
def __init__(self,
restart=None,
ignore_bad_restart_file=False,
label=None,
atoms=None,
timer=None,
communicator=None,
txt='-',
parallel=None,
**kwargs):
self.parallel = dict(self.default_parallel)
if parallel:
self.parallel.update(parallel)
if timer is None:
self.timer = Timer()
else:
self.timer = timer
self.scf = None
self.wfs = None
self.occupations = None
self.density = None
self.hamiltonian = None
self.observers = [] # XXX move to self.scf
self.initialized = False
self.world = communicator
if self.world is None:
self.world = mpi.world
elif not hasattr(self.world, 'new_communicator'):
self.world = mpi.world.new_communicator(np.asarray(self.world))
self.log = GPAWLogger(world=self.world)
self.log.fd = txt
self.reader = None
Calculator.__init__(self, restart, ignore_bad_restart_file, label,
atoms, **kwargs)
def __del__(self):
self.timer.write(self.log.fd)
if self.reader is not None:
self.reader.close()
def write(self, filename, mode=''):
self.log('Writing to {0} (mode={1!r})\n'.format(filename, mode))
writer = Writer(filename, self.world)
self._write(writer, mode)
writer.close()
self.world.barrier()
def _write(self, writer, mode):
from ase.io.trajectory import write_atoms
writer.write(version=1,
gpaw_version=gpaw.__version__,
ha=Ha,
bohr=Bohr)
write_atoms(writer.child('atoms'), self.atoms)
writer.child('results').write(**self.results)
writer.child('parameters').write(**self.todict())
self.density.write(writer.child('density'))
self.hamiltonian.write(writer.child('hamiltonian'))
self.occupations.write(writer.child('occupations'))
self.scf.write(writer.child('scf'))
self.wfs.write(writer.child('wave_functions'), mode == 'all')
return writer
def read(self, filename):
from ase.io.trajectory import read_atoms
self.log('Reading from {0}'.format(filename))
self.reader = reader = Reader(filename)
self.atoms = read_atoms(reader.atoms)
res = reader.results
self.results = dict((key, res.get(key)) for key in res.keys())
if self.results:
self.log('Read {0}'.format(', '.join(sorted(self.results))))
self.log('Reading input parameters:')
self.parameters = self.get_default_parameters()
dct = {}
for key, value in reader.parameters.asdict().items():
if (isinstance(value, dict)
and isinstance(self.parameters[key], dict)):
self.parameters[key].update(value)
else:
self.parameters[key] = value
dct[key] = self.parameters[key]
self.log.print_dict(dct)
self.log()
self.initialize(reading=True)
self.density.read(reader)
self.hamiltonian.read(reader)
self.occupations.read(reader)
self.scf.read(reader)
self.wfs.read(reader)
# We need to do this in a better way: XXX
from gpaw.utilities.partition import AtomPartition
atom_partition = AtomPartition(self.wfs.gd.comm,
np.zeros(len(self.atoms), dtype=int))
self.wfs.atom_partition = atom_partition
self.density.atom_partition = atom_partition
self.hamiltonian.atom_partition = atom_partition
spos_ac = self.atoms.get_scaled_positions() % 1.0
rank_a = self.density.gd.get_ranks_from_positions(spos_ac)
new_atom_partition = AtomPartition(self.density.gd.comm, rank_a)
for obj in [self.density, self.hamiltonian]:
obj.set_positions_without_ruining_everything(
spos_ac, new_atom_partition)
self.hamiltonian.xc.read(reader)
if self.hamiltonian.xc.name == 'GLLBSC':
# XXX GLLB: See lcao/tdgllbsc.py test
self.occupations.calculate(self.wfs)
return reader
def check_state(self, atoms, tol=1e-15):
system_changes = Calculator.check_state(self, atoms, tol)
if 'positions' not in system_changes:
if self.hamiltonian:
if self.hamiltonian.vext:
if self.hamiltonian.vext.vext_g is None:
# QMMM atoms have moved:
system_changes.append('positions')
return system_changes
def calculate(self,
atoms=None,
properties=['energy'],
system_changes=['cell']):
"""Calculate things."""
Calculator.calculate(self, atoms)
atoms = self.atoms
if system_changes:
self.log('System changes:', ', '.join(system_changes), '\n')
if system_changes == ['positions']:
# Only positions have changed:
self.density.reset()
else:
# Drastic changes:
self.wfs = None
self.occupations = None
self.density = None
self.hamiltonian = None
self.scf = None
self.initialize(atoms)
self.set_positions(atoms)
if not self.initialized:
self.initialize(atoms)
self.set_positions(atoms)
if not (self.wfs.positions_set and self.hamiltonian.positions_set):
self.set_positions(atoms)
if not self.scf.converged:
print_cell(self.wfs.gd, self.atoms.pbc, self.log)
with self.timer('SCF-cycle'):
self.scf.run(self.wfs, self.hamiltonian, self.density,
self.occupations, self.log, self.call_observers)
self.log('\nConverged after {0} iterations.\n'.format(
self.scf.niter))
e_free = self.hamiltonian.e_total_free
e_extrapolated = self.hamiltonian.e_total_extrapolated
self.results['energy'] = e_extrapolated * Ha
self.results['free_energy'] = e_free * Ha
if not self.atoms.pbc.all():
dipole_v = self.density.calculate_dipole_moment() * Bohr
self.log(
'Dipole moment: ({0:.6f}, {1:.6f}, {2:.6f}) |e|*Ang\n'.
format(*dipole_v))
self.results['dipole'] = dipole_v
if self.wfs.nspins == 2:
magmom = self.occupations.magmom
magmom_a = self.density.estimate_magnetic_moments(total=magmom)
self.log('Total magnetic moment: %f' % magmom)
self.log('Local magnetic moments:')
symbols = self.atoms.get_chemical_symbols()
for a, mom in enumerate(magmom_a):
self.log('{0:4} {1:2} {2:.6f}'.format(a, symbols[a], mom))
self.log()
self.results['magmom'] = self.occupations.magmom
self.results['magmoms'] = magmom_a
self.summary()
self.call_observers(self.scf.niter, final=True)
if 'forces' in properties:
with self.timer('Forces'):
F_av = calculate_forces(self.wfs, self.density,
self.hamiltonian, self.log)
self.results['forces'] = F_av * (Ha / Bohr)
if 'stress' in properties:
with self.timer('Stress'):
try:
stress = calculate_stress(self).flat[[0, 4, 8, 5, 2, 1]]
except NotImplementedError:
# Our ASE Calculator base class will raise
# PropertyNotImplementedError for us.
pass
else:
self.results['stress'] = stress * (Ha / Bohr**3)
def summary(self):
self.hamiltonian.summary(self.occupations.fermilevel, self.log)
self.density.summary(self.atoms, self.occupations.magmom, self.log)
self.occupations.summary(self.log)
self.wfs.summary(self.log)
self.log.fd.flush()
def set(self, **kwargs):
"""Change parameters for calculator.
Examples::
calc.set(xc='PBE')
calc.set(nbands=20, kpts=(4, 1, 1))
"""
changed_parameters = Calculator.set(self, **kwargs)
for key in ['setups', 'basis']:
if key in changed_parameters:
dct = changed_parameters[key]
if isinstance(dct, dict) and None in dct:
dct['default'] = dct.pop(None)
warnings.warn('Please use {key}={dct}'.format(key=key,
dct=dct))
# We need to handle txt early in order to get logging up and running:
if 'txt' in changed_parameters:
self.log.fd = changed_parameters.pop('txt')
if not changed_parameters:
return {}
self.initialized = False
self.scf = None
self.results = {}
self.log('Input parameters:')
self.log.print_dict(changed_parameters)
self.log()
for key in changed_parameters:
if key in ['eigensolver', 'convergence'] and self.wfs:
self.wfs.set_eigensolver(None)
if key in [
'mixer', 'verbose', 'txt', 'hund', 'random', 'eigensolver',
'idiotproof'
]:
continue
if key in ['convergence', 'fixdensity', 'maxiter']:
continue
# More drastic changes:
if self.wfs:
self.wfs.set_orthonormalized(False)
if key in ['external', 'xc', 'poissonsolver']:
self.hamiltonian = None
elif key in ['occupations', 'width']:
pass
elif key in ['charge', 'background_charge']:
self.hamiltonian = None
self.density = None
self.wfs = None
elif key in ['kpts', 'nbands', 'symmetry']:
self.wfs = None
elif key in ['h', 'gpts', 'setups', 'spinpol', 'dtype', 'mode']:
self.density = None
self.hamiltonian = None
self.wfs = None
elif key in ['basis']:
self.wfs = None
else:
raise TypeError('Unknown keyword argument: "%s"' % key)
def initialize_positions(self, atoms=None):
"""Update the positions of the atoms."""
self.log('Initializing position-dependent things.\n')
if atoms is None:
atoms = self.atoms
else:
# Save the state of the atoms:
self.atoms = atoms.copy()
mpi.synchronize_atoms(atoms, self.world)
spos_ac = atoms.get_scaled_positions() % 1.0
rank_a = self.wfs.gd.get_ranks_from_positions(spos_ac)
atom_partition = AtomPartition(self.wfs.gd.comm, rank_a, name='gd')
self.wfs.set_positions(spos_ac, atom_partition)
self.density.set_positions(spos_ac, atom_partition)
self.hamiltonian.set_positions(spos_ac, atom_partition)
return spos_ac
def set_positions(self, atoms=None):
"""Update the positions of the atoms and initialize wave functions."""
spos_ac = self.initialize_positions(atoms)
nlcao, nrand = self.wfs.initialize(self.density, self.hamiltonian,
spos_ac)
if nlcao + nrand:
self.log('Creating initial wave functions:')
if nlcao:
self.log(' ', plural(nlcao, 'band'), 'from LCAO basis set')
if nrand:
self.log(' ', plural(nrand, 'band'), 'from random numbers')
self.log()
self.wfs.eigensolver.reset()
self.scf.reset()
print_positions(self.atoms, self.log)
def initialize(self, atoms=None, reading=False):
"""Inexpensive initialization."""
self.log('Initialize ...\n')
if atoms is None:
atoms = self.atoms
else:
# Save the state of the atoms:
self.atoms = atoms.copy()
par = self.parameters
natoms = len(atoms)
cell_cv = atoms.get_cell() / Bohr
number_of_lattice_vectors = cell_cv.any(axis=1).sum()
if number_of_lattice_vectors < 3:
raise ValueError(
'GPAW requires 3 lattice vectors. Your system has {0}.'.
format(number_of_lattice_vectors))
pbc_c = atoms.get_pbc()
assert len(pbc_c) == 3
magmom_a = atoms.get_initial_magnetic_moments()
mpi.synchronize_atoms(atoms, self.world)
# Generate new xc functional only when it is reset by set
# XXX sounds like this should use the _changed_keywords dictionary.
if self.hamiltonian is None or self.hamiltonian.xc is None:
if isinstance(par.xc, basestring):
xc = XC(par.xc)
else:
xc = par.xc
else:
xc = self.hamiltonian.xc
mode = par.mode
if isinstance(mode, basestring):
mode = {'name': mode}
if isinstance(mode, dict):
mode = create_wave_function_mode(**mode)
if par.dtype == complex:
warnings.warn('Use mode={0}(..., force_complex_dtype=True) '
'instead of dtype=complex'.format(mode.name.upper()))
mode.force_complex_dtype = True
del par['dtype']
par.mode = mode
if xc.orbital_dependent and mode.name == 'lcao':
raise ValueError('LCAO mode does not support '
'orbital-dependent XC functionals.')
realspace = (mode.name != 'pw' and mode.interpolation != 'fft')
if not realspace:
pbc_c = np.ones(3, bool)
self.create_setups(mode, xc)
magnetic = magmom_a.any()
spinpol = par.spinpol
if par.hund:
if natoms != 1:
raise ValueError('hund=True arg only valid for single atoms!')
spinpol = True
magmom_a[0] = self.setups[0].get_hunds_rule_moment(par.charge)
if spinpol is None:
spinpol = magnetic
elif magnetic and not spinpol:
raise ValueError('Non-zero initial magnetic moment for a ' +
'spin-paired calculation!')
nspins = 1 + int(spinpol)
if spinpol:
self.log('Spin-polarized calculation.')
self.log('Magnetic moment: {0:.6f}\n'.format(magmom_a.sum()))
else:
self.log('Spin-paired calculation\n')
if isinstance(par.background_charge, dict):
background = create_background_charge(**par.background_charge)
else:
background = par.background_charge
nao = self.setups.nao
nvalence = self.setups.nvalence - par.charge
if par.background_charge is not None:
nvalence += background.charge
M = abs(magmom_a.sum())
nbands = par.nbands
orbital_free = any(setup.orbital_free for setup in self.setups)
if orbital_free:
nbands = 1
if isinstance(nbands, basestring):
if nbands[-1] == '%':
basebands = int(nvalence + M + 0.5) // 2
nbands = int((float(nbands[:-1]) / 100) * basebands)
else:
raise ValueError('Integer expected: Only use a string '
'if giving a percentage of occupied bands')
if nbands is None:
nbands = 0
for setup in self.setups:
nbands_from_atom = setup.get_default_nbands()
# Any obscure setup errors?
if nbands_from_atom < -(-setup.Nv // 2):
raise ValueError('Bad setup: This setup requests %d'
' bands but has %d electrons.' %
(nbands_from_atom, setup.Nv))
nbands += nbands_from_atom
nbands = min(nao, nbands)
elif nbands > nao and mode.name == 'lcao':
raise ValueError('Too many bands for LCAO calculation: '
'%d bands and only %d atomic orbitals!' %
(nbands, nao))
if nvalence < 0:
raise ValueError(
'Charge %f is not possible - not enough valence electrons' %
par.charge)
if nbands <= 0:
nbands = int(nvalence + M + 0.5) // 2 + (-nbands)
if nvalence > 2 * nbands and not orbital_free:
raise ValueError('Too few bands! Electrons: %f, bands: %d' %
(nvalence, nbands))
self.create_occupations(magmom_a.sum(), orbital_free)
if self.scf is None:
self.create_scf(nvalence, mode)
self.create_symmetry(magmom_a, cell_cv)
if not self.wfs:
self.create_wave_functions(mode, realspace, nspins, nbands, nao,
nvalence, self.setups, magmom_a,
cell_cv, pbc_c)
else:
self.wfs.set_setups(self.setups)
if not self.wfs.eigensolver:
self.create_eigensolver(xc, nbands, mode)
if self.density is None and not reading:
assert not par.fixdensity, 'No density to fix!'
olddens = None
if (self.density is not None and
(self.density.gd.parsize_c != self.wfs.gd.parsize_c).any()):
# Domain decomposition has changed, so we need to
# reinitialize density and hamiltonian:
if par.fixdensity:
olddens = self.density
self.density = None
self.hamiltonian = None
if self.density is None:
self.create_density(realspace, mode, background)
# XXXXXXXXXX if setups change, then setups.core_charge may change.
# But that parameter was supplied in Density constructor!
# This surely is a bug!
self.density.initialize(self.setups, self.timer, magmom_a, par.hund)
self.density.set_mixer(par.mixer)
if self.density.mixer.driver.name == 'dummy' or par.fixdensity:
self.log('No density mixing\n')
else:
self.log(self.density.mixer, '\n')
self.density.fixed = par.fixdensity
self.density.log = self.log
if olddens is not None:
self.density.initialize_from_other_density(olddens,
self.wfs.kptband_comm)
if self.hamiltonian is None:
self.create_hamiltonian(realspace, mode, xc)
xc.initialize(self.density, self.hamiltonian, self.wfs,
self.occupations)
if xc.name == 'GLLBSC' and olddens is not None:
xc.heeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeelp(olddens)
self.print_memory_estimate(maxdepth=memory_estimate_depth + 1)
print_parallelization_details(self.wfs, self.density, self.log)
self.log('Number of atoms:', natoms)
self.log('Number of atomic orbitals:', self.wfs.setups.nao)
if self.nbands_parallelization_adjustment != 0:
self.log(
'Adjusting number of bands by %+d to match parallelization' %
self.nbands_parallelization_adjustment)
self.log('Number of bands in calculation:', self.wfs.bd.nbands)
self.log('Bands to converge: ', end='')
n = par.convergence.get('bands', 'occupied')
if n == 'occupied':
self.log('occupied states only')
elif n == 'all':
self.log('all')
else:
self.log('%d lowest bands' % n)
self.log('Number of valence electrons:', self.wfs.nvalence)
self.log(flush=True)
self.timer.print_info(self)
if dry_run:
self.dry_run()
if (realspace and self.hamiltonian.poisson.get_description()
== 'FDTD+TDDFT'):
self.hamiltonian.poisson.set_density(self.density)
self.hamiltonian.poisson.print_messages(self.log)
self.log.fd.flush()
self.initialized = True
self.log('... initialized\n')
def create_setups(self, mode, xc):
if self.parameters.filter is None and mode.name != 'pw':
gamma = 1.6
N_c = self.parameters.get('gpts')
if N_c is None:
h = (self.parameters.h or 0.2) / Bohr
else:
icell_vc = np.linalg.inv(self.atoms.cell)
h = ((icell_vc**2).sum(0)**-0.5 / N_c).max() / Bohr
def filter(rgd, rcut, f_r, l=0):
gcut = np.pi / h - 2 / rcut / gamma
f_r[:] = rgd.filter(f_r, rcut * gamma, gcut, l)
else:
filter = self.parameters.filter
Z_a = self.atoms.get_atomic_numbers()
self.setups = Setups(Z_a, self.parameters.setups,
self.parameters.basis, xc, filter, self.world)
self.log(self.setups)
def create_grid_descriptor(self, N_c, cell_cv, pbc_c, domain_comm,
parsize_domain):
return GridDescriptor(N_c, cell_cv, pbc_c, domain_comm, parsize_domain)
def create_occupations(self, magmom, orbital_free):
occ = self.parameters.occupations
if occ is None:
if orbital_free:
occ = {'name': 'orbital-free'}
else:
width = self.parameters.width
if width is not None:
warnings.warn(
'Please use occupations=FermiDirac({0})'.format(width))
elif self.atoms.pbc.any():
width = 0.1 # eV
else:
width = 0.0
occ = {'name': 'fermi-dirac', 'width': width}
if isinstance(occ, dict):
occ = create_occupation_number_object(**occ)
if self.parameters.fixdensity:
occ.fixed_fermilevel = True
if self.occupations:
occ.fermilevel = self.occupations.fermilevel
self.occupations = occ
# If occupation numbers are changed, and we have wave functions,
# recalculate the occupation numbers
if self.wfs is not None:
self.occupations.calculate(self.wfs)
self.occupations.magmom = magmom
self.log(self.occupations)
def create_scf(self, nvalence, mode):
if mode.name == 'lcao':
niter_fixdensity = 0
else:
niter_fixdensity = 2
nv = max(nvalence, 1)
cc = self.parameters.convergence
self.scf = SCFLoop(
cc.get('eigenstates', 4.0e-8) / Ha**2 * nv,
cc.get('energy', 0.0005) / Ha * nv,
cc.get('density', 1.0e-4) * nv,
cc.get('forces', np.inf) / (Ha / Bohr), self.parameters.maxiter,
niter_fixdensity, nv)
self.log(self.scf)
def create_symmetry(self, magmom_a, cell_cv):
symm = self.parameters.symmetry
if symm == 'off':
symm = {'point_group': False, 'time_reversal': False}
m_a = magmom_a.round(decimals=3) # round off
id_a = list(zip(self.setups.id_a, m_a))
self.symmetry = Symmetry(id_a, cell_cv, self.atoms.pbc, **symm)
self.symmetry.analyze(self.atoms.get_scaled_positions())
self.setups.set_symmetry(self.symmetry)
def create_eigensolver(self, xc, nbands, mode):
# Number of bands to converge:
nbands_converge = self.parameters.convergence.get('bands', 'occupied')
if nbands_converge == 'all':
nbands_converge = nbands
elif nbands_converge != 'occupied':
assert isinstance(nbands_converge, int)
if nbands_converge < 0:
nbands_converge += nbands
eigensolver = get_eigensolver(self.parameters.eigensolver, mode,
self.parameters.convergence)
eigensolver.nbands_converge = nbands_converge
# XXX Eigensolver class doesn't define an nbands_converge property
if isinstance(xc, SIC):
eigensolver.blocksize = 1
self.wfs.set_eigensolver(eigensolver)
self.log(self.wfs.eigensolver, '\n')
def create_density(self, realspace, mode, background):
gd = self.wfs.gd
big_gd = gd.new_descriptor(comm=self.world)
# Check whether grid is too small. 8 is smallest admissible.
# (we decide this by how difficult it is to make the tests pass)
# (Actually it depends on stencils! But let the user deal with it)
N_c = big_gd.get_size_of_global_array(pad=True)
too_small = np.any(N_c / big_gd.parsize_c < 8)
if self.parallel['augment_grids'] and not too_small:
aux_gd = big_gd
else:
aux_gd = gd
redistributor = GridRedistributor(self.world, self.wfs.kptband_comm,
gd, aux_gd)
# Construct grid descriptor for fine grids for densities
# and potentials:
finegd = aux_gd.refine()
kwargs = dict(gd=gd,
finegd=finegd,
nspins=self.wfs.nspins,
charge=self.parameters.charge +
self.wfs.setups.core_charge,
redistributor=redistributor,
background_charge=background)
if realspace:
self.density = RealSpaceDensity(stencil=mode.interpolation,
**kwargs)
else:
self.density = pw.ReciprocalSpaceDensity(**kwargs)
self.log(self.density, '\n')
def create_hamiltonian(self, realspace, mode, xc):
dens = self.density
kwargs = dict(gd=dens.gd,
finegd=dens.finegd,
nspins=dens.nspins,
setups=dens.setups,
timer=self.timer,
xc=xc,
world=self.world,
redistributor=dens.redistributor,
vext=self.parameters.external,
psolver=self.parameters.poissonsolver)
if realspace:
self.hamiltonian = RealSpaceHamiltonian(stencil=mode.interpolation,
**kwargs)
xc.set_grid_descriptor(self.hamiltonian.finegd) # XXX
else:
self.hamiltonian = pw.ReciprocalSpaceHamiltonian(
pd2=dens.pd2, pd3=dens.pd3, realpbc_c=self.atoms.pbc, **kwargs)
xc.set_grid_descriptor(dens.xc_redistributor.aux_gd) # XXX
self.log(self.hamiltonian, '\n')
def create_wave_functions(self, mode, realspace, nspins, nbands, nao,
nvalence, setups, magmom_a, cell_cv, pbc_c):
par = self.parameters
bzkpts_kc = kpts2ndarray(par.kpts, self.atoms)
kd = KPointDescriptor(bzkpts_kc, nspins)
self.timer.start('Set symmetry')
kd.set_symmetry(self.atoms, self.symmetry, comm=self.world)
self.timer.stop('Set symmetry')
self.log(kd)
parallelization = mpi.Parallelization(self.world, nspins * kd.nibzkpts)
parsize_kpt = self.parallel['kpt']
parsize_domain = self.parallel['domain']
parsize_bands = self.parallel['band']
ndomains = None
if parsize_domain is not None:
ndomains = np.prod(parsize_domain)
if mode.name == 'pw':
if ndomains is not None and ndomains > 1:
raise ValueError('Planewave mode does not support '
'domain decomposition.')
ndomains = 1
parallelization.set(kpt=parsize_kpt,
domain=ndomains,
band=parsize_bands)
comms = parallelization.build_communicators()
domain_comm = comms['d']
kpt_comm = comms['k']
band_comm = comms['b']
kptband_comm = comms['D']
domainband_comm = comms['K']
self.comms = comms
if par.gpts is not None:
if par.h is not None:
raise ValueError("""You can't use both "gpts" and "h"!""")
N_c = np.array(par.gpts)
else:
h = par.h
if h is not None:
h /= Bohr
N_c = get_number_of_grid_points(cell_cv, h, mode, realspace,
kd.symmetry)
self.symmetry.check_grid(N_c)
kd.set_communicator(kpt_comm)
parstride_bands = self.parallel['stridebands']
# Unfortunately we need to remember that we adjusted the
# number of bands so we can print a warning if it differs
# from the number specified by the user. (The number can
# be inferred from the input parameters, but it's tricky
# because we allow negative numbers)
self.nbands_parallelization_adjustment = -nbands % band_comm.size
nbands += self.nbands_parallelization_adjustment
bd = BandDescriptor(nbands, band_comm, parstride_bands)
# Construct grid descriptor for coarse grids for wave functions:
gd = self.create_grid_descriptor(N_c, cell_cv, pbc_c, domain_comm,
parsize_domain)
if hasattr(self, 'time') or mode.force_complex_dtype:
dtype = complex
else:
if kd.gamma:
dtype = float
else:
dtype = complex
wfs_kwargs = dict(gd=gd,
nvalence=nvalence,
setups=setups,
bd=bd,
dtype=dtype,
world=self.world,
kd=kd,
kptband_comm=kptband_comm,
timer=self.timer)
if self.parallel['sl_auto']:
# Choose scalapack parallelization automatically
for key, val in self.parallel.items():
if (key.startswith('sl_') and key != 'sl_auto'
and val is not None):
raise ValueError("Cannot use 'sl_auto' together "
"with '%s'" % key)
max_scalapack_cpus = bd.comm.size * gd.comm.size
nprow = max_scalapack_cpus
npcol = 1
# Get a sort of reasonable number of columns/rows
while npcol < nprow and nprow % 2 == 0:
npcol *= 2
nprow //= 2
assert npcol * nprow == max_scalapack_cpus
# ScaLAPACK creates trouble if there aren't at least a few
# whole blocks; choose block size so there will always be
# several blocks. This will crash for small test systems,
# but so will ScaLAPACK in any case
blocksize = min(-(-nbands // 4), 64)
sl_default = (nprow, npcol, blocksize)
else:
sl_default = self.parallel['sl_default']
if mode.name == 'lcao':
# Layouts used for general diagonalizer
sl_lcao = self.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
lcaoksl = get_KohnSham_layouts(sl_lcao,
'lcao',
gd,
bd,
domainband_comm,
dtype,
nao=nao,
timer=self.timer)
self.wfs = mode(lcaoksl, **wfs_kwargs)
elif mode.name == 'fd' or mode.name == 'pw':
# buffer_size keyword only relevant for fdpw
buffer_size = self.parallel['buffer_size']
# Layouts used for diagonalizer
sl_diagonalize = self.parallel['sl_diagonalize']
if sl_diagonalize is None:
sl_diagonalize = sl_default
diagksl = get_KohnSham_layouts(
sl_diagonalize,
'fd', # XXX
# choice of key 'fd' not so nice
gd,
bd,
domainband_comm,
dtype,
buffer_size=buffer_size,
timer=self.timer)
# Layouts used for orthonormalizer
sl_inverse_cholesky = self.parallel['sl_inverse_cholesky']
if sl_inverse_cholesky is None:
sl_inverse_cholesky = sl_default
if sl_inverse_cholesky != sl_diagonalize:
message = 'sl_inverse_cholesky != sl_diagonalize ' \
'is not implemented.'
raise NotImplementedError(message)
orthoksl = get_KohnSham_layouts(sl_inverse_cholesky,
'fd',
gd,
bd,
domainband_comm,
dtype,
buffer_size=buffer_size,
timer=self.timer)
# Use (at most) all available LCAO for initialization
lcaonbands = min(nbands, nao // band_comm.size * band_comm.size)
try:
lcaobd = BandDescriptor(lcaonbands, band_comm, parstride_bands)
except RuntimeError:
initksl = None
else:
# Layouts used for general diagonalizer
# (LCAO initialization)
sl_lcao = self.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
initksl = get_KohnSham_layouts(sl_lcao,
'lcao',
gd,
lcaobd,
domainband_comm,
dtype,
nao=nao,
timer=self.timer)
self.wfs = mode(diagksl, orthoksl, initksl, **wfs_kwargs)
else:
self.wfs = mode(self, **wfs_kwargs)
self.log(self.wfs, '\n')
def dry_run(self):
# Can be overridden like in gpaw.atom.atompaw
print_cell(self.wfs.gd, self.atoms.pbc, self.log)
print_positions(self.atoms, self.log)
self.log.fd.flush()
raise SystemExit
class LrTDDFT(ExcitationList):
"""Linear Response TDDFT excitation class
Input parameters:
calculator:
the calculator object after a ground state calculation
nspins:
number of spins considered in the calculation
Note: Valid only for unpolarised ground state calculation
eps:
Minimal occupation difference for a transition (default 0.001)
istart:
First occupied state to consider
jend:
Last unoccupied state to consider
xc:
Exchange-Correlation approximation in the Kernel
derivative_level:
0: use Exc, 1: use vxc, 2: use fxc if available
filename:
read from a file
"""
default_parameters = {
'nspins': None,
'eps': 0.001,
'istart': 0,
'jend': sys.maxsize,
'energy_range': None,
'xc': 'GS',
'derivative_level': 1,
'numscale': 0.00001,
'txt': None,
'filename': None,
'finegrid': 2,
'force_ApmB': False, # for tests
'eh_comm': None} # parallelization over eh-pairs
def __init__(self, calculator=None, **kwargs):
self.timer = Timer()
self.diagonalized = False
changed = self.set(**kwargs)
if isinstance(calculator, str):
ExcitationList.__init__(self, None, self.txt)
self.filename = calculator
else:
ExcitationList.__init__(self, calculator, self.txt)
if self.filename is not None:
self.read(self.filename)
if set(['istart', 'jend', 'energy_range']) & set(changed):
# the user has explicitely demanded these
self.diagonalize()
return
if self.eh_comm is None:
self.eh_comm = mpi.serial_comm
elif isinstance(self.eh_comm, (mpi.world.__class__,
mpi.serial_comm.__class__)):
# Correct type already.
pass
else:
# world should be a list of ranks:
self.eh_comm = mpi.world.new_communicator(
np.asarray(self.eh_comm))
if calculator is not None and calculator.initialized:
if not isinstance(calculator.wfs, FDWaveFunctions):
raise RuntimeError(
'Linear response TDDFT supported only in real space mode')
if calculator.wfs.kd.comm.size > 1:
err_txt = 'Spin parallelization with Linear response '
err_txt += "TDDFT. Use parallel={'domain': world.size} "
err_txt += 'calculator parameter.'
raise NotImplementedError(err_txt)
if self.xc == 'GS':
self.xc = calculator.hamiltonian.xc.name
if calculator.parameters.mode != 'lcao':
calculator.converge_wave_functions()
if calculator.density.nct_G is None:
spos_ac = calculator.initialize_positions()
calculator.wfs.initialize(calculator.density,
calculator.hamiltonian, spos_ac)
self.update(calculator)
def set(self, **kwargs):
"""Change parameters."""
changed = []
for key, value in LrTDDFT.default_parameters.items():
if hasattr(self, key):
value = getattr(self, key) # do not overwrite
setattr(self, key, kwargs.pop(key, value))
if value != getattr(self, key):
changed.append(key)
for key in kwargs:
raise KeyError('Unknown key ' + key)
return changed
def set_calculator(self, calculator):
self.calculator = calculator
# self.force_ApmB = parameters['force_ApmB']
self.force_ApmB = None # XXX
def analyse(self, what=None, out=None, min=0.1):
"""Print info about the transitions.
Parameters:
1. what: I list of excitation indicees, None means all
2. out : I where to send the output, None means sys.stdout
3. min : I minimal contribution to list (0<min<1)
"""
if what is None:
what = range(len(self))
elif isinstance(what, numbers.Integral):
what = [what]
if out is None:
out = sys.stdout
for i in what:
print(str(i) + ':', self[i].analyse(min=min), file=out)
def update(self, calculator=None, **kwargs):
changed = self.set(**kwargs)
if calculator is not None:
changed = True
self.set_calculator(calculator)
if not changed:
return
self.forced_update()
def forced_update(self):
"""Recalc yourself."""
if not self.force_ApmB:
Om = OmegaMatrix
name = 'LrTDDFT'
if self.xc:
xc = XC(self.xc)
if hasattr(xc, 'hybrid') and xc.hybrid > 0.0:
Om = ApmB
name = 'LrTDDFThyb'
else:
Om = ApmB
name = 'LrTDDFThyb'
self.kss = KSSingles(calculator=self.calculator,
nspins=self.nspins,
eps=self.eps,
istart=self.istart,
jend=self.jend,
energy_range=self.energy_range,
txt=self.txt)
self.Om = Om(self.calculator, self.kss,
self.xc, self.derivative_level, self.numscale,
finegrid=self.finegrid, eh_comm=self.eh_comm,
txt=self.txt)
self.name = name
def diagonalize(self, **kwargs):
self.set(**kwargs)
self.timer.start('diagonalize')
self.timer.start('omega')
self.Om.diagonalize(self.istart, self.jend, self.energy_range)
self.timer.stop('omega')
self.diagonalized = True
# remove old stuff
self.timer.start('clean')
while len(self):
self.pop()
self.timer.stop('clean')
print('LrTDDFT digonalized:', file=self.txt)
self.timer.start('build')
for j in range(len(self.Om.kss)):
self.append(LrTDDFTExcitation(self.Om, j))
print(' ', str(self[-1]), file=self.txt)
self.timer.stop('build')
self.timer.stop('diagonalize')
def get_Om(self):
return self.Om
def read(self, filename=None, fh=None):
"""Read myself from a file"""
if fh is None:
if filename.endswith('.gz'):
try:
import gzip
f = gzip.open(filename, 'rt')
except:
f = open(filename, 'r')
else:
f = open(filename, 'r')
self.filename = filename
else:
f = fh
self.filename = None
# get my name
s = f.readline().replace('\n', '')
self.name = s.split()[1]
self.xc = f.readline().replace('\n', '').split()[0]
values = f.readline().split()
self.eps = float(values[0])
if len(values) > 1:
self.derivative_level = int(values[1])
self.numscale = float(values[2])
self.finegrid = int(values[3])
else:
# old writing style, use old defaults
self.numscale = 0.001
self.kss = KSSingles(filehandle=f)
if self.name == 'LrTDDFT':
self.Om = OmegaMatrix(kss=self.kss, filehandle=f,
txt=self.txt)
else:
self.Om = ApmB(kss=self.kss, filehandle=f,
txt=self.txt)
self.Om.Kss(self.kss)
# check if already diagonalized
p = f.tell()
s = f.readline()
if s != '# Eigenvalues\n':
# go back to previous position
f.seek(p)
else:
self.diagonalized = True
# load the eigenvalues
n = int(f.readline().split()[0])
for i in range(n):
self.append(LrTDDFTExcitation(string=f.readline()))
# load the eigenvectors
f.readline()
for i in range(n):
values = f.readline().split()
weights = [float(val) for val in values]
self[i].f = np.array(weights)
self[i].kss = self.kss
if fh is None:
f.close()
def singlets_triplets(self):
"""Split yourself into a singlet and triplet object"""
slr = LrTDDFT(None, nspins=self.nspins, eps=self.eps,
istart=self.istart, jend=self.jend, xc=self.xc,
derivative_level=self.derivative_level,
numscale=self.numscale)
tlr = LrTDDFT(None, nspins=self.nspins, eps=self.eps,
istart=self.istart, jend=self.jend, xc=self.xc,
derivative_level=self.derivative_level,
numscale=self.numscale)
slr.Om, tlr.Om = self.Om.singlets_triplets()
for lr in [slr, tlr]:
lr.kss = lr.Om.fullkss
return slr, tlr
def single_pole_approximation(self, i, j):
"""Return the excitation according to the
single pole approximation. See e.g.:
Grabo et al, Theochem 501 (2000) 353-367
"""
for ij, kss in enumerate(self.kss):
if kss.i == i and kss.j == j:
return sqrt(self.Om.full[ij][ij]) * Hartree
return self.Om.full[ij][ij] / kss.energy * Hartree
def __str__(self):
string = ExcitationList.__str__(self)
string += '# derived from:\n'
string += self.Om.kss.__str__()
return string
def write(self, filename=None, fh=None):
"""Write current state to a file.
'filename' is the filename. If the filename ends in .gz,
the file is automatically saved in compressed gzip format.
'fh' is a filehandle. This can be used to write into already
opened files.
"""
if self.calculator is None:
rank = mpi.world.rank
else:
rank = self.calculator.wfs.world.rank
if rank == 0:
if fh is None:
if filename.endswith('.gz'):
try:
import gzip
f = gzip.open(filename, 'wt')
except:
f = open(filename, 'w')
else:
f = open(filename, 'w')
else:
f = fh
f.write('# ' + self.name + '\n')
xc = self.xc
if xc is None:
xc = 'RPA'
if self.calculator is not None:
xc += ' ' + self.calculator.get_xc_functional()
f.write(xc + '\n')
f.write('%g %d %g %d' % (self.eps, int(self.derivative_level),
self.numscale, int(self.finegrid)) + '\n')
self.kss.write(fh=f)
self.Om.write(fh=f)
if len(self):
f.write('# Eigenvalues\n')
istart = self.istart
if istart is None:
istart = self.kss.istart
jend = self.jend
if jend is None:
jend = self.kss.jend
f.write('%d %d %d' % (len(self), istart, jend) + '\n')
for ex in self:
f.write(ex.outstring())
f.write('# Eigenvectors\n')
for ex in self:
for w in ex.f:
f.write('%g ' % w)
f.write('\n')
if fh is None:
f.close()
mpi.world.barrier()
def __getitem__(self, i):
if not self.diagonalized:
self.diagonalize()
return list.__getitem__(self, i)
def __iter__(self):
if not self.diagonalized:
self.diagonalize()
return list.__iter__(self)
def __len__(self):
if not self.diagonalized:
self.diagonalize()
return list.__len__(self)
def get_rpa(self):
"""Calculate RPA and Hartree-fock part of the A+-B matrices."""
# shorthands
kss = self.fullkss
finegrid = self.finegrid
# calculate omega matrix
nij = len(kss)
print("RPAhyb", nij, "transitions", file=self.txt)
AmB = np.zeros((nij, nij))
ApB = self.ApB
# storage place for Coulomb integrals
integrals = {}
for ij in range(nij):
print("RPAhyb kss[" + "%d" % ij + "]=", kss[ij], file=self.txt)
timer = Timer()
timer.start("init")
timer2 = Timer()
# smooth density including compensation charges
timer2.start("with_compensation_charges 0")
rhot_p = kss[ij].with_compensation_charges(finegrid is not 0)
timer2.stop()
# integrate with 1/|r_1-r_2|
timer2.start("poisson")
phit_p = np.zeros(rhot_p.shape, rhot_p.dtype)
self.poisson.solve(phit_p, rhot_p, charge=None)
timer2.stop()
timer.stop()
t0 = timer.get_time("init")
timer.start(ij)
if finegrid == 1:
rhot = kss[ij].with_compensation_charges()
phit = self.gd.zeros()
self.restrict(phit_p, phit)
else:
phit = phit_p
rhot = rhot_p
for kq in range(ij, nij):
if kq != ij:
# smooth density including compensation charges
timer2.start("kq with_compensation_charges")
rhot = kss[kq].with_compensation_charges(finegrid is 2)
timer2.stop()
pre = self.weight_Kijkq(ij, kq)
timer2.start("integrate")
I = self.Coulomb_integral_kss(kss[ij], kss[kq], phit, rhot)
if kss[ij].spin == kss[kq].spin:
name = self.Coulomb_integral_name(kss[ij].i, kss[ij].j, kss[kq].i, kss[kq].j, kss[ij].spin)
integrals[name] = I
ApB[ij, kq] = pre * I
timer2.stop()
if ij == kq:
epsij = kss[ij].get_energy() / kss[ij].get_weight()
AmB[ij, kq] += epsij
ApB[ij, kq] += epsij
timer.stop()
# timer2.write()
if ij < (nij - 1):
print("RPAhyb estimated time left", self.time_left(timer, t0, ij, nij), file=self.txt)
# add HF parts and apply symmetry
if hasattr(self.xc, "hybrid"):
weight = self.xc.hybrid
else:
weight = 0.0
for ij in range(nij):
print("HF kss[" + "%d" % ij + "]", file=self.txt)
timer = Timer()
timer.start("init")
timer.stop()
t0 = timer.get_time("init")
timer.start(ij)
i = kss[ij].i
j = kss[ij].j
s = kss[ij].spin
for kq in range(ij, nij):
if kss[ij].pspin == kss[kq].pspin:
k = kss[kq].i
q = kss[kq].j
ikjq = self.Coulomb_integral_ijkq(i, k, j, q, s, integrals)
iqkj = self.Coulomb_integral_ijkq(i, q, k, j, s, integrals)
ApB[ij, kq] -= weight * (ikjq + iqkj)
AmB[ij, kq] -= weight * (ikjq - iqkj)
ApB[kq, ij] = ApB[ij, kq]
AmB[kq, ij] = AmB[ij, kq]
timer.stop()
if ij < (nij - 1):
print("HF estimated time left", self.time_left(timer, t0, ij, nij), file=self.txt)
return AmB
class RPACorrelation:
def __init__(self,
calc,
xc='RPA',
filename=None,
skip_gamma=False,
qsym=True,
nlambda=None,
nfrequencies=16,
frequency_max=800.0,
frequency_scale=2.0,
frequencies=None,
weights=None,
world=mpi.world,
nblocks=1,
wstc=False,
txt=sys.stdout):
if isinstance(calc, str):
calc = GPAW(calc, txt=None, communicator=mpi.serial_comm)
self.calc = calc
if world.rank != 0:
txt = devnull
elif isinstance(txt, str):
txt = open(txt, 'w')
self.fd = txt
self.timer = Timer()
if frequencies is None:
frequencies, weights = get_gauss_legendre_points(
nfrequencies, frequency_max, frequency_scale)
user_spec = False
else:
assert weights is not None
user_spec = True
self.omega_w = frequencies / Hartree
self.weight_w = weights / Hartree
if nblocks > 1:
assert len(self.omega_w) % nblocks == 0
assert wstc
self.wstc = wstc
self.nblocks = nblocks
self.world = world
self.skip_gamma = skip_gamma
self.ibzq_qc = None
self.weight_q = None
self.initialize_q_points(qsym)
# Energies for all q-vetors and cutoff energies:
self.energy_qi = []
self.filename = filename
self.print_initialization(xc, frequency_scale, nlambda, user_spec)
def initialize_q_points(self, qsym):
kd = self.calc.wfs.kd
self.bzq_qc = kd.get_bz_q_points(first=True)
if not qsym:
self.ibzq_qc = self.bzq_qc
self.weight_q = np.ones(len(self.bzq_qc)) / len(self.bzq_qc)
else:
U_scc = kd.symmetry.op_scc
self.ibzq_qc = kd.get_ibz_q_points(self.bzq_qc, U_scc)[0]
self.weight_q = kd.q_weights
def read(self):
lines = open(self.filename).readlines()[1:]
n = 0
self.energy_qi = []
nq = len(lines) // len(self.ecut_i)
for q_c in self.ibzq_qc[:nq]:
self.energy_qi.append([])
for ecut in self.ecut_i:
q1, q2, q3, ec, energy = [float(x) for x in lines[n].split()]
self.energy_qi[-1].append(energy / Hartree)
n += 1
if (abs(q_c - (q1, q2, q3)).max() > 1e-4
or abs(int(ecut * Hartree) - ec) > 0):
self.energy_qi = []
return
print('Read %d q-points from file: %s' % (nq, self.filename),
file=self.fd)
print(file=self.fd)
def write(self):
if self.world.rank == 0 and self.filename:
fd = open(self.filename, 'w')
print('#%9s %10s %10s %8s %12s' %
('q1', 'q2', 'q3', 'E_cut', 'E_c(q)'),
file=fd)
for energy_i, q_c in zip(self.energy_qi, self.ibzq_qc):
for energy, ecut in zip(energy_i, self.ecut_i):
print('%10.4f %10.4f %10.4f %8d %r' %
(tuple(q_c) + (ecut * Hartree, energy * Hartree)),
file=fd)
def calculate(self, ecut, nbands=None, spin=False):
"""Calculate RPA correlation energy for one or several cutoffs.
ecut: float or list of floats
Plane-wave cutoff(s).
nbands: int
Number of bands (defaults to number of plane-waves).
spin: bool
Separate spin in response funtion.
(Only needed for beyond RPA methods that inherit this function).
"""
p = functools.partial(print, file=self.fd)
if isinstance(ecut, (float, int)):
ecut = ecut * (1 + 0.5 * np.arange(6))**(-2 / 3)
self.ecut_i = np.asarray(np.sort(ecut)) / Hartree
ecutmax = max(self.ecut_i)
if nbands is None:
p('Response function bands : Equal to number of plane waves')
else:
p('Response function bands : %s' % nbands)
p('Plane wave cutoffs (eV) :', end='')
for e in self.ecut_i:
p(' {0:.3f}'.format(e * Hartree), end='')
p()
p()
if self.filename and os.path.isfile(self.filename):
self.read()
self.world.barrier()
chi0 = Chi0(self.calc,
1j * Hartree * self.omega_w,
eta=0.0,
intraband=False,
hilbert=False,
txt=self.fd,
timer=self.timer,
world=self.world,
no_optical_limit=self.wstc,
nblocks=self.nblocks)
self.blockcomm = chi0.blockcomm
wfs = self.calc.wfs
if self.wstc:
with self.timer('WSTC-init'):
p('Using Wigner-Seitz truncated Coulomb potential.')
self.wstc = WignerSeitzTruncatedCoulomb(
wfs.gd.cell_cv, wfs.kd.N_c, self.fd)
nq = len(self.energy_qi)
nw = len(self.omega_w)
nGmax = max(
count_reciprocal_vectors(ecutmax, wfs.gd, q_c)
for q_c in self.ibzq_qc[nq:])
mynGmax = (nGmax + self.nblocks - 1) // self.nblocks
nx = (1 + spin) * nw * mynGmax * nGmax
A1_x = np.empty(nx, complex)
if self.nblocks > 1:
A2_x = np.empty(nx, complex)
else:
A2_x = None
self.timer.start('RPA')
for q_c in self.ibzq_qc[nq:]:
if np.allclose(q_c, 0.0) and self.skip_gamma:
self.energy_qi.append(len(self.ecut_i) * [0.0])
self.write()
p('Not calculating E_c(q) at Gamma')
p()
continue
thisqd = KPointDescriptor([q_c])
pd = PWDescriptor(ecutmax, wfs.gd, complex, thisqd)
nG = pd.ngmax
mynG = (nG + self.nblocks - 1) // self.nblocks
chi0.Ga = self.blockcomm.rank * mynG
chi0.Gb = min(chi0.Ga + mynG, nG)
shape = (1 + spin, nw, chi0.Gb - chi0.Ga, nG)
chi0_swGG = A1_x[:np.prod(shape)].reshape(shape)
chi0_swGG[:] = 0.0
if self.wstc or np.allclose(q_c, 0.0):
# Wings (x=0,1) and head (G=0) for optical limit and three
# directions (v=0,1,2):
chi0_swxvG = np.zeros((1 + spin, nw, 2, 3, nG), complex)
chi0_swvv = np.zeros((1 + spin, nw, 3, 3), complex)
else:
chi0_swxvG = None
chi0_swvv = None
Q_aGii = chi0.initialize_paw_corrections(pd)
# First not completely filled band:
m1 = chi0.nocc1
p('# %s - %s' % (len(self.energy_qi), ctime().split()[-2]))
p('q = [%1.3f %1.3f %1.3f]' % tuple(q_c))
energy_i = []
for ecut in self.ecut_i:
if ecut == ecutmax:
# Nothing to cut away:
cut_G = None
m2 = nbands or nG
else:
cut_G = np.arange(nG)[pd.G2_qG[0] <= 2 * ecut]
m2 = len(cut_G)
p('E_cut = %d eV / Bands = %d:' % (ecut * Hartree, m2))
self.fd.flush()
energy = self.calculate_q(chi0, pd, chi0_swGG, chi0_swxvG,
chi0_swvv, Q_aGii, m1, m2, cut_G,
A2_x)
energy_i.append(energy)
m1 = m2
a = 1 / chi0.kncomm.size
if ecut < ecutmax and a != 1.0:
# Chi0 will be summed again over chicomm, so we divide
# by its size:
chi0_swGG *= a
if chi0_swxvG is not None:
chi0_swxvG *= a
chi0_swvv *= a
self.energy_qi.append(energy_i)
self.write()
p()
e_i = np.dot(self.weight_q, np.array(self.energy_qi))
p('==========================================================')
p()
p('Total correlation energy:')
for e_cut, e in zip(self.ecut_i, e_i):
p('%6.0f: %6.4f eV' % (e_cut * Hartree, e * Hartree))
p()
self.energy_qi = [] # important if another calculation is performed
if len(e_i) > 1:
self.extrapolate(e_i)
p('Calculation completed at: ', ctime())
p()
self.timer.stop('RPA')
self.timer.write(self.fd)
self.fd.flush()
return e_i * Hartree
@timer('chi0(q)')
def calculate_q(self, chi0, pd, chi0_swGG, chi0_swxvG, chi0_swvv, Q_aGii,
m1, m2, cut_G, A2_x):
chi0_wGG = chi0_swGG[0]
if chi0_swxvG is not None:
chi0_wxvG = chi0_swxvG[0]
chi0_wvv = chi0_swvv[0]
else:
chi0_wxvG = None
chi0_wvv = None
chi0._calculate(pd, chi0_wGG, chi0_wxvG, chi0_wvv, Q_aGii, m1, m2,
[0, 1])
print('E_c(q) = ', end='', file=self.fd)
chi0_wGG = chi0.redistribute(chi0_wGG, A2_x)
if not pd.kd.gamma or self.wstc:
e = self.calculate_energy(pd, chi0_wGG, cut_G)
print('%.3f eV' % (e * Hartree), file=self.fd)
self.fd.flush()
else:
e = 0.0
for v in range(3):
chi0_wGG[:, 0] = chi0_wxvG[:, 0, v]
chi0_wGG[:, :, 0] = chi0_wxvG[:, 1, v]
chi0_wGG[:, 0, 0] = chi0_wvv[:, v, v]
ev = self.calculate_energy(pd, chi0_wGG, cut_G)
e += ev
print('%.3f' % (ev * Hartree), end='', file=self.fd)
if v < 2:
print('/', end='', file=self.fd)
else:
print(' eV', file=self.fd)
self.fd.flush()
e /= 3
return e
@timer('Energy')
def calculate_energy(self, pd, chi0_wGG, cut_G):
"""Evaluate correlation energy from chi0."""
if self.wstc:
invG_G = (self.wstc.get_potential(pd) / (4 * pi))**0.5
else:
G_G = pd.G2_qG[0]**0.5 # |G+q|
if pd.kd.gamma:
G_G[0] = 1.0
invG_G = 1.0 / G_G
if cut_G is not None:
invG_G = invG_G[cut_G]
nG = len(invG_G)
e_w = []
for chi0_GG in chi0_wGG:
if cut_G is not None:
chi0_GG = chi0_GG.take(cut_G, 0).take(cut_G, 1)
e_GG = (np.eye(nG) -
4 * np.pi * chi0_GG * invG_G * invG_G[:, np.newaxis])
e = np.log(np.linalg.det(e_GG)) + nG - np.trace(e_GG)
e_w.append(e.real)
E_w = np.zeros_like(self.omega_w)
self.blockcomm.all_gather(np.array(e_w), E_w)
energy = np.dot(E_w, self.weight_w) / (2 * np.pi)
self.E_w = E_w
return energy
def extrapolate(self, e_i):
print('Extrapolated energies:', file=self.fd)
ex_i = []
for i in range(len(e_i) - 1):
e1, e2 = e_i[i:i + 2]
x1, x2 = self.ecut_i[i:i + 2]**-1.5
ex = (e1 * x2 - e2 * x1) / (x2 - x1)
ex_i.append(ex)
print(' %4.0f -%4.0f: %5.3f eV' %
(self.ecut_i[i] * Hartree, self.ecut_i[i + 1] * Hartree,
ex * Hartree),
file=self.fd)
print(file=self.fd)
self.fd.flush()
return e_i * Hartree
def print_initialization(self, xc, frequency_scale, nlambda, user_spec):
p = functools.partial(print, file=self.fd)
p('----------------------------------------------------------')
p('Non-self-consistent %s correlation energy' % xc)
p('----------------------------------------------------------')
p('Started at: ', ctime())
p()
p('Atoms :',
self.calc.atoms.get_chemical_formula(mode='hill'))
p('Ground state XC functional :', self.calc.hamiltonian.xc.name)
p('Valence electrons :', self.calc.wfs.setups.nvalence)
p('Number of bands :', self.calc.wfs.bd.nbands)
p('Number of spins :', self.calc.wfs.nspins)
p('Number of k-points :', len(self.calc.wfs.kd.bzk_kc))
p('Number of irreducible k-points :', len(self.calc.wfs.kd.ibzk_kc))
p('Number of q-points :', len(self.bzq_qc))
p('Number of irreducible q-points :', len(self.ibzq_qc))
p()
for q, weight in zip(self.ibzq_qc, self.weight_q):
p(' q: [%1.4f %1.4f %1.4f] - weight: %1.3f' %
(q[0], q[1], q[2], weight))
p()
p('----------------------------------------------------------')
p('----------------------------------------------------------')
p()
if nlambda is None:
p('Analytical coupling constant integration')
else:
p('Numerical coupling constant integration using', nlambda,
'Gauss-Legendre points')
p()
p('Frequencies')
if not user_spec:
p(' Gauss-Legendre integration with %s frequency points' %
len(self.omega_w))
p(' Transformed from [0,oo] to [0,1] using e^[-aw^(1/B)]')
p(' Highest frequency point at %5.1f eV and B=%1.1f' %
(self.omega_w[-1] * Hartree, frequency_scale))
else:
p(' User specified frequency integration with',
len(self.omega_w), 'frequency points')
p()
p('Parallelization')
p(' Total number of CPUs : % s' % self.world.size)
p(' G-vector decomposition : % s' % self.nblocks)
p(' K-point/band decomposition : % s' %
(self.world.size // self.nblocks))
p()
def start(self, name):
Timer.start(self, name)
abstime = time.time()
t = self.timers[tuple(self.running)] + abstime
self.txt.write('T%s >> %15.8f %s (%7.5fs) started\n'
% (self.srank, abstime, name, t))
def start(self, name):
Timer.start(self, name)
if name in self.compatible:
self.hpm_start(name)
class ResonantRaman(Vibrations):
"""Class for calculating vibrational modes and
resonant Raman intensities using finite difference.
atoms:
Atoms object
Excitations:
Class to calculate the excitations. The class object is
initialized as::
Excitations(atoms.get_calculator())
or by reading form a file as::
Excitations('filename', **exkwargs)
The file is written by calling the method
Excitations.write('filename').
"""
def __init__(
self,
atoms,
Excitations,
indices=None,
gsname='rraman', # name for ground state calculations
exname=None, # name for excited state calculations
delta=0.01,
nfree=2,
directions=None,
exkwargs={}, # kwargs to be passed to Excitations
exext='.ex.gz', # extension for Excitation names
txt='-',
verbose=False):
assert (nfree == 2)
Vibrations.__init__(self, atoms, indices, gsname, delta, nfree)
self.name = gsname + '-d%.3f' % delta
if exname is None:
exname = gsname
self.exname = exname + '-d%.3f' % delta
self.exext = exext
if directions is None:
self.directions = np.array([0, 1, 2])
else:
self.directions = np.array(directions)
self.exobj = Excitations
self.exkwargs = exkwargs
self.timer = Timer()
self.txt = get_txt(txt, rank)
self.verbose = verbose
def log(self, message, pre='# ', end='\n'):
if self.verbose:
self.txt.write(pre + message + end)
self.txt.flush()
def calculate(self, filename, fd):
"""Call ground and excited state calculation"""
self.timer.start('Ground state')
forces = self.atoms.get_forces()
if rank == 0:
pickle.dump(forces, fd)
fd.close()
self.timer.stop('Ground state')
self.timer.start('Excitations')
basename, _ = os.path.splitext(filename)
excitations = self.exobj(self.atoms.get_calculator())
excitations.write(basename + self.exext)
self.timer.stop('Excitations')
def get_intensity_tensor(self, omega, gamma=0.1):
if not hasattr(self, 'modes'):
self.read()
if not hasattr(self, 'ex0'):
eu = units.Hartree
def get_me_tensor(exname, n, form='v'):
def outer(ex):
me = ex.get_dipole_me(form=form)
return np.outer(me, me.conj())
self.log('reading ' + exname)
ex_p = self.exobj(exname, **self.exkwargs)
if len(ex_p) != n:
raise RuntimeError(
('excitations {0} of wrong length: {1} != {2}' +
' exkwargs={3}').format(exname, len(ex_p), n,
self.exkwargs))
m_ccp = np.empty((3, 3, len(ex_p)), dtype=complex)
for p, ex in enumerate(ex_p):
m_ccp[:, :, p] = outer(ex)
return m_ccp
self.timer.start('reading excitations')
self.log('reading ' + self.exname + '.eq' + self.exext)
ex_p = self.exobj(self.exname + '.eq' + self.exext,
**self.exkwargs)
n = len(ex_p)
self.ex0 = np.array([ex.energy * eu for ex in ex_p])
self.exminus = []
self.explus = []
for a in self.indices:
for i in 'xyz':
name = '%s.%d%s' % (self.exname, a, i)
self.exminus.append(
get_me_tensor(name + '-' + self.exext, n))
self.explus.append(
get_me_tensor(name + '+' + self.exext, n))
self.timer.stop('reading excitations')
self.timer.start('amplitudes')
self.timer.start('init')
ndof = 3 * len(self.indices)
amplitudes = np.zeros((ndof, 3, 3), dtype=complex)
pre = 1. / (2 * self.delta)
self.timer.stop('init')
def kappa(me_ccp, e_p, omega, gamma, form='v'):
"""Kappa tensor after Profeta and Mauri
PRB 63 (2001) 245415"""
result = (me_ccp / (e_p - omega - 1j * gamma) + me_ccp.conj() /
(e_p + omega + 1j * gamma))
return result.sum(2)
r = 0
for a in self.indices:
for i in 'xyz':
amplitudes[r] = pre * (
kappa(self.explus[r], self.ex0, omega, gamma) -
kappa(self.exminus[r], self.ex0, omega, gamma))
r += 1
self.timer.stop('amplitudes')
# map to modes
am = np.dot(amplitudes.T, self.modes.T).T
return omega**4 * (am * am.conj()).real
def get_intensities(self, omega, gamma=0.1):
return self.get_intensity_tensor(omega, gamma).sum(axis=1).sum(axis=1)
def get_spectrum(self,
omega,
gamma=0.1,
start=200.0,
end=4000.0,
npts=None,
width=4.0,
type='Gaussian',
method='standard',
direction='central',
intensity_unit='????',
normalize=False):
"""Get resonant Raman spectrum.
The method returns wavenumbers in cm^-1 with corresponding
absolute infrared intensity.
Start and end point, and width of the Gaussian/Lorentzian should
be given in cm^-1.
normalize=True ensures the integral over the peaks to give the
intensity.
"""
self.type = type.lower()
assert self.type in ['gaussian', 'lorentzian']
if not npts:
npts = int((end - start) / width * 10 + 1)
frequencies = self.get_frequencies(method, direction).real
intensities = self.get_intensities(omega, gamma)
prefactor = 1
if type == 'lorentzian':
intensities = intensities * width * np.pi / 2.
if normalize:
prefactor = 2. / width / np.pi
else:
sigma = width / 2. / np.sqrt(2. * np.log(2.))
if normalize:
prefactor = 1. / sigma / np.sqrt(2 * np.pi)
# Make array with spectrum data
spectrum = np.empty(npts)
energies = np.linspace(start, end, npts)
for i, energy in enumerate(energies):
energies[i] = energy
if type == 'lorentzian':
spectrum[i] = (intensities * 0.5 * width / np.pi / (
(frequencies - energy)**2 + 0.25 * width**2)).sum()
else:
spectrum[i] = (
intensities *
np.exp(-(frequencies - energy)**2 / 2. / sigma**2)).sum()
return [energies, prefactor * spectrum]
def write_spectrum(self,
omega,
gamma,
out='resonant-raman-spectra.dat',
start=200,
end=4000,
npts=None,
width=10,
type='Gaussian',
method='standard',
direction='central'):
"""Write out spectrum to file.
First column is the wavenumber in cm^-1, the second column the
absolute infrared intensities, and
the third column the absorbance scaled so that data runs
from 1 to 0. Start and end
point, and width of the Gaussian/Lorentzian should be given
in cm^-1."""
energies, spectrum = self.get_spectrum(omega, gamma, start, end, npts,
width, type, method, direction)
# Write out spectrum in file. First column is absolute intensities.
outdata = np.empty([len(energies), 3])
outdata.T[0] = energies
outdata.T[1] = spectrum
fd = open(out, 'w')
fd.write('# Resonant Raman spectrum\n')
fd.write('# omega={0:g} eV, gamma={1:g} eV\n'.format(omega, gamma))
fd.write('# %s folded, width=%g cm^-1\n' % (type.title(), width))
fd.write('# [cm^-1] [a.u.]\n')
for row in outdata:
fd.write('%.3f %15.5g\n' % (row[0], row[1]))
fd.close()
def summary(self,
omega,
gamma=0.1,
method='standard',
direction='central',
intensity_unit='(D/A)2/amu',
log=sys.stdout):
"""Print summary for given omega [eV]"""
hnu = self.get_energies(method, direction)
s = 0.01 * units._e / units._c / units._hplanck
intensities = self.get_intensities(omega, gamma)
if isinstance(log, str):
log = paropen(log, 'a')
parprint('-------------------------------------', file=log)
parprint(' excitation at ' + str(omega) + ' eV', file=log)
parprint(' gamma ' + str(gamma) + ' eV\n', file=log)
parprint(' Mode Frequency Intensity', file=log)
parprint(' # meV cm^-1 [a.u.]', file=log)
parprint('-------------------------------------', file=log)
for n, e in enumerate(hnu):
if e.imag != 0:
c = 'i'
e = e.imag
else:
c = ' '
e = e.real
parprint('%3d %6.1f%s %7.1f%s %9.3g' %
(n, 1000 * e, c, s * e, c, intensities[n]),
file=log)
parprint('-------------------------------------', file=log)
parprint('Zero-point energy: %.3f eV' % self.get_zero_point_energy(),
file=log)
def __del__(self):
self.timer.write(self.txt)
class GPAW(PAW, Calculator):
"""This is the ASE-calculator frontend for doing a PAW calculation."""
implemented_properties = [
'energy', 'forces', 'stress', 'dipole', 'magmom', 'magmoms'
]
default_parameters = {
'mode': 'fd',
'xc': 'LDA',
'occupations': None,
'poissonsolver': None,
'h': None, # Angstrom
'gpts': None,
'kpts': [(0.0, 0.0, 0.0)],
'nbands': None,
'charge': 0,
'setups': {},
'basis': {},
'spinpol': None,
'fixdensity': False,
'filter': None,
'mixer': None,
'eigensolver': None,
'background_charge': None,
'experimental': {
'reuse_wfs_method': 'paw',
'niter_fixdensity': 0,
'magmoms': None,
'soc': None,
'kpt_refine': None
},
'external': None,
'random': False,
'hund': False,
'maxiter': 333,
'idiotproof': True,
'symmetry': {
'point_group': True,
'time_reversal': True,
'symmorphic': True,
'tolerance': 1e-7,
'do_not_symmetrize_the_density': False
},
'convergence': {
'energy': 0.0005, # eV / electron
'density': 1.0e-4,
'eigenstates': 4.0e-8, # eV^2
'bands': 'occupied',
'forces': np.inf
}, # eV / Ang
'dtype': None, # Deprecated
'width': None, # Deprecated
'verbose': 0
}
default_parallel = {
'kpt': None,
'domain': gpaw.parsize_domain,
'band': gpaw.parsize_bands,
'order': 'kdb',
'stridebands': False,
'augment_grids': gpaw.augment_grids,
'sl_auto': False,
'sl_default': gpaw.sl_default,
'sl_diagonalize': gpaw.sl_diagonalize,
'sl_inverse_cholesky': gpaw.sl_inverse_cholesky,
'sl_lcao': gpaw.sl_lcao,
'sl_lrtddft': gpaw.sl_lrtddft,
'use_elpa': False,
'elpasolver': '2stage',
'buffer_size': gpaw.buffer_size
}
def __init__(self,
restart=None,
ignore_bad_restart_file=False,
label=None,
atoms=None,
timer=None,
communicator=None,
txt='-',
parallel=None,
**kwargs):
self.parallel = dict(self.default_parallel)
if parallel:
for key in parallel:
if key not in self.default_parallel:
allowed = ', '.join(list(self.default_parallel.keys()))
raise TypeError('Unexpected keyword "{}" in "parallel" '
'dictionary. Must be one of: {}'.format(
key, allowed))
self.parallel.update(parallel)
if timer is None:
self.timer = Timer()
else:
self.timer = timer
self.scf = None
self.wfs = None
self.occupations = None
self.density = None
self.hamiltonian = None
self.spos_ac = None # XXX store this in some better way.
self.observers = [] # XXX move to self.scf
self.initialized = False
self.world = communicator
if self.world is None:
self.world = mpi.world
elif not hasattr(self.world, 'new_communicator'):
self.world = mpi.world.new_communicator(np.asarray(self.world))
self.log = GPAWLogger(world=self.world)
self.log.fd = txt
self.reader = None
Calculator.__init__(self, restart, ignore_bad_restart_file, label,
atoms, **kwargs)
def __del__(self):
# Write timings and close reader if necessary.
# If we crashed in the constructor (e.g. a bad keyword), we may not
# have the normally expected attributes:
if hasattr(self, 'timer'):
self.timer.write(self.log.fd)
if hasattr(self, 'reader') and self.reader is not None:
self.reader.close()
def write(self, filename, mode=''):
self.log('Writing to {} (mode={!r})\n'.format(filename, mode))
writer = Writer(filename, self.world)
self._write(writer, mode)
writer.close()
self.world.barrier()
def _write(self, writer, mode):
from ase.io.trajectory import write_atoms
writer.write(version=1,
gpaw_version=gpaw.__version__,
ha=Ha,
bohr=Bohr)
write_atoms(writer.child('atoms'), self.atoms)
writer.child('results').write(**self.results)
writer.child('parameters').write(**self.todict())
self.density.write(writer.child('density'))
self.hamiltonian.write(writer.child('hamiltonian'))
self.occupations.write(writer.child('occupations'))
self.scf.write(writer.child('scf'))
self.wfs.write(writer.child('wave_functions'), mode == 'all')
return writer
def _set_atoms(self, atoms):
check_atoms_too_close(atoms)
self.atoms = atoms
# GPAW works in terms of the scaled positions. We want to
# extract the scaled positions in only one place, and that is
# here. No other place may recalculate them, or we might end up
# with rounding errors and inconsistencies.
self.spos_ac = atoms.get_scaled_positions() % 1.0
def read(self, filename):
from ase.io.trajectory import read_atoms
self.log('Reading from {}'.format(filename))
self.reader = reader = Reader(filename)
atoms = read_atoms(reader.atoms)
self._set_atoms(atoms)
res = reader.results
self.results = dict((key, res.get(key)) for key in res.keys())
if self.results:
self.log('Read {}'.format(', '.join(sorted(self.results))))
self.log('Reading input parameters:')
# XXX param
self.parameters = self.get_default_parameters()
dct = {}
for key, value in reader.parameters.asdict().items():
if (isinstance(value, dict)
and isinstance(self.parameters[key], dict)):
self.parameters[key].update(value)
else:
self.parameters[key] = value
dct[key] = self.parameters[key]
self.log.print_dict(dct)
self.log()
self.initialize(reading=True)
self.density.read(reader)
self.hamiltonian.read(reader)
self.occupations.read(reader)
self.scf.read(reader)
self.wfs.read(reader)
# We need to do this in a better way: XXX
from gpaw.utilities.partition import AtomPartition
atom_partition = AtomPartition(self.wfs.gd.comm,
np.zeros(len(self.atoms), dtype=int))
self.wfs.atom_partition = atom_partition
self.density.atom_partition = atom_partition
self.hamiltonian.atom_partition = atom_partition
rank_a = self.density.gd.get_ranks_from_positions(self.spos_ac)
new_atom_partition = AtomPartition(self.density.gd.comm, rank_a)
for obj in [self.density, self.hamiltonian]:
obj.set_positions_without_ruining_everything(
self.spos_ac, new_atom_partition)
self.hamiltonian.xc.read(reader)
if self.hamiltonian.xc.name == 'GLLBSC':
# XXX GLLB: See test/lcaotddft/gllbsc.py
self.occupations.calculate(self.wfs)
return reader
def check_state(self, atoms, tol=1e-15):
system_changes = Calculator.check_state(self, atoms, tol)
if 'positions' not in system_changes:
if self.hamiltonian:
if self.hamiltonian.vext:
if self.hamiltonian.vext.vext_g is None:
# QMMM atoms have moved:
system_changes.append('positions')
return system_changes
def calculate(self,
atoms=None,
properties=['energy'],
system_changes=['cell']):
"""Calculate things."""
Calculator.calculate(self, atoms)
atoms = self.atoms
if system_changes:
self.log('System changes:', ', '.join(system_changes), '\n')
if system_changes == ['positions']:
# Only positions have changed:
self.density.reset()
else:
# Drastic changes:
self.wfs = None
self.occupations = None
self.density = None
self.hamiltonian = None
self.scf = None
self.initialize(atoms)
self.set_positions(atoms)
if not self.initialized:
self.initialize(atoms)
self.set_positions(atoms)
if not (self.wfs.positions_set and self.hamiltonian.positions_set):
self.set_positions(atoms)
if not self.scf.converged:
print_cell(self.wfs.gd, self.atoms.pbc, self.log)
with self.timer('SCF-cycle'):
self.scf.run(self.wfs, self.hamiltonian, self.density,
self.occupations, self.log, self.call_observers)
self.log('\nConverged after {} iterations.\n'.format(
self.scf.niter))
e_free = self.hamiltonian.e_total_free
e_extrapolated = self.hamiltonian.e_total_extrapolated
self.results['energy'] = e_extrapolated * Ha
self.results['free_energy'] = e_free * Ha
dipole_v = self.density.calculate_dipole_moment() * Bohr
self.log(
'Dipole moment: ({:.6f}, {:.6f}, {:.6f}) |e|*Ang\n'.format(
*dipole_v))
self.results['dipole'] = dipole_v
if self.wfs.nspins == 2 or not self.density.collinear:
totmom_v, magmom_av = self.density.estimate_magnetic_moments()
self.log(
'Total magnetic moment: ({:.6f}, {:.6f}, {:.6f})'.format(
*totmom_v))
self.log('Local magnetic moments:')
symbols = self.atoms.get_chemical_symbols()
for a, mom_v in enumerate(magmom_av):
self.log('{:4} {:2} ({:9.6f}, {:9.6f}, {:9.6f})'.format(
a, symbols[a], *mom_v))
self.log()
self.results['magmom'] = self.occupations.magmom
self.results['magmoms'] = magmom_av[:, 2].copy()
self.summary()
self.call_observers(self.scf.niter, final=True)
if 'forces' in properties:
with self.timer('Forces'):
F_av = calculate_forces(self.wfs, self.density,
self.hamiltonian, self.log)
self.results['forces'] = F_av * (Ha / Bohr)
if 'stress' in properties:
with self.timer('Stress'):
try:
stress = calculate_stress(self).flat[[0, 4, 8, 5, 2, 1]]
except NotImplementedError:
# Our ASE Calculator base class will raise
# PropertyNotImplementedError for us.
pass
else:
self.results['stress'] = stress * (Ha / Bohr**3)
def summary(self):
efermi = self.occupations.fermilevel
self.hamiltonian.summary(efermi, self.log)
self.density.summary(self.atoms, self.occupations.magmom, self.log)
self.occupations.summary(self.log)
self.wfs.summary(self.log)
try:
bandgap(self, output=self.log.fd, efermi=efermi * Ha)
except ValueError:
pass
self.log.fd.flush()
def set(self, **kwargs):
"""Change parameters for calculator.
Examples::
calc.set(xc='PBE')
calc.set(nbands=20, kpts=(4, 1, 1))
"""
# Verify that keys are consistent with default ones.
for key in kwargs:
if key != 'txt' and key not in self.default_parameters:
raise TypeError('Unknown GPAW parameter: {}'.format(key))
if key in ['convergence', 'symmetry', 'experimental'
] and isinstance(kwargs[key], dict):
# For values that are dictionaries, verify subkeys, too.
default_dict = self.default_parameters[key]
for subkey in kwargs[key]:
if subkey not in default_dict:
allowed = ', '.join(list(default_dict.keys()))
raise TypeError('Unknown subkeyword "{}" of keyword '
'"{}". Must be one of: {}'.format(
subkey, key, allowed))
changed_parameters = Calculator.set(self, **kwargs)
for key in ['setups', 'basis']:
if key in changed_parameters:
dct = changed_parameters[key]
if isinstance(dct, dict) and None in dct:
dct['default'] = dct.pop(None)
warnings.warn('Please use {key}={dct}'.format(key=key,
dct=dct))
# We need to handle txt early in order to get logging up and running:
if 'txt' in changed_parameters:
self.log.fd = changed_parameters.pop('txt')
if not changed_parameters:
return {}
self.initialized = False
self.scf = None
self.results = {}
self.log('Input parameters:')
self.log.print_dict(changed_parameters)
self.log()
for key in changed_parameters:
if key in ['eigensolver', 'convergence'] and self.wfs:
self.wfs.set_eigensolver(None)
if key in [
'mixer', 'verbose', 'txt', 'hund', 'random', 'eigensolver',
'idiotproof'
]:
continue
if key in ['convergence', 'fixdensity', 'maxiter']:
continue
# Check nested arguments
if key in ['experimental']:
changed_parameters2 = changed_parameters[key]
for key2 in changed_parameters2:
if key2 in ['kpt_refine', 'magmoms', 'soc']:
self.wfs = None
elif key2 in ['reuse_wfs_method', 'niter_fixdensity']:
continue
else:
raise TypeError('Unknown keyword argument:', key2)
continue
# More drastic changes:
if self.wfs:
self.wfs.set_orthonormalized(False)
if key in ['external', 'xc', 'poissonsolver']:
self.hamiltonian = None
elif key in ['occupations', 'width']:
pass
elif key in ['charge', 'background_charge']:
self.hamiltonian = None
self.density = None
self.wfs = None
elif key in ['kpts', 'nbands', 'symmetry']:
self.wfs = None
elif key in ['h', 'gpts', 'setups', 'spinpol', 'dtype', 'mode']:
self.density = None
self.hamiltonian = None
self.wfs = None
elif key in ['basis']:
self.wfs = None
else:
raise TypeError('Unknown keyword argument: "%s"' % key)
def initialize_positions(self, atoms=None):
"""Update the positions of the atoms."""
self.log('Initializing position-dependent things.\n')
if atoms is None:
atoms = self.atoms
else:
atoms = atoms.copy()
self._set_atoms(atoms)
mpi.synchronize_atoms(atoms, self.world)
rank_a = self.wfs.gd.get_ranks_from_positions(self.spos_ac)
atom_partition = AtomPartition(self.wfs.gd.comm, rank_a, name='gd')
self.wfs.set_positions(self.spos_ac, atom_partition)
self.density.set_positions(self.spos_ac, atom_partition)
self.hamiltonian.set_positions(self.spos_ac, atom_partition)
def set_positions(self, atoms=None):
"""Update the positions of the atoms and initialize wave functions."""
self.initialize_positions(atoms)
nlcao, nrand = self.wfs.initialize(self.density, self.hamiltonian,
self.spos_ac)
if nlcao + nrand:
self.log('Creating initial wave functions:')
if nlcao:
self.log(' ', plural(nlcao, 'band'), 'from LCAO basis set')
if nrand:
self.log(' ', plural(nrand, 'band'), 'from random numbers')
self.log()
self.wfs.eigensolver.reset()
self.scf.reset()
print_positions(self.atoms, self.log, self.density.magmom_av)
def initialize(self, atoms=None, reading=False):
"""Inexpensive initialization."""
self.log('Initialize ...\n')
if atoms is None:
atoms = self.atoms
else:
atoms = atoms.copy()
self._set_atoms(atoms)
par = self.parameters
natoms = len(atoms)
cell_cv = atoms.get_cell() / Bohr
number_of_lattice_vectors = cell_cv.any(axis=1).sum()
if number_of_lattice_vectors < 3:
raise ValueError(
'GPAW requires 3 lattice vectors. Your system has {}.'.format(
number_of_lattice_vectors))
pbc_c = atoms.get_pbc()
assert len(pbc_c) == 3
magmom_a = atoms.get_initial_magnetic_moments()
if par.experimental.get('magmoms') is not None:
magmom_av = np.array(par.experimental['magmoms'], float)
collinear = False
else:
magmom_av = np.zeros((natoms, 3))
magmom_av[:, 2] = magmom_a
collinear = True
mpi.synchronize_atoms(atoms, self.world)
# Generate new xc functional only when it is reset by set
# XXX sounds like this should use the _changed_keywords dictionary.
if self.hamiltonian is None or self.hamiltonian.xc is None:
if isinstance(par.xc, (basestring, dict)):
xc = XC(par.xc, collinear=collinear, atoms=atoms)
else:
xc = par.xc
else:
xc = self.hamiltonian.xc
mode = par.mode
if isinstance(mode, basestring):
mode = {'name': mode}
if isinstance(mode, dict):
mode = create_wave_function_mode(**mode)
if par.dtype == complex:
warnings.warn('Use mode={}(..., force_complex_dtype=True) '
'instead of dtype=complex'.format(mode.name.upper()))
mode.force_complex_dtype = True
del par['dtype']
par.mode = mode
if xc.orbital_dependent and mode.name == 'lcao':
raise ValueError('LCAO mode does not support '
'orbital-dependent XC functionals.')
realspace = (mode.name != 'pw' and mode.interpolation != 'fft')
if not realspace:
pbc_c = np.ones(3, bool)
self.create_setups(mode, xc)
if par.hund:
if natoms != 1:
raise ValueError('hund=True arg only valid for single atoms!')
spinpol = True
magmom_av[0, 2] = self.setups[0].get_hunds_rule_moment(par.charge)
if collinear:
magnetic = magmom_av.any()
spinpol = par.spinpol
if spinpol is None:
spinpol = magnetic
elif magnetic and not spinpol:
raise ValueError('Non-zero initial magnetic moment for a ' +
'spin-paired calculation!')
nspins = 1 + int(spinpol)
if spinpol:
self.log('Spin-polarized calculation.')
self.log('Magnetic moment: {:.6f}\n'.format(magmom_av.sum()))
else:
self.log('Spin-paired calculation\n')
else:
nspins = 1
self.log('Non-collinear calculation.')
self.log('Magnetic moment: ({:.6f}, {:.6f}, {:.6f})\n'.format(
*magmom_av.sum(0)))
if isinstance(par.background_charge, dict):
background = create_background_charge(**par.background_charge)
else:
background = par.background_charge
nao = self.setups.nao
nvalence = self.setups.nvalence - par.charge
if par.background_charge is not None:
nvalence += background.charge
M = np.linalg.norm(magmom_av.sum(0))
nbands = par.nbands
orbital_free = any(setup.orbital_free for setup in self.setups)
if orbital_free:
nbands = 1
if isinstance(nbands, basestring):
if nbands == 'nao':
nbands = nao
elif nbands[-1] == '%':
basebands = (nvalence + M) / 2
nbands = int(np.ceil(float(nbands[:-1]) / 100 * basebands))
else:
raise ValueError('Integer expected: Only use a string '
'if giving a percentage of occupied bands')
if nbands is None:
# Number of bound partial waves:
nbandsmax = sum(setup.get_default_nbands()
for setup in self.setups)
nbands = int(np.ceil((1.2 * (nvalence + M) / 2))) + 4
if nbands > nbandsmax:
nbands = nbandsmax
if mode.name == 'lcao' and nbands > nao:
nbands = nao
elif nbands <= 0:
nbands = max(1, int(nvalence + M + 0.5) // 2 + (-nbands))
if nbands > nao and mode.name == 'lcao':
raise ValueError('Too many bands for LCAO calculation: '
'%d bands and only %d atomic orbitals!' %
(nbands, nao))
if nvalence < 0:
raise ValueError(
'Charge %f is not possible - not enough valence electrons' %
par.charge)
if nvalence > 2 * nbands and not orbital_free:
raise ValueError('Too few bands! Electrons: %f, bands: %d' %
(nvalence, nbands))
self.create_occupations(magmom_av[:, 2].sum(), orbital_free)
if self.scf is None:
self.create_scf(nvalence, mode)
self.create_symmetry(magmom_av, cell_cv)
if not collinear:
nbands *= 2
if not self.wfs:
self.create_wave_functions(mode, realspace, nspins, collinear,
nbands, nao, nvalence, self.setups,
cell_cv, pbc_c)
else:
self.wfs.set_setups(self.setups)
if not self.wfs.eigensolver:
self.create_eigensolver(xc, nbands, mode)
if self.density is None and not reading:
assert not par.fixdensity, 'No density to fix!'
olddens = None
if (self.density is not None and
(self.density.gd.parsize_c != self.wfs.gd.parsize_c).any()):
# Domain decomposition has changed, so we need to
# reinitialize density and hamiltonian:
if par.fixdensity:
olddens = self.density
self.density = None
self.hamiltonian = None
if self.density is None:
self.create_density(realspace, mode, background)
# XXXXXXXXXX if setups change, then setups.core_charge may change.
# But that parameter was supplied in Density constructor!
# This surely is a bug!
self.density.initialize(self.setups, self.timer, magmom_av, par.hund)
self.density.set_mixer(par.mixer)
if self.density.mixer.driver.name == 'dummy' or par.fixdensity:
self.log('No density mixing\n')
else:
self.log(self.density.mixer, '\n')
self.density.fixed = par.fixdensity
self.density.log = self.log
if olddens is not None:
self.density.initialize_from_other_density(olddens,
self.wfs.kptband_comm)
if self.hamiltonian is None:
self.create_hamiltonian(realspace, mode, xc)
xc.initialize(self.density, self.hamiltonian, self.wfs,
self.occupations)
description = xc.get_description()
if description is not None:
self.log('XC parameters: {}\n'.format('\n '.join(
description.splitlines())))
if xc.name == 'GLLBSC' and olddens is not None:
xc.heeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeelp(olddens)
self.print_memory_estimate(maxdepth=memory_estimate_depth + 1)
print_parallelization_details(self.wfs, self.hamiltonian, self.log)
self.log('Number of atoms:', natoms)
self.log('Number of atomic orbitals:', self.wfs.setups.nao)
self.log('Number of bands in calculation:', self.wfs.bd.nbands)
self.log('Bands to converge: ', end='')
n = par.convergence.get('bands', 'occupied')
if n == 'occupied':
self.log('occupied states only')
elif n == 'all':
self.log('all')
else:
self.log('%d lowest bands' % n)
self.log('Number of valence electrons:', self.wfs.nvalence)
self.log(flush=True)
self.timer.print_info(self)
if dry_run:
self.dry_run()
if (realspace and self.hamiltonian.poisson.get_description()
== 'FDTD+TDDFT'):
self.hamiltonian.poisson.set_density(self.density)
self.hamiltonian.poisson.print_messages(self.log)
self.log.fd.flush()
self.initialized = True
self.log('... initialized\n')
def create_setups(self, mode, xc):
if self.parameters.filter is None and mode.name != 'pw':
gamma = 1.6
N_c = self.parameters.get('gpts')
if N_c is None:
h = (self.parameters.h or 0.2) / Bohr
else:
icell_vc = np.linalg.inv(self.atoms.cell)
h = ((icell_vc**2).sum(0)**-0.5 / N_c).max() / Bohr
def filter(rgd, rcut, f_r, l=0):
gcut = np.pi / h - 2 / rcut / gamma
ftmp = rgd.filter(f_r, rcut * gamma, gcut, l)
f_r[:] = ftmp[:len(f_r)]
else:
filter = self.parameters.filter
Z_a = self.atoms.get_atomic_numbers()
self.setups = Setups(Z_a, self.parameters.setups,
self.parameters.basis, xc, filter, self.world)
self.log(self.setups)
def create_grid_descriptor(self, N_c, cell_cv, pbc_c, domain_comm,
parsize_domain):
return GridDescriptor(N_c, cell_cv, pbc_c, domain_comm, parsize_domain)
def create_occupations(self, magmom, orbital_free):
occ = self.parameters.occupations
if occ is None:
if orbital_free:
occ = {'name': 'orbital-free'}
else:
width = self.parameters.width
if width is not None:
warnings.warn(
'Please use occupations=FermiDirac({})'.format(width))
elif self.atoms.pbc.any():
width = 0.1 # eV
else:
width = 0.0
occ = {'name': 'fermi-dirac', 'width': width}
if isinstance(occ, dict):
occ = create_occupation_number_object(**occ)
if self.parameters.fixdensity:
occ.fixed_fermilevel = True
if self.occupations:
occ.fermilevel = self.occupations.fermilevel
self.occupations = occ
# If occupation numbers are changed, and we have wave functions,
# recalculate the occupation numbers
if self.wfs is not None:
self.occupations.calculate(self.wfs)
self.occupations.magmom = magmom
self.log(self.occupations)
def create_scf(self, nvalence, mode):
# if mode.name == 'lcao':
# niter_fixdensity = 0
# else:
# niter_fixdensity = 2
nv = max(nvalence, 1)
cc = self.parameters.convergence
self.scf = SCFLoop(
cc.get('eigenstates', 4.0e-8) / Ha**2 * nv,
cc.get('energy', 0.0005) / Ha * nv,
cc.get('density', 1.0e-4) * nv,
cc.get('forces', np.inf) / (Ha / Bohr),
self.parameters.maxiter,
# XXX make sure niter_fixdensity value is *always* set from default
# Subdictionary defaults seem to not be set when user provides
# e.g. {}. We should change that so it works like the ordinary
# parameters.
self.parameters.experimental.get('niter_fixdensity', 0),
nv)
self.log(self.scf)
def create_symmetry(self, magmom_av, cell_cv):
symm = self.parameters.symmetry
if symm == 'off':
symm = {'point_group': False, 'time_reversal': False}
m_av = magmom_av.round(decimals=3) # round off
id_a = [id + tuple(m_v) for id, m_v in zip(self.setups.id_a, m_av)]
self.symmetry = Symmetry(id_a, cell_cv, self.atoms.pbc, **symm)
self.symmetry.analyze(self.spos_ac)
self.setups.set_symmetry(self.symmetry)
def create_eigensolver(self, xc, nbands, mode):
# Number of bands to converge:
nbands_converge = self.parameters.convergence.get('bands', 'occupied')
if nbands_converge == 'all':
nbands_converge = nbands
elif nbands_converge != 'occupied':
assert isinstance(nbands_converge, int)
if nbands_converge < 0:
nbands_converge += nbands
eigensolver = get_eigensolver(self.parameters.eigensolver, mode,
self.parameters.convergence)
eigensolver.nbands_converge = nbands_converge
# XXX Eigensolver class doesn't define an nbands_converge property
if isinstance(xc, SIC):
eigensolver.blocksize = 1
self.wfs.set_eigensolver(eigensolver)
self.log('Eigensolver\n ', self.wfs.eigensolver, '\n')
def create_density(self, realspace, mode, background):
gd = self.wfs.gd
big_gd = gd.new_descriptor(comm=self.world)
# Check whether grid is too small. 8 is smallest admissible.
# (we decide this by how difficult it is to make the tests pass)
# (Actually it depends on stencils! But let the user deal with it)
N_c = big_gd.get_size_of_global_array(pad=True)
too_small = np.any(N_c / big_gd.parsize_c < 8)
if (self.parallel['augment_grids'] and not too_small
and mode.name != 'pw'):
aux_gd = big_gd
else:
aux_gd = gd
redistributor = GridRedistributor(self.world, self.wfs.kptband_comm,
gd, aux_gd)
# Construct grid descriptor for fine grids for densities
# and potentials:
finegd = aux_gd.refine()
kwargs = dict(gd=gd,
finegd=finegd,
nspins=self.wfs.nspins,
collinear=self.wfs.collinear,
charge=self.parameters.charge +
self.wfs.setups.core_charge,
redistributor=redistributor,
background_charge=background)
if realspace:
self.density = RealSpaceDensity(stencil=mode.interpolation,
**kwargs)
else:
self.density = pw.ReciprocalSpaceDensity(**kwargs)
self.log(self.density, '\n')
def create_hamiltonian(self, realspace, mode, xc):
dens = self.density
kwargs = dict(gd=dens.gd,
finegd=dens.finegd,
nspins=dens.nspins,
collinear=dens.collinear,
setups=dens.setups,
timer=self.timer,
xc=xc,
world=self.world,
redistributor=dens.redistributor,
vext=self.parameters.external,
psolver=self.parameters.poissonsolver)
if realspace:
self.hamiltonian = RealSpaceHamiltonian(stencil=mode.interpolation,
**kwargs)
xc.set_grid_descriptor(self.hamiltonian.finegd)
else:
# This code will work if dens.redistributor uses
# ordinary density.gd as aux_gd
gd = dens.finegd
xc_redist = None
if self.parallel['augment_grids']:
from gpaw.grid_descriptor import BadGridError
try:
aux_gd = gd.new_descriptor(comm=self.world)
except BadGridError as err:
import warnings
warnings.warn('Ignoring augment_grids: {}'.format(err))
else:
bcast_comm = dens.redistributor.broadcast_comm
xc_redist = GridRedistributor(self.world, bcast_comm, gd,
aux_gd)
self.hamiltonian = pw.ReciprocalSpaceHamiltonian(
pd2=dens.pd2,
pd3=dens.pd3,
realpbc_c=self.atoms.pbc,
xc_redistributor=xc_redist,
**kwargs)
xc.set_grid_descriptor(self.hamiltonian.xc_gd)
self.hamiltonian.soc = self.parameters.experimental.get('soc')
self.log(self.hamiltonian, '\n')
def create_kpoint_descriptor(self, nspins):
par = self.parameters
bzkpts_kc = kpts2ndarray(par.kpts, self.atoms)
kpt_refine = par.experimental.get('kpt_refine')
if kpt_refine is None:
kd = KPointDescriptor(bzkpts_kc, nspins)
self.timer.start('Set symmetry')
kd.set_symmetry(self.atoms, self.symmetry, comm=self.world)
self.timer.stop('Set symmetry')
else:
self.timer.start('Set k-point refinement')
kd = create_kpoint_descriptor_with_refinement(kpt_refine,
bzkpts_kc,
nspins,
self.atoms,
self.symmetry,
comm=self.world,
timer=self.timer)
self.timer.stop('Set k-point refinement')
# Update quantities which might have changed, if symmetry
# was changed
self.symmetry = kd.symmetry
self.setups.set_symmetry(kd.symmetry)
self.log(kd)
return kd
def create_wave_functions(self, mode, realspace, nspins, collinear, nbands,
nao, nvalence, setups, cell_cv, pbc_c):
par = self.parameters
kd = self.create_kpoint_descriptor(nspins)
parallelization = mpi.Parallelization(self.world, nspins * kd.nibzkpts)
parsize_kpt = self.parallel['kpt']
parsize_domain = self.parallel['domain']
parsize_bands = self.parallel['band']
ndomains = None
if parsize_domain is not None:
ndomains = np.prod(parsize_domain)
parallelization.set(kpt=parsize_kpt,
domain=ndomains,
band=parsize_bands)
comms = parallelization.build_communicators()
domain_comm = comms['d']
kpt_comm = comms['k']
band_comm = comms['b']
kptband_comm = comms['D']
domainband_comm = comms['K']
self.comms = comms
if par.gpts is not None:
if par.h is not None:
raise ValueError("""You can't use both "gpts" and "h"!""")
N_c = np.array(par.gpts)
else:
h = par.h
if h is not None:
h /= Bohr
N_c = get_number_of_grid_points(cell_cv, h, mode, realspace,
kd.symmetry)
self.symmetry.check_grid(N_c)
kd.set_communicator(kpt_comm)
parstride_bands = self.parallel['stridebands']
bd = BandDescriptor(nbands, band_comm, parstride_bands)
# Construct grid descriptor for coarse grids for wave functions:
gd = self.create_grid_descriptor(N_c, cell_cv, pbc_c, domain_comm,
parsize_domain)
if hasattr(self, 'time') or mode.force_complex_dtype or not collinear:
dtype = complex
else:
if kd.gamma:
dtype = float
else:
dtype = complex
wfs_kwargs = dict(gd=gd,
nvalence=nvalence,
setups=setups,
bd=bd,
dtype=dtype,
world=self.world,
kd=kd,
kptband_comm=kptband_comm,
timer=self.timer)
if self.parallel['sl_auto']:
# Choose scalapack parallelization automatically
for key, val in self.parallel.items():
if (key.startswith('sl_') and key != 'sl_auto'
and val is not None):
raise ValueError("Cannot use 'sl_auto' together "
"with '%s'" % key)
max_scalapack_cpus = bd.comm.size * gd.comm.size
sl_default = suggest_blocking(nbands, max_scalapack_cpus)
else:
sl_default = self.parallel['sl_default']
if mode.name == 'lcao':
assert collinear
# Layouts used for general diagonalizer
sl_lcao = self.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
elpasolver = None
if self.parallel['use_elpa']:
elpasolver = self.parallel['elpasolver']
lcaoksl = get_KohnSham_layouts(sl_lcao,
'lcao',
gd,
bd,
domainband_comm,
dtype,
nao=nao,
timer=self.timer,
elpasolver=elpasolver)
self.wfs = mode(lcaoksl, **wfs_kwargs)
elif mode.name == 'fd' or mode.name == 'pw':
# Use (at most) all available LCAO for initialization
lcaonbands = min(nbands, nao)
try:
lcaobd = BandDescriptor(lcaonbands, band_comm, parstride_bands)
except RuntimeError:
initksl = None
else:
# Layouts used for general diagonalizer
# (LCAO initialization)
sl_lcao = self.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
initksl = get_KohnSham_layouts(sl_lcao,
'lcao',
gd,
lcaobd,
domainband_comm,
dtype,
nao=nao,
timer=self.timer)
reuse_wfs_method = par.experimental.get('reuse_wfs_method', 'paw')
sl = (domainband_comm, ) + (self.parallel['sl_diagonalize']
or sl_default or (1, 1, None))
self.wfs = mode(sl,
initksl,
reuse_wfs_method=reuse_wfs_method,
collinear=collinear,
**wfs_kwargs)
else:
self.wfs = mode(self, collinear=collinear, **wfs_kwargs)
self.log(self.wfs, '\n')
def dry_run(self):
# Can be overridden like in gpaw.atom.atompaw
print_cell(self.wfs.gd, self.atoms.pbc, self.log)
print_positions(self.atoms, self.log, self.density.magmom_av)
self.log.fd.flush()
# Write timing info now before the interpreter shuts down:
self.__del__()
# Disable timing output during shut-down:
del self.timer
raise SystemExit
class PAW(PAWTextOutput):
"""This is the main calculation object for doing a PAW calculation."""
def __init__(self,
filename=None,
timer=None,
read_projections=True,
**kwargs):
"""ASE-calculator interface.
The following parameters can be used: nbands, xc, kpts,
spinpol, gpts, h, charge, symmetry, width, mixer,
hund, lmax, fixdensity, convergence, txt, parallel,
communicator, dtype, softgauss and stencils.
If you don't specify any parameters, you will get:
Defaults: neutrally charged, LDA, gamma-point calculation, a
reasonable grid-spacing, zero Kelvin electronic temperature,
and the number of bands will be equal to the number of atomic
orbitals present in the setups. Only occupied bands are used
in the convergence decision. The calculation will be
spin-polarized if and only if one or more of the atoms have
non-zero magnetic moments. Text output will be written to
standard output.
For a non-gamma point calculation, the electronic temperature
will be 0.1 eV (energies are extrapolated to zero Kelvin) and
all symmetries will be used to reduce the number of
**k**-points."""
PAWTextOutput.__init__(self)
self.grid_descriptor_class = GridDescriptor
self.input_parameters = InputParameters()
if timer is None:
self.timer = Timer()
else:
self.timer = timer
self.scf = None
self.forces = ForceCalculator(self.timer)
self.stress_vv = None
self.dipole_v = None
self.magmom_av = None
self.wfs = EmptyWaveFunctions()
self.occupations = None
self.density = None
self.hamiltonian = None
self.atoms = None
self.iter = 0
self.initialized = False
self.nbands_parallelization_adjustment = None # Somehow avoid this?
# Possibly read GPAW keyword arguments from file:
if filename is not None and filename.endswith('.gkw'):
from gpaw.utilities.kwargs import load
parameters = load(filename)
parameters.update(kwargs)
kwargs = parameters
filename = None # XXX
if filename is not None:
comm = kwargs.get('communicator', mpi.world)
reader = gpaw.io.open(filename, 'r', comm)
self.atoms = gpaw.io.read_atoms(reader)
par = self.input_parameters
par.read(reader)
# _changed_keywords contains those keywords that have been
# changed by set() since last time initialize() was called.
self._changed_keywords = set()
self.set(**kwargs)
# Here in the beginning, effectively every keyword has been changed.
self._changed_keywords.update(self.input_parameters)
if filename is not None:
# Setups are not saved in the file if the setups were not loaded
# *from* files in the first place
if par.setups is None:
if par.idiotproof:
raise RuntimeError('Setups not specified in file. Use '
'idiotproof=False to proceed anyway.')
else:
par.setups = {None: 'paw'}
if par.basis is None:
if par.idiotproof:
raise RuntimeError('Basis not specified in file. Use '
'idiotproof=False to proceed anyway.')
else:
par.basis = {}
self.initialize()
self.read(reader, read_projections)
if self.hamiltonian.xc.type == 'GLLB':
self.occupations.calculate(self.wfs)
self.print_cell_and_parameters()
self.observers = []
def read(self, reader, read_projections=True):
gpaw.io.read(self, reader, read_projections)
def set(self, **kwargs):
"""Change parameters for calculator.
Examples::
calc.set(xc='PBE')
calc.set(nbands=20, kpts=(4, 1, 1))
"""
p = self.input_parameters
self._changed_keywords.update(kwargs)
if (kwargs.get('h') is not None) and (kwargs.get('gpts') is not None):
raise TypeError("""You can't use both "gpts" and "h"!""")
if 'h' in kwargs:
p['gpts'] = None
if 'gpts' in kwargs:
p['h'] = None
# Special treatment for dictionary parameters:
for name in ['convergence', 'parallel']:
if kwargs.get(name) is not None:
tmp = p[name]
for key in kwargs[name]:
if key not in tmp:
raise KeyError('Unknown subparameter "%s" in '
'dictionary parameter "%s"' %
(key, name))
tmp.update(kwargs[name])
kwargs[name] = tmp
self.initialized = False
for key in kwargs:
if key == 'basis' and str(p['mode']) == 'fd': # umm what about PW?
# The second criterion seems buggy, will not touch it. -Ask
continue
if key == 'eigensolver':
self.wfs.set_eigensolver(None)
if key in [
'fixmom', 'mixer', 'verbose', 'txt', 'hund', 'random',
'eigensolver', 'idiotproof', 'notify'
]:
continue
if key in ['convergence', 'fixdensity', 'maxiter']:
self.scf = None
continue
# More drastic changes:
self.scf = None
self.wfs.set_orthonormalized(False)
if key in [
'lmax', 'width', 'stencils', 'external', 'xc',
'poissonsolver'
]:
self.hamiltonian = None
self.occupations = None
elif key in ['occupations']:
self.occupations = None
elif key in ['charge']:
self.hamiltonian = None
self.density = None
self.wfs = EmptyWaveFunctions()
self.occupations = None
elif key in ['kpts', 'nbands', 'usesymm', 'symmetry']:
self.wfs = EmptyWaveFunctions()
self.occupations = None
elif key in [
'h', 'gpts', 'setups', 'spinpol', 'realspace', 'parallel',
'communicator', 'dtype', 'mode'
]:
self.density = None
self.occupations = None
self.hamiltonian = None
self.wfs = EmptyWaveFunctions()
elif key in ['basis']:
self.wfs = EmptyWaveFunctions()
elif key in ['parsize', 'parsize_bands', 'parstride_bands']:
name = {
'parsize': 'domain',
'parsize_bands': 'band',
'parstride_bands': 'stridebands'
}[key]
raise DeprecationWarning(
'Keyword argument has been moved ' +
"to the 'parallel' dictionary keyword under '%s'." % name)
else:
raise TypeError("Unknown keyword argument: '%s'" % key)
p.update(kwargs)
def calculate(self,
atoms=None,
converge=False,
force_call_to_set_positions=False):
"""Update PAW calculaton if needed.
Returns True/False whether a calculation was performed or not."""
self.timer.start('Initialization')
if atoms is None:
atoms = self.atoms
if self.atoms is None:
# First time:
self.initialize(atoms)
self.set_positions(atoms)
elif (len(atoms) != len(self.atoms)
or (atoms.get_atomic_numbers() !=
self.atoms.get_atomic_numbers()).any()
or (atoms.get_initial_magnetic_moments() !=
self.atoms.get_initial_magnetic_moments()).any()
or (atoms.get_cell() != self.atoms.get_cell()).any()
or (atoms.get_pbc() != self.atoms.get_pbc()).any()):
# Drastic changes:
self.wfs = EmptyWaveFunctions()
self.occupations = None
self.density = None
self.hamiltonian = None
self.scf = None
self.initialize(atoms)
self.set_positions(atoms)
elif not self.initialized:
self.initialize(atoms)
self.set_positions(atoms)
elif (atoms.get_positions() != self.atoms.get_positions()).any():
self.density.reset()
self.set_positions(atoms)
elif not self.scf.converged:
# Do not call scf.check_convergence() here as it overwrites
# scf.converged, and setting scf.converged is the only
# 'practical' way for a user to force the calculation to proceed
self.set_positions(atoms)
elif force_call_to_set_positions:
self.set_positions(atoms)
self.timer.stop('Initialization')
if self.scf.converged:
return False
else:
self.print_cell_and_parameters()
self.timer.start('SCF-cycle')
for iter in self.scf.run(self.wfs, self.hamiltonian, self.density,
self.occupations, self.forces):
self.iter = iter
self.call_observers(iter)
self.print_iteration(iter)
self.timer.stop('SCF-cycle')
if self.scf.converged:
self.call_observers(iter, final=True)
self.print_converged(iter)
elif converge:
self.txt.write(oops)
raise KohnShamConvergenceError(
'Did not converge! See text output for help.')
return True
def initialize_positions(self, atoms=None):
"""Update the positions of the atoms."""
if atoms is None:
atoms = self.atoms
else:
# Save the state of the atoms:
self.atoms = atoms.copy()
self.check_atoms()
spos_ac = atoms.get_scaled_positions() % 1.0
self.wfs.set_positions(spos_ac)
self.density.set_positions(spos_ac, self.wfs.rank_a)
self.hamiltonian.set_positions(spos_ac, self.wfs.rank_a)
return spos_ac
def set_positions(self, atoms=None):
"""Update the positions of the atoms and initialize wave functions."""
spos_ac = self.initialize_positions(atoms)
self.wfs.initialize(self.density, self.hamiltonian, spos_ac)
self.wfs.eigensolver.reset()
self.scf.reset()
self.forces.reset()
self.stress_vv = None
self.dipole_v = None
self.magmom_av = None
self.print_positions()
def initialize(self, atoms=None):
"""Inexpensive initialization."""
if atoms is None:
atoms = self.atoms
else:
# Save the state of the atoms:
self.atoms = atoms.copy()
par = self.input_parameters
world = par.communicator
if world is None:
world = mpi.world
elif hasattr(world, 'new_communicator'):
# Check for whether object has correct type already
#
# Using isinstance() is complicated because of all the
# combinations, serial/parallel/debug...
pass
else:
# world should be a list of ranks:
world = mpi.world.new_communicator(np.asarray(world))
self.wfs.world = world
if 'txt' in self._changed_keywords:
self.set_txt(par.txt)
self.verbose = par.verbose
natoms = len(atoms)
cell_cv = atoms.get_cell() / Bohr
pbc_c = atoms.get_pbc()
Z_a = atoms.get_atomic_numbers()
magmom_av = atoms.get_initial_magnetic_moments()
self.check_atoms()
# Generate new xc functional only when it is reset by set
# XXX sounds like this should use the _changed_keywords dictionary.
if self.hamiltonian is None or self.hamiltonian.xc is None:
if isinstance(par.xc, str):
xc = XC(par.xc)
else:
xc = par.xc
else:
xc = self.hamiltonian.xc
mode = par.mode
if mode == 'fd':
mode = FD()
elif mode == 'pw':
mode = pw.PW()
elif mode == 'lcao':
mode = LCAO()
else:
assert hasattr(mode, 'name'), str(mode)
if xc.orbital_dependent and mode.name == 'lcao':
raise NotImplementedError('LCAO mode does not support '
'orbital-dependent XC functionals.')
if par.realspace is None:
realspace = (mode.name != 'pw')
else:
realspace = par.realspace
if mode.name == 'pw':
assert not realspace
if par.filter is None and mode.name != 'pw':
gamma = 1.6
if par.gpts is not None:
h = ((np.linalg.inv(cell_cv)**2).sum(0)**-0.5 / par.gpts).max()
else:
h = (par.h or 0.2) / Bohr
def filter(rgd, rcut, f_r, l=0):
gcut = np.pi / h - 2 / rcut / gamma
f_r[:] = rgd.filter(f_r, rcut * gamma, gcut, l)
else:
filter = par.filter
setups = Setups(Z_a, par.setups, par.basis, par.lmax, xc, filter,
world)
if magmom_av.ndim == 1:
collinear = True
magmom_av, magmom_a = np.zeros((natoms, 3)), magmom_av
magmom_av[:, 2] = magmom_a
else:
collinear = False
magnetic = magmom_av.any()
spinpol = par.spinpol
if par.hund:
if natoms != 1:
raise ValueError('hund=True arg only valid for single atoms!')
spinpol = True
magmom_av[0] = (0, 0, setups[0].get_hunds_rule_moment(par.charge))
if spinpol is None:
spinpol = magnetic
elif magnetic and not spinpol:
raise ValueError('Non-zero initial magnetic moment for a ' +
'spin-paired calculation!')
if collinear:
nspins = 1 + int(spinpol)
ncomp = 1
else:
nspins = 1
ncomp = 2
if par.usesymm != 'default':
warnings.warn('Use "symmetry" keyword instead of ' +
'"usesymm" keyword')
par.symmetry = usesymm2symmetry(par.usesymm)
symm = par.symmetry
if symm == 'off':
symm = {'point_group': False, 'time_reversal': False}
bzkpts_kc = kpts2ndarray(par.kpts, self.atoms)
kd = KPointDescriptor(bzkpts_kc, nspins, collinear)
m_av = magmom_av.round(decimals=3) # round off
id_a = zip(setups.id_a, *m_av.T)
symmetry = Symmetry(id_a, cell_cv, atoms.pbc, **symm)
kd.set_symmetry(atoms, symmetry, comm=world)
setups.set_symmetry(symmetry)
if par.gpts is not None:
N_c = np.array(par.gpts)
else:
h = par.h
if h is not None:
h /= Bohr
N_c = get_number_of_grid_points(cell_cv, h, mode, realspace,
kd.symmetry)
symmetry.check_grid(N_c)
width = par.width
if width is None:
if pbc_c.any():
width = 0.1 # eV
else:
width = 0.0
else:
assert par.occupations is None
if hasattr(self, 'time') or par.dtype == complex:
dtype = complex
else:
if kd.gamma:
dtype = float
else:
dtype = complex
nao = setups.nao
nvalence = setups.nvalence - par.charge
M_v = magmom_av.sum(0)
M = np.dot(M_v, M_v)**0.5
nbands = par.nbands
orbital_free = any(setup.orbital_free for setup in setups)
if orbital_free:
nbands = 1
if isinstance(nbands, basestring):
if nbands[-1] == '%':
basebands = int(nvalence + M + 0.5) // 2
nbands = int((float(nbands[:-1]) / 100) * basebands)
else:
raise ValueError('Integer Expected: Only use a string '
'if giving a percentage of occupied bands')
if nbands is None:
nbands = 0
for setup in setups:
nbands_from_atom = setup.get_default_nbands()
# Any obscure setup errors?
if nbands_from_atom < -(-setup.Nv // 2):
raise ValueError('Bad setup: This setup requests %d'
' bands but has %d electrons.' %
(nbands_from_atom, setup.Nv))
nbands += nbands_from_atom
nbands = min(nao, nbands)
elif nbands > nao and mode.name == 'lcao':
raise ValueError('Too many bands for LCAO calculation: '
'%d bands and only %d atomic orbitals!' %
(nbands, nao))
if nvalence < 0:
raise ValueError(
'Charge %f is not possible - not enough valence electrons' %
par.charge)
if nbands <= 0:
nbands = int(nvalence + M + 0.5) // 2 + (-nbands)
if nvalence > 2 * nbands and not orbital_free:
raise ValueError('Too few bands! Electrons: %f, bands: %d' %
(nvalence, nbands))
nbands *= ncomp
if par.width is not None:
self.text('**NOTE**: please start using '
'occupations=FermiDirac(width).')
if par.fixmom:
self.text('**NOTE**: please start using '
'occupations=FermiDirac(width, fixmagmom=True).')
if self.occupations is None:
if par.occupations is None:
# Create object for occupation numbers:
if orbital_free:
width = 0.0 # even for PBC
self.occupations = occupations.TFOccupations(
width, par.fixmom)
else:
self.occupations = occupations.FermiDirac(
width, par.fixmom)
else:
self.occupations = par.occupations
# If occupation numbers are changed, and we have wave functions,
# recalculate the occupation numbers
if self.wfs is not None and not isinstance(self.wfs,
EmptyWaveFunctions):
self.occupations.calculate(self.wfs)
self.occupations.magmom = M_v[2]
cc = par.convergence
if mode.name == 'lcao':
niter_fixdensity = 0
else:
niter_fixdensity = None
if self.scf is None:
force_crit = cc['forces']
if force_crit is not None:
force_crit /= Hartree / Bohr
self.scf = SCFLoop(cc['eigenstates'] / Hartree**2 * nvalence,
cc['energy'] / Hartree * max(nvalence, 1),
cc['density'] * nvalence, par.maxiter,
par.fixdensity, niter_fixdensity, force_crit)
parsize_kpt = par.parallel['kpt']
parsize_domain = par.parallel['domain']
parsize_bands = par.parallel['band']
if not realspace:
pbc_c = np.ones(3, bool)
if not self.wfs:
if parsize_domain == 'domain only': # XXX this was silly!
parsize_domain = world.size
parallelization = mpi.Parallelization(world, nspins * kd.nibzkpts)
ndomains = None
if parsize_domain is not None:
ndomains = np.prod(parsize_domain)
if mode.name == 'pw':
if ndomains > 1:
raise ValueError('Planewave mode does not support '
'domain decomposition.')
ndomains = 1
parallelization.set(kpt=parsize_kpt,
domain=ndomains,
band=parsize_bands)
comms = parallelization.build_communicators()
domain_comm = comms['d']
kpt_comm = comms['k']
band_comm = comms['b']
kptband_comm = comms['D']
domainband_comm = comms['K']
self.comms = comms
kd.set_communicator(kpt_comm)
parstride_bands = par.parallel['stridebands']
# Unfortunately we need to remember that we adjusted the
# number of bands so we can print a warning if it differs
# from the number specified by the user. (The number can
# be inferred from the input parameters, but it's tricky
# because we allow negative numbers)
self.nbands_parallelization_adjustment = -nbands % band_comm.size
nbands += self.nbands_parallelization_adjustment
# I would like to give the following error message, but apparently
# there are cases, e.g. gpaw/test/gw_ppa.py, which involve
# nbands > nao and are supposed to work that way.
#if nbands > nao:
# raise ValueError('Number of bands %d adjusted for band '
# 'parallelization %d exceeds number of atomic '
# 'orbitals %d. This problem can be fixed '
# 'by reducing the number of bands a bit.'
# % (nbands, band_comm.size, nao))
bd = BandDescriptor(nbands, band_comm, parstride_bands)
if (self.density is not None
and self.density.gd.comm.size != domain_comm.size):
# Domain decomposition has changed, so we need to
# reinitialize density and hamiltonian:
if par.fixdensity:
raise RuntimeError(
'Density reinitialization conflict ' +
'with "fixdensity" - specify domain decomposition.')
self.density = None
self.hamiltonian = None
# Construct grid descriptor for coarse grids for wave functions:
gd = self.grid_descriptor_class(N_c, cell_cv, pbc_c, domain_comm,
parsize_domain)
# do k-point analysis here? XXX
args = (gd, nvalence, setups, bd, dtype, world, kd, kptband_comm,
self.timer)
if par.parallel['sl_auto']:
# Choose scalapack parallelization automatically
for key, val in par.parallel.items():
if (key.startswith('sl_') and key != 'sl_auto'
and val is not None):
raise ValueError("Cannot use 'sl_auto' together "
"with '%s'" % key)
max_scalapack_cpus = bd.comm.size * gd.comm.size
nprow = max_scalapack_cpus
npcol = 1
# Get a sort of reasonable number of columns/rows
while npcol < nprow and nprow % 2 == 0:
npcol *= 2
nprow //= 2
assert npcol * nprow == max_scalapack_cpus
# ScaLAPACK creates trouble if there aren't at least a few
# whole blocks; choose block size so there will always be
# several blocks. This will crash for small test systems,
# but so will ScaLAPACK in any case
blocksize = min(-(-nbands // 4), 64)
sl_default = (nprow, npcol, blocksize)
else:
sl_default = par.parallel['sl_default']
if mode.name == 'lcao':
# Layouts used for general diagonalizer
sl_lcao = par.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
lcaoksl = get_KohnSham_layouts(sl_lcao,
'lcao',
gd,
bd,
domainband_comm,
dtype,
nao=nao,
timer=self.timer)
self.wfs = mode(collinear, lcaoksl, *args)
elif mode.name == 'fd' or mode.name == 'pw':
# buffer_size keyword only relevant for fdpw
buffer_size = par.parallel['buffer_size']
# Layouts used for diagonalizer
sl_diagonalize = par.parallel['sl_diagonalize']
if sl_diagonalize is None:
sl_diagonalize = sl_default
diagksl = get_KohnSham_layouts(
sl_diagonalize,
'fd', # XXX
# choice of key 'fd' not so nice
gd,
bd,
domainband_comm,
dtype,
buffer_size=buffer_size,
timer=self.timer)
# Layouts used for orthonormalizer
sl_inverse_cholesky = par.parallel['sl_inverse_cholesky']
if sl_inverse_cholesky is None:
sl_inverse_cholesky = sl_default
if sl_inverse_cholesky != sl_diagonalize:
message = 'sl_inverse_cholesky != sl_diagonalize ' \
'is not implemented.'
raise NotImplementedError(message)
orthoksl = get_KohnSham_layouts(sl_inverse_cholesky,
'fd',
gd,
bd,
domainband_comm,
dtype,
buffer_size=buffer_size,
timer=self.timer)
# Use (at most) all available LCAO for initialization
lcaonbands = min(nbands, nao)
try:
lcaobd = BandDescriptor(lcaonbands, band_comm,
parstride_bands)
except RuntimeError:
initksl = None
else:
# Layouts used for general diagonalizer
# (LCAO initialization)
sl_lcao = par.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
initksl = get_KohnSham_layouts(sl_lcao,
'lcao',
gd,
lcaobd,
domainband_comm,
dtype,
nao=nao,
timer=self.timer)
if hasattr(self, 'time'):
assert mode.name == 'fd'
from gpaw.tddft import TimeDependentWaveFunctions
self.wfs = TimeDependentWaveFunctions(
par.stencils[0], diagksl, orthoksl, initksl, gd,
nvalence, setups, bd, world, kd, kptband_comm,
self.timer)
elif mode.name == 'fd':
self.wfs = mode(par.stencils[0], diagksl, orthoksl,
initksl, *args)
else:
assert mode.name == 'pw'
self.wfs = mode(diagksl, orthoksl, initksl, *args)
else:
self.wfs = mode(self, *args)
else:
self.wfs.set_setups(setups)
if not self.wfs.eigensolver:
# Number of bands to converge:
nbands_converge = cc['bands']
if nbands_converge == 'all':
nbands_converge = nbands
elif nbands_converge != 'occupied':
assert isinstance(nbands_converge, int)
if nbands_converge < 0:
nbands_converge += nbands
eigensolver = get_eigensolver(par.eigensolver, mode,
par.convergence)
eigensolver.nbands_converge = nbands_converge
# XXX Eigensolver class doesn't define an nbands_converge property
if isinstance(xc, SIC):
eigensolver.blocksize = 1
self.wfs.set_eigensolver(eigensolver)
if self.density is None:
gd = self.wfs.gd
if par.stencils[1] != 9:
# Construct grid descriptor for fine grids for densities
# and potentials:
finegd = gd.refine()
else:
# Special case (use only coarse grid):
finegd = gd
if realspace:
self.density = RealSpaceDensity(
gd, finegd, nspins, par.charge + setups.core_charge,
collinear, par.stencils[1])
else:
self.density = pw.ReciprocalSpaceDensity(
gd, finegd, nspins, par.charge + setups.core_charge,
collinear)
self.density.initialize(setups, self.timer, magmom_av, par.hund)
self.density.set_mixer(par.mixer)
if self.hamiltonian is None:
gd, finegd = self.density.gd, self.density.finegd
if realspace:
self.hamiltonian = RealSpaceHamiltonian(
gd, finegd, nspins, setups, self.timer, xc, world,
self.wfs.kptband_comm, par.external, collinear,
par.poissonsolver, par.stencils[1])
else:
self.hamiltonian = pw.ReciprocalSpaceHamiltonian(
gd, finegd, self.density.pd2, self.density.pd3, nspins,
setups, self.timer, xc, world, self.wfs.kptband_comm,
par.external, collinear)
xc.initialize(self.density, self.hamiltonian, self.wfs,
self.occupations)
self.text()
self.print_memory_estimate(self.txt, maxdepth=memory_estimate_depth)
self.txt.flush()
self.timer.print_info(self)
if dry_run:
self.dry_run()
if realspace and \
self.hamiltonian.poisson.get_description() == 'FDTD+TDDFT':
self.hamiltonian.poisson.set_density(self.density)
self.hamiltonian.poisson.print_messages(self.text)
self.txt.flush()
self.initialized = True
self._changed_keywords.clear()
def dry_run(self):
# Can be overridden like in gpaw.atom.atompaw
self.print_cell_and_parameters()
self.print_positions()
self.txt.flush()
raise SystemExit
def linearize_to_xc(self, newxc):
"""Linearize Hamiltonian to difference XC functional.
Used in real time TDDFT to perform calculations with various kernels.
"""
if isinstance(newxc, str):
newxc = XC(newxc)
self.txt.write('Linearizing xc-hamiltonian to ' + str(newxc))
newxc.initialize(self.density, self.hamiltonian, self.wfs,
self.occupations)
self.hamiltonian.linearize_to_xc(newxc, self.density)
def restore_state(self):
"""After restart, calculate fine density and poisson solution.
These are not initialized by default.
TODO: Is this really the most efficient way?
"""
spos_ac = self.atoms.get_scaled_positions() % 1.0
self.density.set_positions(spos_ac, self.wfs.rank_a)
self.density.interpolate_pseudo_density()
self.density.calculate_pseudo_charge()
self.hamiltonian.set_positions(spos_ac, self.wfs.rank_a)
self.hamiltonian.update(self.density)
def attach(self, function, n=1, *args, **kwargs):
"""Register observer function.
Call *function* using *args* and
*kwargs* as arguments.
If *n* is positive, then
*function* will be called every *n* iterations + the
final iteration if it would not be otherwise
If *n* is negative, then *function* will only be
called on iteration *abs(n)*.
If *n* is 0, then *function* will only be called
on convergence"""
try:
slf = function.im_self
except AttributeError:
pass
else:
if slf is self:
# function is a bound method of self. Store the name
# of the method and avoid circular reference:
function = function.im_func.func_name
self.observers.append((function, n, args, kwargs))
def call_observers(self, iter, final=False):
"""Call all registered callback functions."""
for function, n, args, kwargs in self.observers:
call = False
# Call every n iterations, including the last
if n > 0:
if ((iter % n) == 0) != final:
call = True
# Call only on iteration n
elif n < 0 and not final:
if iter == abs(n):
call = True
# Call only on convergence
elif n == 0 and final:
call = True
if call:
if isinstance(function, str):
function = getattr(self, function)
function(*args, **kwargs)
def get_reference_energy(self):
return self.wfs.setups.Eref * Hartree
def write(self, filename, mode='', cmr_params={}, **kwargs):
"""Write state to file.
use mode='all' to write the wave functions. cmr_params is a
dictionary that allows you to specify parameters for CMR
(Computational Materials Repository).
"""
self.timer.start('IO')
gpaw.io.write(self, filename, mode, cmr_params=cmr_params, **kwargs)
self.timer.stop('IO')
def get_myu(self, k, s):
"""Return my u corresponding to a certain kpoint and spin - or None"""
# very slow, but we are sure that we have it
for u in range(len(self.wfs.kpt_u)):
if self.wfs.kpt_u[u].k == k and self.wfs.kpt_u[u].s == s:
return u
return None
def get_homo_lumo(self):
"""Return H**O and LUMO eigenvalues."""
return self.occupations.get_homo_lumo(self.wfs) * Hartree
def estimate_memory(self, mem):
"""Estimate memory use of this object."""
for name, obj in [
('Density', self.density),
('Hamiltonian', self.hamiltonian),
('Wavefunctions', self.wfs),
]:
obj.estimate_memory(mem.subnode(name))
def print_memory_estimate(self, txt=None, maxdepth=-1):
"""Print estimated memory usage for PAW object and components.
maxdepth is the maximum nesting level of displayed components.
The PAW object must be initialize()'d, but needs not have large
arrays allocated."""
# NOTE. This should work with --dry-run=N
#
# However, the initial overhead estimate is wrong if this method
# is called within a real mpirun/gpaw-python context.
if txt is None:
txt = self.txt
txt.write('Memory estimate\n')
txt.write('---------------\n')
mem_init = maxrss() # initial overhead includes part of Hamiltonian!
txt.write('Process memory now: %.2f MiB\n' % (mem_init / 1024.0**2))
mem = MemNode('Calculator', 0)
try:
self.estimate_memory(mem)
except AttributeError as m:
txt.write('Attribute error: %r' % m)
txt.write('Some object probably lacks estimate_memory() method')
txt.write('Memory breakdown may be incomplete')
mem.calculate_size()
mem.write(txt, maxdepth=maxdepth)
def converge_wave_functions(self):
"""Converge the wave-functions if not present."""
if not self.wfs or not self.scf:
self.initialize()
else:
self.wfs.initialize_wave_functions_from_restart_file()
spos_ac = self.atoms.get_scaled_positions() % 1.0
self.wfs.set_positions(spos_ac)
no_wave_functions = (self.wfs.kpt_u[0].psit_nG is None)
converged = self.scf.check_convergence(self.density,
self.wfs.eigensolver, self.wfs,
self.hamiltonian, self.forces)
if no_wave_functions or not converged:
self.wfs.eigensolver.error = np.inf
self.scf.converged = False
# is the density ok ?
error = self.density.mixer.get_charge_sloshing()
criterion = (self.input_parameters['convergence']['density'] *
self.wfs.nvalence)
if error < criterion and not self.hamiltonian.xc.orbital_dependent:
self.scf.fix_density()
self.calculate()
def diagonalize_full_hamiltonian(self,
nbands=None,
scalapack=None,
expert=False):
self.wfs.diagonalize_full_hamiltonian(self.hamiltonian, self.atoms,
self.occupations, self.txt,
nbands, scalapack, expert)
def check_atoms(self):
"""Check that atoms objects are identical on all processors."""
if not mpi.compare_atoms(self.atoms, comm=self.wfs.world):
raise RuntimeError('Atoms objects on different processors ' +
'are not identical!')
class ResonantRaman(Vibrations):
"""Class for calculating vibrational modes and
resonant Raman intensities using finite difference.
atoms:
Atoms object
Excitations:
Class to calculate the excitations. The class object is
initialized as::
Excitations(atoms.get_calculator())
or by reading form a file as::
Excitations('filename', **exkwargs)
The file is written by calling the method
Excitations.write('filename').
Excitations should work like a list of ex obejects, where:
ex.get_dipole_me(form='v'):
gives the dipole matrix element in |e| * Angstrom
ex.energy:
is the transition energy in Hartrees
"""
def __init__(
self,
atoms,
Excitations,
indices=None,
gsname='rraman', # name for ground state calculations
exname=None, # name for excited state calculations
delta=0.01,
nfree=2,
directions=None,
approximation='Profeta',
observation={'geometry': '-Z(XX)Z'},
exkwargs={}, # kwargs to be passed to Excitations
exext='.ex.gz', # extension for Excitation names
txt='-',
verbose=False,
):
assert (nfree == 2)
Vibrations.__init__(self, atoms, indices, gsname, delta, nfree)
self.name = gsname + '-d%.3f' % delta
if exname is None:
exname = gsname
self.exname = exname + '-d%.3f' % delta
self.exext = exext
if directions is None:
self.directions = np.array([0, 1, 2])
else:
self.directions = np.array(directions)
self.approximation = approximation
self.observation = observation
self.exobj = Excitations
self.exkwargs = exkwargs
self.timer = Timer()
self.txt = convert_string_to_fd(txt)
self.verbose = verbose
@staticmethod
def m2(z):
return (z * z.conj()).real
def log(self, message, pre='# ', end='\n'):
if self.verbose:
self.txt.write(pre + message + end)
self.txt.flush()
def calculate(self, filename, fd):
"""Call ground and excited state calculation"""
self.timer.start('Ground state')
forces = self.atoms.get_forces()
if rank == 0:
pickle.dump(forces, fd, protocol=2)
fd.close()
self.timer.stop('Ground state')
self.timer.start('Excitations')
basename, _ = os.path.splitext(filename)
excitations = self.exobj(self.atoms.get_calculator(), **self.exkwargs)
excitations.write(basename + self.exext)
self.timer.stop('Excitations')
def read_excitations(self):
self.timer.start('read excitations')
self.timer.start('really read')
self.log('reading ' + self.exname + '.eq' + self.exext)
ex0_object = self.exobj(self.exname + '.eq' + self.exext,
**self.exkwargs)
self.timer.stop('really read')
self.timer.start('index')
matching = frozenset(ex0_object)
self.timer.stop('index')
def append(lst, exname, matching):
self.timer.start('really read')
self.log('reading ' + exname, end=' ')
exo = self.exobj(exname, **self.exkwargs)
lst.append(exo)
self.timer.stop('really read')
self.timer.start('index')
matching = matching.intersection(exo)
self.log('len={0}, matching={1}'.format(len(exo), len(matching)),
pre='')
self.timer.stop('index')
return matching
exm_object_list = []
exp_object_list = []
for a in self.indices:
for i in 'xyz':
name = '%s.%d%s' % (self.exname, a, i)
matching = append(exm_object_list, name + '-' + self.exext,
matching)
matching = append(exp_object_list, name + '+' + self.exext,
matching)
self.ndof = 3 * len(self.indices)
self.nex = len(matching)
self.timer.stop('read excitations')
self.timer.start('select')
def select(exl, matching):
mlst = [ex for ex in exl if ex in matching]
assert (len(mlst) == len(matching))
return mlst
ex0 = select(ex0_object, matching)
exm = []
exp = []
r = 0
for a in self.indices:
for i in 'xyz':
exm.append(select(exm_object_list[r], matching))
exp.append(select(exp_object_list[r], matching))
r += 1
self.timer.stop('select')
self.timer.start('me and energy')
eu = units.Hartree
self.ex0E_p = np.array([ex.energy * eu for ex in ex0])
self.ex0m_pc = np.array([ex.get_dipole_me(form='v') for ex in ex0])
exmE_rp = []
expE_rp = []
exF_rp = []
exmm_rpc = []
expm_rpc = []
r = 0
for a in self.indices:
for i in 'xyz':
exmE_rp.append([em.energy for em in exm[r]])
expE_rp.append([ep.energy for ep in exp[r]])
exF_rp.append([(ep.energy - em.energy)
for ep, em in zip(exp[r], exm[r])])
exmm_rpc.append([ex.get_dipole_me(form='v') for ex in exm[r]])
expm_rpc.append([ex.get_dipole_me(form='v') for ex in exp[r]])
r += 1
self.exmE_rp = np.array(exmE_rp) * eu
self.expE_rp = np.array(expE_rp) * eu
self.exF_rp = np.array(exF_rp) * eu / 2 / self.delta
self.exmm_rpc = np.array(exmm_rpc)
self.expm_rpc = np.array(expm_rpc)
self.timer.stop('me and energy')
def read(self, method='standard', direction='central'):
"""Read data from a pre-performed calculation."""
if not hasattr(self, 'modes'):
self.timer.start('read vibrations')
Vibrations.read(self, method, direction)
# we now have:
# self.H : Hessian matrix
# self.im : 1./sqrt(masses)
# self.modes : Eigenmodes of the mass weighted H
self.om_r = self.hnu.real # energies in eV
self.timer.stop('read vibrations')
if not hasattr(self, 'ex0E_p'):
self.read_excitations()
def get_Huang_Rhys_factors(self, forces_r):
"""Evaluate Huang-Rhys factors derived from forces."""
self.timer.start('Huang-Rhys')
assert (len(forces_r.flat) == self.ndof)
# solve the matrix equation for the equilibrium displacements
# XXX why are the forces mass weighted ???
X_r = np.linalg.solve(self.im[:, None] * self.H * self.im,
forces_r.flat * self.im)
d_r = np.dot(self.modes, X_r)
# Huang-Rhys factors S
s = 1.e-20 / units.kg / units.C / units._hbar**2 # SI units
self.timer.stop('Huang-Rhys')
return s * d_r**2 * self.om_r / 2.
def get_matrix_element_AlbrechtA(self, omega, gamma=0.1, ml=range(16)):
"""Evaluate Albrecht A term.
Unit: |e|^2Angstrom^2/eV
"""
self.read()
self.timer.start('AlbrechtA')
if not hasattr(self, 'fco'):
self.fco = FranckCondonOverlap()
# excited state forces
F_pr = self.exF_rp.T
m_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
for p, energy in enumerate(self.ex0E_p):
S_r = self.get_Huang_Rhys_factors(F_pr[p])
me_cc = np.outer(self.ex0m_pc[p], self.ex0m_pc[p].conj())
for m in ml:
self.timer.start('0mm1')
fco_r = self.fco.direct0mm1(m, S_r)
self.timer.stop('0mm1')
self.timer.start('einsum')
m_rcc += np.einsum(
'a,bc->abc',
fco_r / (energy + m * self.om_r - omega - 1j * gamma),
me_cc)
m_rcc += np.einsum(
'a,bc->abc', fco_r /
(energy + (m - 1) * self.om_r + omega + 1j * gamma), me_cc)
self.timer.stop('einsum')
self.timer.stop('AlbrechtA')
return m_rcc
def get_matrix_element_AlbrechtBC(self,
omega,
gamma=0.1,
ml=[1],
term='BC'):
"""Evaluate Albrecht B and/or C term(s)."""
self.read()
self.timer.start('AlbrechtBC')
if not hasattr(self, 'fco'):
self.fco = FranckCondonOverlap()
# excited state forces
F_pr = self.exF_rp.T
m_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
for p, energy in enumerate(self.ex0E_p):
S_r = self.get_Huang_Rhys_factors(F_pr[p])
for m in ml:
self.timer.start('Franck-Condon overlaps')
fc1mm1_r = self.fco.direct(1, m, S_r)
fc0mm02_r = self.fco.direct(0, m, S_r)
fc0mm02_r += np.sqrt(2) * self.fco.direct0mm2(m, S_r)
# XXXXX
fc1mm1_r[-1] = 1
fc0mm02_r[-1] = 1
print(m, fc1mm1_r[-1], fc0mm02_r[-1])
self.timer.stop('Franck-Condon overlaps')
self.timer.start('me dervivatives')
dm_rc = []
r = 0
for a in self.indices:
for i in 'xyz':
dm_rc.append(
(self.expm_rpc[r, p] - self.exmm_rpc[r, p]) *
self.im[r])
print('pm=', self.expm_rpc[r, p], self.exmm_rpc[r, p])
r += 1
dm_rc = np.array(dm_rc) / (2 * self.delta)
self.timer.stop('me dervivatives')
self.timer.start('map to modes')
# print('dm_rc[2], dm_rc[5]', dm_rc[2], dm_rc[5])
print('dm_rc=', dm_rc)
dm_rc = np.dot(dm_rc.T, self.modes.T).T
print('dm_rc[-1][2]', dm_rc[-1][2])
self.timer.stop('map to modes')
self.timer.start('multiply')
# me_cc = np.outer(self.ex0m_pc[p], self.ex0m_pc[p].conj())
for r in range(self.ndof):
if 'B' in term:
# XXXX
denom = (1. / (energy + m * 0 * self.om_r[r] - omega -
1j * gamma))
# ok print('denom=', denom)
m_rcc[r] += (
np.outer(dm_rc[r], self.ex0m_pc[p].conj()) *
fc1mm1_r[r] * denom)
if r == 5:
print('m_rcc[r]=', m_rcc[r][2, 2])
m_rcc[r] += (
np.outer(self.ex0m_pc[p], dm_rc[r].conj()) *
fc0mm02_r[r] * denom)
if 'C' in term:
denom = (1. /
(energy +
(m - 1) * self.om_r[r] + omega + 1j * gamma))
m_rcc[r] += (
np.outer(self.ex0m_pc[p], dm_rc[r].conj()) *
fc1mm1_r[r] * denom)
m_rcc[r] += (
np.outer(dm_rc[r], self.ex0m_pc[p].conj()) *
fc0mm02_r[r] * denom)
self.timer.stop('multiply')
print('m_rcc[-1]=', m_rcc[-1][2, 2])
self.timer.start('pre_r')
with np.errstate(divide='ignore'):
pre_r = np.where(self.om_r > 0,
np.sqrt(units._hbar**2 / 2. / self.om_r), 0)
# print('BC: pre_r=', pre_r)
for r, p in enumerate(pre_r):
m_rcc[r] *= p
self.timer.stop('pre_r')
self.timer.stop('AlbrechtBC')
return m_rcc
def get_matrix_element_Profeta(self,
omega,
gamma=0.1,
energy_derivative=False):
"""Evaluate Albrecht B+C term in Profeta and Mauri approximation"""
self.read()
self.timer.start('amplitudes')
self.timer.start('init')
V_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
pre = 1. / (2 * self.delta)
self.timer.stop('init')
def kappa(me_pc, e_p, omega, gamma, form='v'):
"""Kappa tensor after Profeta and Mauri
PRB 63 (2001) 245415"""
me_ccp = np.empty((3, 3, len(e_p)), dtype=complex)
for p, me_c in enumerate(me_pc):
me_ccp[:, :, p] = np.outer(me_pc[p], me_pc[p].conj())
# print('kappa: me_ccp=', me_ccp[2,2,0])
# ok print('kappa: den=', 1./(e_p - omega - 1j * gamma))
kappa_ccp = (me_ccp / (e_p - omega - 1j * gamma) + me_ccp.conj() /
(e_p + omega + 1j * gamma))
return kappa_ccp.sum(2)
self.timer.start('kappa')
r = 0
for a in self.indices:
for i in 'xyz':
if not energy_derivative < 0:
V_rcc[r] = pre * self.im[r] * (
kappa(self.expm_rpc[r], self.ex0E_p, omega, gamma) -
kappa(self.exmm_rpc[r], self.ex0E_p, omega, gamma))
if energy_derivative:
V_rcc[r] += pre * self.im[r] * (
kappa(self.ex0m_pc, self.expE_rp[r], omega, gamma) -
kappa(self.ex0m_pc, self.exmE_rp[r], omega, gamma))
r += 1
self.timer.stop('kappa')
# print('V_rcc[2], V_rcc[5]=', V_rcc[2,2,2], V_rcc[5,2,2])
self.timer.stop('amplitudes')
# map to modes
self.timer.start('pre_r')
with np.errstate(divide='ignore'):
pre_r = np.where(self.om_r > 0,
np.sqrt(units._hbar**2 / 2. / self.om_r), 0)
V_rcc = np.dot(V_rcc.T, self.modes.T).T
# looks ok print('self.modes.T[-1]',self.modes.T)
# looks ok print('V_rcc[-1]=', V_rcc[-1][2,2])
# ok print('Profeta: pre_r=', pre_r)
for r, p in enumerate(pre_r):
V_rcc[r] *= p
self.timer.stop('pre_r')
return V_rcc
def get_matrix_element(self, omega, gamma):
self.read()
V_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
if self.approximation.lower() == 'profeta':
V_rcc += self.get_matrix_element_Profeta(omega, gamma)
elif self.approximation.lower() == 'placzek':
V_rcc += self.get_matrix_element_Profeta(omega, gamma, True)
elif self.approximation.lower() == 'p-p':
V_rcc += self.get_matrix_element_Profeta(omega, gamma, -1)
elif self.approximation.lower() == 'albrecht a':
V_rcc += self.get_matrix_element_AlbrechtA(omega, gamma)
elif self.approximation.lower() == 'albrecht b':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma, term='B')
elif self.approximation.lower() == 'albrecht c':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma, term='C')
elif self.approximation.lower() == 'albrecht bc':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma)
elif self.approximation.lower() == 'albrecht':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtA(omega, gamma)
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma)
elif self.approximation.lower() == 'albrecht+profeta':
V_rcc += self.get_matrix_element_AlbrechtA(omega, gamma)
V_rcc += self.get_matrix_element_Profeta(omega, gamma)
else:
raise NotImplementedError(
'Approximation {0} not implemented. '.format(
self.approximation) +
'Please use "Profeta", "Albrecht A/B/C/BC", ' +
'or "Albrecht".')
return V_rcc
def get_intensities(self, omega, gamma=0.1):
m2 = ResonantRaman.m2
alpha_rcc = self.get_matrix_element(omega, gamma)
if not self.observation: # XXXX remove
"""Simple sum, maybe too simple"""
return m2(alpha_rcc).sum(axis=1).sum(axis=1)
# XXX enable when appropraiate
# if self.observation['orientation'].lower() != 'random':
# raise NotImplementedError('not yet')
# random orientation of the molecular frame
# Woodward & Long,
# Guthmuller, J. J. Chem. Phys. 2016, 144 (6), 64106
m2 = ResonantRaman.m2
alpha2_r = m2(alpha_rcc[:, 0, 0] + alpha_rcc[:, 1, 1] +
alpha_rcc[:, 2, 2]) / 9.
delta2_r = 3 / 4. * (m2(alpha_rcc[:, 0, 1] - alpha_rcc[:, 1, 0]) +
m2(alpha_rcc[:, 0, 2] - alpha_rcc[:, 2, 0]) +
m2(alpha_rcc[:, 1, 2] - alpha_rcc[:, 2, 1]))
gamma2_r = (3 / 4. * (m2(alpha_rcc[:, 0, 1] + alpha_rcc[:, 1, 0]) +
m2(alpha_rcc[:, 0, 2] + alpha_rcc[:, 2, 0]) +
m2(alpha_rcc[:, 1, 2] + alpha_rcc[:, 2, 1])) +
(m2(alpha_rcc[:, 0, 0] - alpha_rcc[:, 1, 1]) +
m2(alpha_rcc[:, 0, 0] - alpha_rcc[:, 2, 2]) +
m2(alpha_rcc[:, 1, 1] - alpha_rcc[:, 2, 2])) / 2)
if self.observation['geometry'] == '-Z(XX)Z': # Porto's notation
return (45 * alpha2_r + 5 * delta2_r + 4 * gamma2_r) / 45.
elif self.observation['geometry'] == '-Z(XY)Z': # Porto's notation
return gamma2_r / 15.
elif self.observation['scattered'] == 'Z':
# scattered light in direction of incoming light
return (45 * alpha2_r + 5 * delta2_r + 7 * gamma2_r) / 45.
elif self.observation['scattered'] == 'parallel':
# scattered light perendicular and
# polarization in plane
return 6 * gamma2_r / 45.
elif self.observation['scattered'] == 'perpendicular':
# scattered light perendicular and
# polarization out of plane
return (45 * alpha2_r + 5 * delta2_r + 7 * gamma2_r) / 45.
else:
raise NotImplementedError
def get_cross_sections(self, omega, gamma=0.1):
I_r = self.get_intensities(omega, gamma)
pre = 1. / 16 / np.pi**2 / units.eps0**2 / units.c**4
# frequency of scattered light
omS_r = omega - self.hnu
return pre * omega * omS_r**3 * I_r
def get_spectrum(self,
omega,
gamma=0.1,
start=200.0,
end=4000.0,
npts=None,
width=4.0,
type='Gaussian',
method='standard',
direction='central',
intensity_unit='????',
normalize=False):
"""Get resonant Raman spectrum.
The method returns wavenumbers in cm^-1 with corresponding
Raman cross section.
Start and end point, and width of the Gaussian/Lorentzian should
be given in cm^-1.
"""
self.type = type.lower()
assert self.type in ['gaussian', 'lorentzian']
if not npts:
npts = int((end - start) / width * 10 + 1)
frequencies = self.get_frequencies(method, direction).real
intensities = self.get_cross_sections(omega, gamma)
prefactor = 1
if type == 'lorentzian':
intensities = intensities * width * np.pi / 2.
if normalize:
prefactor = 2. / width / np.pi
else:
sigma = width / 2. / np.sqrt(2. * np.log(2.))
if normalize:
prefactor = 1. / sigma / np.sqrt(2 * np.pi)
# Make array with spectrum data
spectrum = np.empty(npts)
energies = np.linspace(start, end, npts)
for i, energy in enumerate(energies):
energies[i] = energy
if type == 'lorentzian':
spectrum[i] = (intensities * 0.5 * width / np.pi / (
(frequencies - energy)**2 + 0.25 * width**2)).sum()
else:
spectrum[i] = (
intensities *
np.exp(-(frequencies - energy)**2 / 2. / sigma**2)).sum()
return [energies, prefactor * spectrum]
def write_spectrum(self,
omega,
gamma,
out='resonant-raman-spectra.dat',
start=200,
end=4000,
npts=None,
width=10,
type='Gaussian',
method='standard',
direction='central'):
"""Write out spectrum to file.
First column is the wavenumber in cm^-1, the second column the
absolute infrared intensities, and
the third column the absorbance scaled so that data runs
from 1 to 0. Start and end
point, and width of the Gaussian/Lorentzian should be given
in cm^-1."""
energies, spectrum = self.get_spectrum(omega, gamma, start, end, npts,
width, type, method, direction)
# Write out spectrum in file. First column is absolute intensities.
outdata = np.empty([len(energies), 3])
outdata.T[0] = energies
outdata.T[1] = spectrum
fd = open(out, 'w')
fd.write('# Resonant Raman spectrum\n')
fd.write('# omega={0:g} eV, gamma={1:g} eV\n'.format(omega, gamma))
fd.write('# %s folded, width=%g cm^-1\n' % (type.title(), width))
fd.write('# [cm^-1] [a.u.]\n')
for row in outdata:
fd.write('%.3f %15.5g\n' % (row[0], row[1]))
fd.close()
def summary(self,
omega,
gamma=0.1,
method='standard',
direction='central',
log=sys.stdout):
"""Print summary for given omega [eV]"""
hnu = self.get_energies(method, direction)
s = 0.01 * units._e / units._c / units._hplanck
intensities = self.get_intensities(omega, gamma)
if isinstance(log, basestring):
log = paropen(log, 'a')
parprint('-------------------------------------', file=log)
parprint(' excitation at ' + str(omega) + ' eV', file=log)
parprint(' gamma ' + str(gamma) + ' eV', file=log)
parprint(' approximation:', self.approximation, file=log)
parprint(' observation:', self.observation, '\n', file=log)
parprint(' Mode Frequency Intensity', file=log)
parprint(' # meV cm^-1 [e^4A^4/eV^2]', file=log)
parprint('-------------------------------------', file=log)
for n, e in enumerate(hnu):
if e.imag != 0:
c = 'i'
e = e.imag
else:
c = ' '
e = e.real
parprint('%3d %6.1f%s %7.1f%s %9.3g' %
(n, 1000 * e, c, s * e, c, intensities[n]),
file=log)
parprint('-------------------------------------', file=log)
parprint('Zero-point energy: %.3f eV' % self.get_zero_point_energy(),
file=log)
def __del__(self):
self.timer.write(self.txt)
loa.center()
fgl = [False, True]
#fgl = [True, False]
txt='-'
txt='/dev/null'
E = {}
niter = {}
for fg in fgl:
if fg:
tstr = 'Exx on fine grid'
else:
tstr = 'Exx on coarse grid'
timer.start(tstr)
calc = GPAW(h=0.3,
eigensolver='rmm-diis',
xc='PBE',
nbands=4,
convergence={'eigenstates': 1e-4},
charge=-1)
loa.set_calculator(calc)
E[fg] = loa.get_potential_energy()
calc.set(xc=HybridXC('PBE0', finegrid=fg))
E[fg] = loa.get_potential_energy()
niter[fg] = calc.get_number_of_iterations()
timer.stop(tstr)
timer.write(sys.stdout)
class ResonantRaman(Vibrations):
"""Class for calculating vibrational modes and
resonant Raman intensities using finite difference.
atoms:
Atoms object
Excitations:
Class to calculate the excitations. The class object is
initialized as::
Excitations(atoms.get_calculator())
or by reading form a file as::
Excitations('filename', **exkwargs)
The file is written by calling the method
Excitations.write('filename').
Excitations should work like a list of ex obejects, where:
ex.get_dipole_me(form='v'):
gives the dipole matrix element in |e| * Angstrom
ex.energy:
is the transition energy in Hartrees
"""
def __init__(self, atoms, Excitations,
indices=None,
gsname='rraman', # name for ground state calculations
exname=None, # name for excited state calculations
delta=0.01,
nfree=2,
directions=None,
approximation='Profeta',
observation={'geometry': '-Z(XX)Z'},
exkwargs={}, # kwargs to be passed to Excitations
exext='.ex.gz', # extension for Excitation names
txt='-',
verbose=False,):
assert(nfree == 2)
Vibrations.__init__(self, atoms, indices, gsname, delta, nfree)
self.name = gsname + '-d%.3f' % delta
if exname is None:
exname = gsname
self.exname = exname + '-d%.3f' % delta
self.exext = exext
if directions is None:
self.directions = np.array([0, 1, 2])
else:
self.directions = np.array(directions)
self.approximation = approximation
self.observation = observation
self.exobj = Excitations
self.exkwargs = exkwargs
self.timer = Timer()
self.txt = convert_string_to_fd(txt)
self.verbose = verbose
@staticmethod
def m2(z):
return (z * z.conj()).real
def log(self, message, pre='# ', end='\n'):
if self.verbose:
self.txt.write(pre + message + end)
self.txt.flush()
def calculate(self, filename, fd):
"""Call ground and excited state calculation"""
self.timer.start('Ground state')
forces = self.atoms.get_forces()
if rank == 0:
pickle.dump(forces, fd, protocol=2)
fd.close()
self.timer.stop('Ground state')
self.timer.start('Excitations')
basename, _ = os.path.splitext(filename)
excitations = self.exobj(
self.atoms.get_calculator(), **self.exkwargs)
excitations.write(basename + self.exext)
self.timer.stop('Excitations')
def read_excitations(self):
self.timer.start('read excitations')
self.timer.start('really read')
self.log('reading ' + self.exname + '.eq' + self.exext)
ex0_object = self.exobj(self.exname + '.eq' + self.exext,
**self.exkwargs)
self.timer.stop('really read')
self.timer.start('index')
matching = frozenset(ex0_object)
self.timer.stop('index')
def append(lst, exname, matching):
self.timer.start('really read')
self.log('reading ' + exname, end=' ')
exo = self.exobj(exname, **self.exkwargs)
lst.append(exo)
self.timer.stop('really read')
self.timer.start('index')
matching = matching.intersection(exo)
self.log('len={0}, matching={1}'.format(len(exo),
len(matching)), pre='')
self.timer.stop('index')
return matching
exm_object_list = []
exp_object_list = []
for a in self.indices:
for i in 'xyz':
name = '%s.%d%s' % (self.exname, a, i)
matching = append(exm_object_list,
name + '-' + self.exext, matching)
matching = append(exp_object_list,
name + '+' + self.exext, matching)
self.ndof = 3 * len(self.indices)
self.nex = len(matching)
self.timer.stop('read excitations')
self.timer.start('select')
def select(exl, matching):
mlst = [ex for ex in exl if ex in matching]
assert(len(mlst) == len(matching))
return mlst
ex0 = select(ex0_object, matching)
exm = []
exp = []
r = 0
for a in self.indices:
for i in 'xyz':
exm.append(select(exm_object_list[r], matching))
exp.append(select(exp_object_list[r], matching))
r += 1
self.timer.stop('select')
self.timer.start('me and energy')
eu = units.Hartree
self.ex0E_p = np.array([ex.energy * eu for ex in ex0])
self.ex0m_pc = np.array(
[ex.get_dipole_me(form='v') for ex in ex0])
exmE_rp = []
expE_rp = []
exF_rp = []
exmm_rpc = []
expm_rpc = []
r = 0
for a in self.indices:
for i in 'xyz':
exmE_rp.append([em.energy for em in exm[r]])
expE_rp.append([ep.energy for ep in exp[r]])
exF_rp.append(
[(ep.energy - em.energy)
for ep, em in zip(exp[r], exm[r])])
exmm_rpc.append(
[ex.get_dipole_me(form='v') for ex in exm[r]])
expm_rpc.append(
[ex.get_dipole_me(form='v') for ex in exp[r]])
r += 1
self.exmE_rp = np.array(exmE_rp) * eu
self.expE_rp = np.array(expE_rp) * eu
self.exF_rp = np.array(exF_rp) * eu / 2 / self.delta
self.exmm_rpc = np.array(exmm_rpc)
self.expm_rpc = np.array(expm_rpc)
self.timer.stop('me and energy')
def read(self, method='standard', direction='central'):
"""Read data from a pre-performed calculation."""
if not hasattr(self, 'modes'):
self.timer.start('read vibrations')
Vibrations.read(self, method, direction)
# we now have:
# self.H : Hessian matrix
# self.im : 1./sqrt(masses)
# self.modes : Eigenmodes of the mass weighted H
self.om_r = self.hnu.real # energies in eV
self.timer.stop('read vibrations')
if not hasattr(self, 'ex0E_p'):
self.read_excitations()
def get_Huang_Rhys_factors(self, forces_r):
"""Evaluate Huang-Rhys factors derived from forces."""
self.timer.start('Huang-Rhys')
assert(len(forces_r.flat) == self.ndof)
# solve the matrix equation for the equilibrium displacements
# XXX why are the forces mass weighted ???
X_r = np.linalg.solve(self.im[:, None] * self.H * self.im,
forces_r.flat * self.im)
d_r = np.dot(self.modes, X_r)
# Huang-Rhys factors S
s = 1.e-20 / units.kg / units.C / units._hbar**2 # SI units
self.timer.stop('Huang-Rhys')
return s * d_r**2 * self.om_r / 2.
def get_matrix_element_AlbrechtA(self, omega, gamma=0.1, ml=range(16)):
"""Evaluate Albrecht A term.
Unit: |e|^2Angstrom^2/eV
"""
self.read()
self.timer.start('AlbrechtA')
if not hasattr(self, 'fco'):
self.fco = FranckCondonOverlap()
# excited state forces
F_pr = self.exF_rp.T
m_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
for p, energy in enumerate(self.ex0E_p):
S_r = self.get_Huang_Rhys_factors(F_pr[p])
me_cc = np.outer(self.ex0m_pc[p], self.ex0m_pc[p].conj())
for m in ml:
self.timer.start('0mm1')
fco_r = self.fco.direct0mm1(m, S_r)
self.timer.stop('0mm1')
self.timer.start('einsum')
m_rcc += np.einsum('a,bc->abc',
fco_r / (energy + m * self.om_r - omega -
1j * gamma),
me_cc)
m_rcc += np.einsum('a,bc->abc',
fco_r / (energy + (m - 1) * self.om_r +
omega + 1j * gamma),
me_cc)
self.timer.stop('einsum')
self.timer.stop('AlbrechtA')
return m_rcc
def get_matrix_element_AlbrechtBC(self, omega, gamma=0.1, ml=[1],
term='BC'):
"""Evaluate Albrecht B and/or C term(s)."""
self.read()
self.timer.start('AlbrechtBC')
if not hasattr(self, 'fco'):
self.fco = FranckCondonOverlap()
# excited state forces
F_pr = self.exF_rp.T
m_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
for p, energy in enumerate(self.ex0E_p):
S_r = self.get_Huang_Rhys_factors(F_pr[p])
for m in ml:
self.timer.start('Franck-Condon overlaps')
fc1mm1_r = self.fco.direct(1, m, S_r)
fc0mm02_r = self.fco.direct(0, m, S_r)
fc0mm02_r += np.sqrt(2) * self.fco.direct0mm2(m, S_r)
# XXXXX
fc1mm1_r[-1] = 1
fc0mm02_r[-1] = 1
print(m, fc1mm1_r[-1], fc0mm02_r[-1])
self.timer.stop('Franck-Condon overlaps')
self.timer.start('me dervivatives')
dm_rc = []
r = 0
for a in self.indices:
for i in 'xyz':
dm_rc.append(
(self.expm_rpc[r, p] - self.exmm_rpc[r, p]) *
self.im[r])
print('pm=', self.expm_rpc[r, p], self.exmm_rpc[r, p])
r += 1
dm_rc = np.array(dm_rc) / (2 * self.delta)
self.timer.stop('me dervivatives')
self.timer.start('map to modes')
# print('dm_rc[2], dm_rc[5]', dm_rc[2], dm_rc[5])
print('dm_rc=', dm_rc)
dm_rc = np.dot(dm_rc.T, self.modes.T).T
print('dm_rc[-1][2]', dm_rc[-1][2])
self.timer.stop('map to modes')
self.timer.start('multiply')
# me_cc = np.outer(self.ex0m_pc[p], self.ex0m_pc[p].conj())
for r in range(self.ndof):
if 'B' in term:
# XXXX
denom = (1. /
(energy + m * 0 * self.om_r[r] -
omega - 1j * gamma))
# ok print('denom=', denom)
m_rcc[r] += (np.outer(dm_rc[r],
self.ex0m_pc[p].conj()) *
fc1mm1_r[r] * denom)
if r == 5:
print('m_rcc[r]=', m_rcc[r][2, 2])
m_rcc[r] += (np.outer(self.ex0m_pc[p],
dm_rc[r].conj()) *
fc0mm02_r[r] * denom)
if 'C' in term:
denom = (1. /
(energy + (m - 1) * self.om_r[r] +
omega + 1j * gamma))
m_rcc[r] += (np.outer(self.ex0m_pc[p],
dm_rc[r].conj()) *
fc1mm1_r[r] * denom)
m_rcc[r] += (np.outer(dm_rc[r],
self.ex0m_pc[p].conj()) *
fc0mm02_r[r] * denom)
self.timer.stop('multiply')
print('m_rcc[-1]=', m_rcc[-1][2, 2])
self.timer.start('pre_r')
with np.errstate(divide='ignore'):
pre_r = np.where(self.om_r > 0,
np.sqrt(units._hbar**2 / 2. / self.om_r), 0)
# print('BC: pre_r=', pre_r)
for r, p in enumerate(pre_r):
m_rcc[r] *= p
self.timer.stop('pre_r')
self.timer.stop('AlbrechtBC')
return m_rcc
def get_matrix_element_Profeta(self, omega, gamma=0.1,
energy_derivative=False):
"""Evaluate Albrecht B+C term in Profeta and Mauri approximation"""
self.read()
self.timer.start('amplitudes')
self.timer.start('init')
V_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
pre = 1. / (2 * self.delta)
self.timer.stop('init')
def kappa(me_pc, e_p, omega, gamma, form='v'):
"""Kappa tensor after Profeta and Mauri
PRB 63 (2001) 245415"""
me_ccp = np.empty((3, 3, len(e_p)), dtype=complex)
for p, me_c in enumerate(me_pc):
me_ccp[:, :, p] = np.outer(me_pc[p], me_pc[p].conj())
# print('kappa: me_ccp=', me_ccp[2,2,0])
# ok print('kappa: den=', 1./(e_p - omega - 1j * gamma))
kappa_ccp = (me_ccp / (e_p - omega - 1j * gamma) +
me_ccp.conj() / (e_p + omega + 1j * gamma))
return kappa_ccp.sum(2)
self.timer.start('kappa')
r = 0
for a in self.indices:
for i in 'xyz':
if not energy_derivative < 0:
V_rcc[r] = pre * self.im[r] * (
kappa(self.expm_rpc[r], self.ex0E_p, omega, gamma) -
kappa(self.exmm_rpc[r], self.ex0E_p, omega, gamma))
if energy_derivative:
V_rcc[r] += pre * self.im[r] * (
kappa(self.ex0m_pc, self.expE_rp[r], omega, gamma) -
kappa(self.ex0m_pc, self.exmE_rp[r], omega, gamma))
r += 1
self.timer.stop('kappa')
# print('V_rcc[2], V_rcc[5]=', V_rcc[2,2,2], V_rcc[5,2,2])
self.timer.stop('amplitudes')
# map to modes
self.timer.start('pre_r')
with np.errstate(divide='ignore'):
pre_r = np.where(self.om_r > 0,
np.sqrt(units._hbar**2 / 2. / self.om_r), 0)
V_rcc = np.dot(V_rcc.T, self.modes.T).T
# looks ok print('self.modes.T[-1]',self.modes.T)
# looks ok print('V_rcc[-1]=', V_rcc[-1][2,2])
# ok print('Profeta: pre_r=', pre_r)
for r, p in enumerate(pre_r):
V_rcc[r] *= p
self.timer.stop('pre_r')
return V_rcc
def get_matrix_element(self, omega, gamma):
self.read()
V_rcc = np.zeros((self.ndof, 3, 3), dtype=complex)
if self.approximation.lower() == 'profeta':
V_rcc += self.get_matrix_element_Profeta(omega, gamma)
elif self.approximation.lower() == 'placzek':
V_rcc += self.get_matrix_element_Profeta(omega, gamma, True)
elif self.approximation.lower() == 'p-p':
V_rcc += self.get_matrix_element_Profeta(omega, gamma, -1)
elif self.approximation.lower() == 'albrecht a':
V_rcc += self.get_matrix_element_AlbrechtA(omega, gamma)
elif self.approximation.lower() == 'albrecht b':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma, term='B')
elif self.approximation.lower() == 'albrecht c':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma, term='C')
elif self.approximation.lower() == 'albrecht bc':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma)
elif self.approximation.lower() == 'albrecht':
raise NotImplementedError('not working')
V_rcc += self.get_matrix_element_AlbrechtA(omega, gamma)
V_rcc += self.get_matrix_element_AlbrechtBC(omega, gamma)
elif self.approximation.lower() == 'albrecht+profeta':
V_rcc += self.get_matrix_element_AlbrechtA(omega, gamma)
V_rcc += self.get_matrix_element_Profeta(omega, gamma)
else:
raise NotImplementedError(
'Approximation {0} not implemented. '.format(
self.approximation) +
'Please use "Profeta", "Albrecht A/B/C/BC", ' +
'or "Albrecht".')
return V_rcc
def get_intensities(self, omega, gamma=0.1):
m2 = ResonantRaman.m2
alpha_rcc = self.get_matrix_element(omega, gamma)
if not self.observation: # XXXX remove
"""Simple sum, maybe too simple"""
return m2(alpha_rcc).sum(axis=1).sum(axis=1)
# XXX enable when appropraiate
# if self.observation['orientation'].lower() != 'random':
# raise NotImplementedError('not yet')
# random orientation of the molecular frame
# Woodward & Long,
# Guthmuller, J. J. Chem. Phys. 2016, 144 (6), 64106
m2 = ResonantRaman.m2
alpha2_r = m2(alpha_rcc[:, 0, 0] + alpha_rcc[:, 1, 1] +
alpha_rcc[:, 2, 2]) / 9.
delta2_r = 3 / 4. * (
m2(alpha_rcc[:, 0, 1] - alpha_rcc[:, 1, 0]) +
m2(alpha_rcc[:, 0, 2] - alpha_rcc[:, 2, 0]) +
m2(alpha_rcc[:, 1, 2] - alpha_rcc[:, 2, 1]))
gamma2_r = (3 / 4. * (m2(alpha_rcc[:, 0, 1] + alpha_rcc[:, 1, 0]) +
m2(alpha_rcc[:, 0, 2] + alpha_rcc[:, 2, 0]) +
m2(alpha_rcc[:, 1, 2] + alpha_rcc[:, 2, 1])) +
(m2(alpha_rcc[:, 0, 0] - alpha_rcc[:, 1, 1]) +
m2(alpha_rcc[:, 0, 0] - alpha_rcc[:, 2, 2]) +
m2(alpha_rcc[:, 1, 1] - alpha_rcc[:, 2, 2])) / 2)
if self.observation['geometry'] == '-Z(XX)Z': # Porto's notation
return (45 * alpha2_r + 5 * delta2_r + 4 * gamma2_r) / 45.
elif self.observation['geometry'] == '-Z(XY)Z': # Porto's notation
return gamma2_r / 15.
elif self.observation['scattered'] == 'Z':
# scattered light in direction of incoming light
return (45 * alpha2_r + 5 * delta2_r + 7 * gamma2_r) / 45.
elif self.observation['scattered'] == 'parallel':
# scattered light perendicular and
# polarization in plane
return 6 * gamma2_r / 45.
elif self.observation['scattered'] == 'perpendicular':
# scattered light perendicular and
# polarization out of plane
return (45 * alpha2_r + 5 * delta2_r + 7 * gamma2_r) / 45.
else:
raise NotImplementedError
def get_cross_sections(self, omega, gamma=0.1):
I_r = self.get_intensities(omega, gamma)
pre = 1. / 16 / np.pi**2 / units.eps0**2 / units.c**4
# frequency of scattered light
omS_r = omega - self.hnu
return pre * omega * omS_r**3 * I_r
def get_spectrum(self, omega, gamma=0.1,
start=200.0, end=4000.0, npts=None, width=4.0,
type='Gaussian', method='standard', direction='central',
intensity_unit='????', normalize=False):
"""Get resonant Raman spectrum.
The method returns wavenumbers in cm^-1 with corresponding
Raman cross section.
Start and end point, and width of the Gaussian/Lorentzian should
be given in cm^-1.
"""
self.type = type.lower()
assert self.type in ['gaussian', 'lorentzian']
if not npts:
npts = int((end - start) / width * 10 + 1)
frequencies = self.get_frequencies(method, direction).real
intensities = self.get_cross_sections(omega, gamma)
prefactor = 1
if type == 'lorentzian':
intensities = intensities * width * np.pi / 2.
if normalize:
prefactor = 2. / width / np.pi
else:
sigma = width / 2. / np.sqrt(2. * np.log(2.))
if normalize:
prefactor = 1. / sigma / np.sqrt(2 * np.pi)
# Make array with spectrum data
spectrum = np.empty(npts)
energies = np.linspace(start, end, npts)
for i, energy in enumerate(energies):
energies[i] = energy
if type == 'lorentzian':
spectrum[i] = (intensities * 0.5 * width / np.pi /
((frequencies - energy)**2 +
0.25 * width**2)).sum()
else:
spectrum[i] = (intensities *
np.exp(-(frequencies - energy)**2 /
2. / sigma**2)).sum()
return [energies, prefactor * spectrum]
def write_spectrum(self, omega, gamma,
out='resonant-raman-spectra.dat',
start=200, end=4000,
npts=None, width=10,
type='Gaussian', method='standard',
direction='central'):
"""Write out spectrum to file.
First column is the wavenumber in cm^-1, the second column the
absolute infrared intensities, and
the third column the absorbance scaled so that data runs
from 1 to 0. Start and end
point, and width of the Gaussian/Lorentzian should be given
in cm^-1."""
energies, spectrum = self.get_spectrum(omega, gamma,
start, end, npts, width,
type, method, direction)
# Write out spectrum in file. First column is absolute intensities.
outdata = np.empty([len(energies), 3])
outdata.T[0] = energies
outdata.T[1] = spectrum
fd = open(out, 'w')
fd.write('# Resonant Raman spectrum\n')
fd.write('# omega={0:g} eV, gamma={1:g} eV\n'.format(omega, gamma))
fd.write('# %s folded, width=%g cm^-1\n' % (type.title(), width))
fd.write('# [cm^-1] [a.u.]\n')
for row in outdata:
fd.write('%.3f %15.5g\n' %
(row[0], row[1]))
fd.close()
def summary(self, omega, gamma=0.1,
method='standard', direction='central',
log=sys.stdout):
"""Print summary for given omega [eV]"""
hnu = self.get_energies(method, direction)
s = 0.01 * units._e / units._c / units._hplanck
intensities = self.get_intensities(omega, gamma)
if isinstance(log, basestring):
log = paropen(log, 'a')
parprint('-------------------------------------', file=log)
parprint(' excitation at ' + str(omega) + ' eV', file=log)
parprint(' gamma ' + str(gamma) + ' eV', file=log)
parprint(' approximation:', self.approximation, file=log)
parprint(' observation:', self.observation, '\n', file=log)
parprint(' Mode Frequency Intensity', file=log)
parprint(' # meV cm^-1 [e^4A^4/eV^2]', file=log)
parprint('-------------------------------------', file=log)
for n, e in enumerate(hnu):
if e.imag != 0:
c = 'i'
e = e.imag
else:
c = ' '
e = e.real
parprint('%3d %6.1f%s %7.1f%s %9.3g' %
(n, 1000 * e, c, s * e, c, intensities[n]),
file=log)
parprint('-------------------------------------', file=log)
parprint('Zero-point energy: %.3f eV' % self.get_zero_point_energy(),
file=log)
def __del__(self):
self.timer.write(self.txt)
def get_rpa(self):
"""Calculate RPA and Hartree-fock part of the A+-B matrices."""
# shorthands
kss = self.fullkss
finegrid = self.finegrid
# calculate omega matrix
nij = len(kss)
print('RPAhyb', nij, 'transitions', file=self.txt)
AmB = np.zeros((nij, nij))
ApB = self.ApB
# storage place for Coulomb integrals
integrals = {}
for ij in range(nij):
print('RPAhyb kss[' + '%d' % ij + ']=', kss[ij], file=self.txt)
timer = Timer()
timer.start('init')
timer2 = Timer()
# smooth density including compensation charges
timer2.start('with_compensation_charges 0')
rhot_p = kss[ij].with_compensation_charges(finegrid is not 0)
timer2.stop()
# integrate with 1/|r_1-r_2|
timer2.start('poisson')
phit_p = np.zeros(rhot_p.shape, rhot_p.dtype)
self.poisson.solve(phit_p, rhot_p, charge=None)
timer2.stop()
timer.stop()
t0 = timer.get_time('init')
timer.start(ij)
if finegrid == 1:
rhot = kss[ij].with_compensation_charges()
phit = self.gd.zeros()
self.restrict(phit_p, phit)
else:
phit = phit_p
rhot = rhot_p
for kq in range(ij, nij):
if kq != ij:
# smooth density including compensation charges
timer2.start('kq with_compensation_charges')
rhot = kss[kq].with_compensation_charges(finegrid is 2)
timer2.stop()
pre = self.weight_Kijkq(ij, kq)
timer2.start('integrate')
I = self.Coulomb_integral_kss(kss[ij], kss[kq], phit, rhot)
if kss[ij].spin == kss[kq].spin:
name = self.Coulomb_integral_name(kss[ij].i, kss[ij].j,
kss[kq].i, kss[kq].j,
kss[ij].spin)
integrals[name] = I
ApB[ij, kq] = pre * I
timer2.stop()
if ij == kq:
epsij = kss[ij].get_energy() / kss[ij].get_weight()
AmB[ij, kq] += epsij
ApB[ij, kq] += epsij
timer.stop()
# timer2.write()
if ij < (nij - 1):
print('RPAhyb estimated time left',
self.time_left(timer, t0, ij, nij),
file=self.txt)
# add HF parts and apply symmetry
if hasattr(self.xc, 'hybrid'):
weight = self.xc.hybrid
else:
weight = 0.0
for ij in range(nij):
print('HF kss[' + '%d' % ij + ']', file=self.txt)
timer = Timer()
timer.start('init')
timer.stop()
t0 = timer.get_time('init')
timer.start(ij)
i = kss[ij].i
j = kss[ij].j
s = kss[ij].spin
for kq in range(ij, nij):
if kss[ij].pspin == kss[kq].pspin:
k = kss[kq].i
q = kss[kq].j
ikjq = self.Coulomb_integral_ijkq(i, k, j, q, s, integrals)
iqkj = self.Coulomb_integral_ijkq(i, q, k, j, s, integrals)
ApB[ij, kq] -= weight * (ikjq + iqkj)
AmB[ij, kq] -= weight * (ikjq - iqkj)
ApB[kq, ij] = ApB[ij, kq]
AmB[kq, ij] = AmB[ij, kq]
timer.stop()
if ij < (nij - 1):
print('HF estimated time left',
self.time_left(timer, t0, ij, nij),
file=self.txt)
return AmB
def start(self, name):
Timer.start(self, name)
if name in self.compatible:
self.hpm_start(name)
def start(self, name):
Timer.start(self, name)
abstime = time.time()
t = self.timers[tuple(self.running)] + abstime
self.txt.write('T%s >> %15.8f %s (%7.5fs) started\n'
% (self.srank, abstime, name, t))
class RPACorrelation:
def __init__(self, calc, xc='RPA', filename=None,
skip_gamma=False, qsym=True, nlambda=None,
nfrequencies=16, frequency_max=800.0, frequency_scale=2.0,
frequencies=None, weights=None, truncation=None,
world=mpi.world, nblocks=1, txt=sys.stdout):
"""Creates the RPACorrelation object
calc: str or calculator object
The string should refer to the .gpw file contaning KS orbitals
xc: str
Exchange-correlation kernel. This is only different from RPA when
this object is constructed from a different module - e.g. fxc.py
filename: str
txt output
skip_gamme: bool
If True, skip q = [0,0,0] from the calculation
qsym: bool
Use symmetry to reduce q-points
nlambda: int
Number of lambda points. Only used for numerical coupling
constant integration involved when called from fxc.py
nfrequencies: int
Number of frequency points used in the Gauss-Legendre integration
frequency_max: float
Largest frequency point in Gauss-Legendre integration
frequency_scale: float
Determines density of frequency points at low frequencies. A slight
increase to e.g. 2.5 or 3.0 improves convergence wth respect to
frequency points for metals
frequencies: list
List of frequancies for user-specified frequency integration
weights: list
list of weights (integration measure) for a user specified
frequency grid. Must be specified and have the same length as
frequencies if frequencies is not None
truncation: str
Coulomb truncation scheme. Can be either wigner-seitz,
2D, 1D, or 0D
world: communicator
nblocks: int
Number of parallelization blocks. Frequency parallelization
can be specified by setting nblocks=nfrequencies and is useful
for memory consuming calculations
txt: str
txt file for saving and loading contributions to the correlation
energy from different q-points
"""
if isinstance(calc, str):
calc = GPAW(calc, txt=None, communicator=mpi.serial_comm)
self.calc = calc
if world.rank != 0:
txt = devnull
elif isinstance(txt, str):
txt = open(txt, 'w', 1)
self.fd = txt
self.timer = Timer()
if frequencies is None:
frequencies, weights = get_gauss_legendre_points(nfrequencies,
frequency_max,
frequency_scale)
user_spec = False
else:
assert weights is not None
user_spec = True
self.omega_w = frequencies / Hartree
self.weight_w = weights / Hartree
if nblocks > 1:
assert len(self.omega_w) % nblocks == 0
self.nblocks = nblocks
self.world = world
self.truncation = truncation
self.skip_gamma = skip_gamma
self.ibzq_qc = None
self.weight_q = None
self.initialize_q_points(qsym)
# Energies for all q-vetors and cutoff energies:
self.energy_qi = []
self.filename = filename
self.print_initialization(xc, frequency_scale, nlambda, user_spec)
def initialize_q_points(self, qsym):
kd = self.calc.wfs.kd
self.bzq_qc = kd.get_bz_q_points(first=True)
if not qsym:
self.ibzq_qc = self.bzq_qc
self.weight_q = np.ones(len(self.bzq_qc)) / len(self.bzq_qc)
else:
U_scc = kd.symmetry.op_scc
self.ibzq_qc = kd.get_ibz_q_points(self.bzq_qc, U_scc)[0]
self.weight_q = kd.q_weights
def read(self):
lines = open(self.filename).readlines()[1:]
n = 0
self.energy_qi = []
nq = len(lines) // len(self.ecut_i)
for q_c in self.ibzq_qc[:nq]:
self.energy_qi.append([])
for ecut in self.ecut_i:
q1, q2, q3, ec, energy = [float(x)
for x in lines[n].split()]
self.energy_qi[-1].append(energy / Hartree)
n += 1
if (abs(q_c - (q1, q2, q3)).max() > 1e-4 or
abs(int(ecut * Hartree) - ec) > 0):
self.energy_qi = []
return
print('Read %d q-points from file: %s' % (nq, self.filename),
file=self.fd)
print(file=self.fd)
def write(self):
if self.world.rank == 0 and self.filename:
fd = open(self.filename, 'w')
print('#%9s %10s %10s %8s %12s' %
('q1', 'q2', 'q3', 'E_cut', 'E_c(q)'), file=fd)
for energy_i, q_c in zip(self.energy_qi, self.ibzq_qc):
for energy, ecut in zip(energy_i, self.ecut_i):
print('%10.4f %10.4f %10.4f %8d %r' %
(tuple(q_c) + (ecut * Hartree, energy * Hartree)),
file=fd)
def calculate(self, ecut, nbands=None, spin=False):
"""Calculate RPA correlation energy for one or several cutoffs.
ecut: float or list of floats
Plane-wave cutoff(s).
nbands: int
Number of bands (defaults to number of plane-waves).
spin: bool
Separate spin in response function.
(Only needed for beyond RPA methods that inherit this function).
"""
p = functools.partial(print, file=self.fd)
if isinstance(ecut, (float, int)):
ecut = ecut * (1 + 0.5 * np.arange(6))**(-2 / 3)
self.ecut_i = np.asarray(np.sort(ecut)) / Hartree
ecutmax = max(self.ecut_i)
if nbands is None:
p('Response function bands : Equal to number of plane waves')
else:
p('Response function bands : %s' % nbands)
p('Plane wave cutoffs (eV) :', end='')
for e in self.ecut_i:
p(' {0:.3f}'.format(e * Hartree), end='')
p()
if self.truncation is not None:
p('Using %s Coulomb truncation' % self.truncation)
p()
if self.filename and os.path.isfile(self.filename):
self.read()
self.world.barrier()
chi0 = Chi0(self.calc, 1j * Hartree * self.omega_w, eta=0.0,
intraband=False, hilbert=False,
txt='chi0.txt', timer=self.timer, world=self.world,
nblocks=self.nblocks)
self.blockcomm = chi0.blockcomm
wfs = self.calc.wfs
if self.truncation == 'wigner-seitz':
self.wstc = WignerSeitzTruncatedCoulomb(wfs.gd.cell_cv,
wfs.kd.N_c, self.fd)
else:
self.wstc = None
nq = len(self.energy_qi)
nw = len(self.omega_w)
nGmax = max(count_reciprocal_vectors(ecutmax, wfs.gd, q_c)
for q_c in self.ibzq_qc[nq:])
mynGmax = (nGmax + self.nblocks - 1) // self.nblocks
nx = (1 + spin) * nw * mynGmax * nGmax
A1_x = np.empty(nx, complex)
if self.nblocks > 1:
A2_x = np.empty(nx, complex)
else:
A2_x = None
self.timer.start('RPA')
for q_c in self.ibzq_qc[nq:]:
if np.allclose(q_c, 0.0) and self.skip_gamma:
self.energy_qi.append(len(self.ecut_i) * [0.0])
self.write()
p('Not calculating E_c(q) at Gamma')
p()
continue
thisqd = KPointDescriptor([q_c])
pd = PWDescriptor(ecutmax, wfs.gd, complex, thisqd)
nG = pd.ngmax
mynG = (nG + self.nblocks - 1) // self.nblocks
chi0.Ga = self.blockcomm.rank * mynG
chi0.Gb = min(chi0.Ga + mynG, nG)
shape = (1 + spin, nw, chi0.Gb - chi0.Ga, nG)
chi0_swGG = A1_x[:np.prod(shape)].reshape(shape)
chi0_swGG[:] = 0.0
if np.allclose(q_c, 0.0):
chi0_swxvG = np.zeros((1 + spin, nw, 2, 3, nG), complex)
chi0_swvv = np.zeros((1 + spin, nw, 3, 3), complex)
else:
chi0_swxvG = None
chi0_swvv = None
# First not completely filled band:
m1 = chi0.nocc1
p('# %s - %s' % (len(self.energy_qi), ctime().split()[-2]))
p('q = [%1.3f %1.3f %1.3f]' % tuple(q_c))
energy_i = []
for ecut in self.ecut_i:
if ecut == ecutmax:
# Nothing to cut away:
cut_G = None
m2 = nbands or nG
else:
cut_G = np.arange(nG)[pd.G2_qG[0] <= 2 * ecut]
m2 = len(cut_G)
p('E_cut = %d eV / Bands = %d:' % (ecut * Hartree, m2))
self.fd.flush()
energy = self.calculate_q(chi0, pd,
chi0_swGG, chi0_swxvG, chi0_swvv,
m1, m2, cut_G, A2_x)
energy_i.append(energy)
m1 = m2
a = 1 / chi0.kncomm.size
if ecut < ecutmax and a != 1.0:
# Chi0 will be summed again over chicomm, so we divide
# by its size:
chi0_swGG *= a
if chi0_swxvG is not None:
chi0_swxvG *= a
chi0_swvv *= a
self.energy_qi.append(energy_i)
self.write()
p()
e_i = np.dot(self.weight_q, np.array(self.energy_qi))
p('==========================================================')
p()
p('Total correlation energy:')
for e_cut, e in zip(self.ecut_i, e_i):
p('%6.0f: %6.4f eV' % (e_cut * Hartree, e * Hartree))
p()
self.energy_qi = [] # important if another calculation is performed
if len(e_i) > 1:
self.extrapolate(e_i)
p('Calculation completed at: ', ctime())
p()
self.timer.stop('RPA')
self.timer.write(self.fd)
self.fd.flush()
return e_i * Hartree
@timer('chi0(q)')
def calculate_q(self, chi0, pd, chi0_swGG, chi0_swxvG, chi0_swvv,
m1, m2, cut_G, A2_x):
chi0_wGG = chi0_swGG[0]
if chi0_swxvG is not None:
chi0_wxvG = chi0_swxvG[0]
chi0_wvv = chi0_swvv[0]
else:
chi0_wxvG = None
chi0_wvv = None
chi0._calculate(pd, chi0_wGG, chi0_wxvG, chi0_wvv,
m1, m2, [0, 1])
print('E_c(q) = ', end='', file=self.fd)
chi0_wGG = chi0.redistribute(chi0_wGG, A2_x)
if not pd.kd.gamma:
e = self.calculate_energy(pd, chi0_wGG, cut_G)
print('%.3f eV' % (e * Hartree), file=self.fd)
self.fd.flush()
else:
from ase.dft import monkhorst_pack
kd = self.calc.wfs.kd
N = 4
N_c = np.array([N, N, N])
if self.truncation is not None:
N_c[kd.N_c == 1] = 1
q_qc = monkhorst_pack(N_c) / kd.N_c
q_qc *= 1.0e-6
U_scc = kd.symmetry.op_scc
q_qc = kd.get_ibz_q_points(q_qc, U_scc)[0]
weight_q = kd.q_weights
q_qv = 2 * np.pi * np.dot(q_qc, pd.gd.icell_cv)
nw = len(self.omega_w)
mynw = nw // self.nblocks
w1 = self.blockcomm.rank * mynw
w2 = w1 + mynw
a_qw = np.sum(np.dot(chi0_wvv[w1:w2], q_qv.T) * q_qv.T, axis=1).T
a0_qwG = np.dot(q_qv, chi0_wxvG[w1:w2, 0])
a1_qwG = np.dot(q_qv, chi0_wxvG[w1:w2, 1])
e = 0
for iq in range(len(q_qv)):
chi0_wGG[:, 0] = a0_qwG[iq]
chi0_wGG[:, :, 0] = a1_qwG[iq]
chi0_wGG[:, 0, 0] = a_qw[iq]
ev = self.calculate_energy(pd, chi0_wGG, cut_G,
q_v=q_qv[iq])
e += ev * weight_q[iq]
print('%.3f eV' % (e * Hartree), file=self.fd)
self.fd.flush()
return e
@timer('Energy')
def calculate_energy(self, pd, chi0_wGG, cut_G, q_v=None):
"""Evaluate correlation energy from chi0."""
sqrV_G = get_coulomb_kernel(pd, self.calc.wfs.kd.N_c, q_v=q_v,
truncation=self.truncation,
wstc=self.wstc)**0.5
if cut_G is not None:
sqrV_G = sqrV_G[cut_G]
nG = len(sqrV_G)
e_w = []
for chi0_GG in chi0_wGG:
if cut_G is not None:
chi0_GG = chi0_GG.take(cut_G, 0).take(cut_G, 1)
e_GG = np.eye(nG) - chi0_GG * sqrV_G * sqrV_G[:, np.newaxis]
e = np.log(np.linalg.det(e_GG)) + nG - np.trace(e_GG)
e_w.append(e.real)
E_w = np.zeros_like(self.omega_w)
self.blockcomm.all_gather(np.array(e_w), E_w)
energy = np.dot(E_w, self.weight_w) / (2 * np.pi)
self.E_w = E_w
return energy
def extrapolate(self, e_i):
print('Extrapolated energies:', file=self.fd)
ex_i = []
for i in range(len(e_i) - 1):
e1, e2 = e_i[i:i + 2]
x1, x2 = self.ecut_i[i:i + 2]**-1.5
ex = (e1 * x2 - e2 * x1) / (x2 - x1)
ex_i.append(ex)
print(' %4.0f -%4.0f: %5.3f eV' % (self.ecut_i[i] * Hartree,
self.ecut_i[i + 1] * Hartree,
ex * Hartree),
file=self.fd)
print(file=self.fd)
self.fd.flush()
return e_i * Hartree
def print_initialization(self, xc, frequency_scale, nlambda, user_spec):
p = functools.partial(print, file=self.fd)
p('----------------------------------------------------------')
p('Non-self-consistent %s correlation energy' % xc)
p('----------------------------------------------------------')
p('Started at: ', ctime())
p()
p('Atoms :',
self.calc.atoms.get_chemical_formula(mode='hill'))
p('Ground state XC functional :', self.calc.hamiltonian.xc.name)
p('Valence electrons :', self.calc.wfs.setups.nvalence)
p('Number of bands :', self.calc.wfs.bd.nbands)
p('Number of spins :', self.calc.wfs.nspins)
p('Number of k-points :', len(self.calc.wfs.kd.bzk_kc))
p('Number of irreducible k-points :', len(self.calc.wfs.kd.ibzk_kc))
p('Number of q-points :', len(self.bzq_qc))
p('Number of irreducible q-points :', len(self.ibzq_qc))
p()
for q, weight in zip(self.ibzq_qc, self.weight_q):
p(' q: [%1.4f %1.4f %1.4f] - weight: %1.3f' %
(q[0], q[1], q[2], weight))
p()
p('----------------------------------------------------------')
p('----------------------------------------------------------')
p()
if nlambda is None:
p('Analytical coupling constant integration')
else:
p('Numerical coupling constant integration using', nlambda,
'Gauss-Legendre points')
p()
p('Frequencies')
if not user_spec:
p(' Gauss-Legendre integration with %s frequency points' %
len(self.omega_w))
p(' Transformed from [0,oo] to [0,1] using e^[-aw^(1/B)]')
p(' Highest frequency point at %5.1f eV and B=%1.1f' %
(self.omega_w[-1] * Hartree, frequency_scale))
else:
p(' User specified frequency integration with',
len(self.omega_w), 'frequency points')
p()
p('Parallelization')
p(' Total number of CPUs : % s' % self.world.size)
p(' G-vector decomposition : % s' % self.nblocks)
p(' K-point/band decomposition : % s' %
(self.world.size // self.nblocks))
p()
class ResonantRaman(Vibrations):
"""Base Class for resonant Raman intensities using finite differences.
Parameters
----------
overlap : function or False
Function to calculate overlaps between excitation at
equilibrium and at a displaced position. Calculators are
given as first and second argument, respectively.
"""
def __init__(self, atoms, Excitations,
indices=None,
gsname='rraman', # name for ground state calculations
exname=None, # name for excited state calculations
delta=0.01,
nfree=2,
directions=None,
observation={'geometry': '-Z(XX)Z'},
form='v', # form of the dipole operator
exkwargs={}, # kwargs to be passed to Excitations
exext='.ex.gz', # extension for Excitation names
txt='-',
verbose=False,
overlap=False,
minoverlap=0.02,
minrep=0.8,
comm=world,
):
"""
Parameters
----------
atoms: ase Atoms object
Excitations: class
Type of the excitation list object. The class object is
initialized as::
Excitations(atoms.get_calculator())
or by reading form a file as::
Excitations('filename', **exkwargs)
The file is written by calling the method
Excitations.write('filename').
Excitations should work like a list of ex obejects, where:
ex.get_dipole_me(form='v'):
gives the velocity form dipole matrix element in
units |e| * Angstrom
ex.energy:
is the transition energy in Hartrees
indices: list
gsname: string
name for ground state calculations
exname: string
name for excited state calculations
delta: float
Finite difference displacement in Angstrom.
nfree: float
directions:
approximation: string
Level of approximation used.
observation: dict
Polarization settings
form: string
Form of the dipole operator, 'v' for velocity form (default)
and 'r' for length form.
exkwargs: dict
Arguments given to the Excitations objects in reading.
exext: string
Extension for filenames of Excitation lists.
txt:
Output stream
verbose:
Verbosity level of output
overlap: bool or function
Use wavefunction overlaps.
minoverlap: float ord dict
Minimal absolute overlap to consider. Defaults to 0.02 to avoid
numerical garbage.
minrep: float
Minimal represention to consider derivative, defaults to 0.8
"""
assert(nfree == 2)
Vibrations.__init__(self, atoms, indices, gsname, delta, nfree)
self.name = gsname + '-d%.3f' % delta
if exname is None:
exname = gsname
self.exname = exname + '-d%.3f' % delta
self.exext = exext
if directions is None:
self.directions = np.array([0, 1, 2])
else:
self.directions = np.array(directions)
self.observation = observation
self.exobj = Excitations
self.exkwargs = exkwargs
self.dipole_form = form
self.timer = Timer()
self.txt = convert_string_to_fd(txt)
self.verbose = verbose
self.overlap = overlap
if not isinstance(minoverlap, dict):
# assume it's a number
self.minoverlap = {'orbitals': minoverlap,
'excitations': minoverlap}
else:
self.minoverlap = minoverlap
self.minrep = minrep
self.comm = comm
@property
def approximation(self):
return self._approx
@approximation.setter
def approximation(self, value):
self.set_approximation(value)
@staticmethod
def m2(z):
return (z * z.conj()).real
def log(self, message, pre='# ', end='\n'):
if self.verbose:
self.txt.write(pre + message + end)
self.txt.flush()
def run(self):
if self.overlap:
# XXXX stupid way to make a copy
self.atoms.get_potential_energy()
self.eq_calculator = self.atoms.get_calculator()
fname = self.exname + '.eq.gpw'
self.eq_calculator.write(fname, 'all')
self.eq_calculator = self.eq_calculator.__class__(fname)
self.eq_calculator.converge_wave_functions()
Vibrations.run(self)
def calculate(self, atoms, filename, fd):
"""Call ground and excited state calculation"""
assert(atoms == self.atoms) # XXX action required
self.timer.start('Ground state')
forces = self.atoms.get_forces()
if rank == 0:
pickle.dump(forces, fd, protocol=2)
fd.close()
if self.overlap:
self.timer.start('Overlap')
"""Overlap is determined as
ov_ij = int dr displaced*_i(r) eqilibrium_j(r)
"""
ov_nn = self.overlap(self.atoms.get_calculator(),
self.eq_calculator)
if rank == 0:
np.save(filename + '.ov', ov_nn)
self.timer.stop('Overlap')
self.timer.stop('Ground state')
self.timer.start('Excitations')
basename, _ = os.path.splitext(filename)
excitations = self.exobj(
self.atoms.get_calculator(), **self.exkwargs)
excitations.write(basename + self.exext)
self.timer.stop('Excitations')
def init_parallel_read(self):
"""Initialize variables for parallel read"""
rank = self.comm.rank
self.ndof = 3 * len(self.indices)
myn = -(-self.ndof // self.comm.size) # ceil divide
self.slize = s = slice(myn * rank, myn * (rank + 1))
self.myindices = np.repeat(self.indices, 3)[s]
self.myxyz = ('xyz' * len(self.indices))[s]
self.myr = range(self.ndof)[s]
self.mynd = len(self.myr)
def read_excitations(self):
"""Read all finite difference excitations and select matching."""
self.timer.start('read excitations')
self.timer.start('really read')
self.log('reading ' + self.exname + '.eq' + self.exext)
ex0_object = self.exobj(self.exname + '.eq' + self.exext,
**self.exkwargs)
self.timer.stop('really read')
self.timer.start('index')
matching = frozenset(ex0_object)
self.timer.stop('index')
def append(lst, exname, matching):
self.timer.start('really read')
self.log('reading ' + exname, end=' ')
exo = self.exobj(exname, **self.exkwargs)
lst.append(exo)
self.timer.stop('really read')
self.timer.start('index')
matching = matching.intersection(exo)
self.log('len={0}, matching={1}'.format(len(exo),
len(matching)), pre='')
self.timer.stop('index')
return matching
exm_object_list = []
exp_object_list = []
for a, i in zip(self.myindices, self.myxyz):
name = '%s.%d%s' % (self.exname, a, i)
matching = append(exm_object_list,
name + '-' + self.exext, matching)
matching = append(exp_object_list,
name + '+' + self.exext, matching)
self.ndof = 3 * len(self.indices)
self.nex = len(matching)
self.timer.stop('read excitations')
self.timer.start('select')
def select(exl, matching):
mlst = [ex for ex in exl if ex in matching]
assert(len(mlst) == len(matching))
return mlst
ex0 = select(ex0_object, matching)
exm = []
exp = []
r = 0
for a, i in zip(self.myindices, self.myxyz):
exm.append(select(exm_object_list[r], matching))
exp.append(select(exp_object_list[r], matching))
r += 1
self.timer.stop('select')
self.timer.start('me and energy')
eu = u.Hartree
self.ex0E_p = np.array([ex.energy * eu for ex in ex0])
self.ex0m_pc = (np.array(
[ex.get_dipole_me(form=self.dipole_form) for ex in ex0]) *
u.Bohr)
exmE_rp = []
expE_rp = []
exF_rp = []
exmm_rpc = []
expm_rpc = []
r = 0
for a, i in zip(self.myindices, self.myxyz):
exmE_rp.append([em.energy for em in exm[r]])
expE_rp.append([ep.energy for ep in exp[r]])
exF_rp.append(
[(em.energy - ep.energy)
for ep, em in zip(exp[r], exm[r])])
exmm_rpc.append(
[ex.get_dipole_me(form=self.dipole_form)
for ex in exm[r]])
expm_rpc.append(
[ex.get_dipole_me(form=self.dipole_form)
for ex in exp[r]])
r += 1
# indicees: r=coordinate, p=excitation
# energies in eV
self.exmE_rp = np.array(exmE_rp) * eu
self.expE_rp = np.array(expE_rp) * eu
# forces in eV / Angstrom
self.exF_rp = np.array(exF_rp) * eu / 2 / self.delta
# matrix elements in e * Angstrom
self.exmm_rpc = np.array(exmm_rpc) * u.Bohr
self.expm_rpc = np.array(expm_rpc) * u.Bohr
self.timer.stop('me and energy')
def read_excitations_overlap(self):
"""Read all finite difference excitations and wf overlaps.
We assume that the wave function overlaps are determined as
ov_ij = int dr displaced*_i(r) eqilibrium_j(r)
"""
self.timer.start('read excitations')
self.timer.start('read+rotate')
self.log('reading ' + self.exname + '.eq' + self.exext)
ex0 = self.exobj(self.exname + '.eq' + self.exext,
**self.exkwargs)
rep0_p = np.ones((len(ex0)), dtype=float)
def load(name, pm, rep0_p):
self.log('reading ' + name + pm + self.exext)
ex_p = self.exobj(name + pm + self.exext, **self.exkwargs)
self.log('reading ' + name + pm + '.pckl.ov.npy')
ov_nn = np.load(name + pm + '.pckl.ov.npy')
# remove numerical garbage
ov_nn = np.where(np.abs(ov_nn) > self.minoverlap['orbitals'],
ov_nn, 0)
self.timer.start('ex overlap')
ov_pp = ex_p.overlap(ov_nn, ex0)
# remove numerical garbage
ov_pp = np.where(np.abs(ov_pp) > self.minoverlap['excitations'],
ov_pp, 0)
rep0_p *= (ov_pp.real**2 + ov_pp.imag**2).sum(axis=0)
self.timer.stop('ex overlap')
return ex_p, ov_pp
def rotate(ex_p, ov_pp):
e_p = np.array([ex.energy for ex in ex_p])
m_pc = np.array(
[ex.get_dipole_me(form=self.dipole_form) for ex in ex_p])
r_pp = ov_pp.T
return ((r_pp.real**2 + r_pp.imag**2).dot(e_p),
r_pp.dot(m_pc))
exmE_rp = []
expE_rp = []
exF_rp = []
exmm_rpc = []
expm_rpc = []
exdmdr_rpc = []
for a, i in zip(self.myindices, self.myxyz):
name = '%s.%d%s' % (self.exname, a, i)
ex, ov = load(name, '-', rep0_p)
exmE_p, exmm_pc = rotate(ex, ov)
ex, ov = load(name, '+', rep0_p)
expE_p, expm_pc = rotate(ex, ov)
exmE_rp.append(exmE_p)
expE_rp.append(expE_p)
exF_rp.append(exmE_p - expE_p)
exmm_rpc.append(exmm_pc)
expm_rpc.append(expm_pc)
exdmdr_rpc.append(expm_pc - exmm_pc)
self.timer.stop('read+rotate')
self.timer.start('me and energy')
# select only excitations that are sufficiently represented
self.comm.product(rep0_p)
select = np.where(rep0_p > self.minrep)[0]
eu = u.Hartree
self.ex0E_p = np.array([ex.energy * eu for ex in ex0])[select]
self.ex0m_pc = (np.array(
[ex.get_dipole_me(form=self.dipole_form)
for ex in ex0])[select] * u.Bohr)
if len(self.myr):
# indicees: r=coordinate, p=excitation
# energies in eV
self.exmE_rp = np.array(exmE_rp)[:,select] * eu
##print(len(select), np.array(exmE_rp).shape, self.exmE_rp.shape)
self.expE_rp = np.array(expE_rp)[:,select] * eu
# forces in eV / Angstrom
self.exF_rp = np.array(exF_rp)[:,select] * eu / 2 / self.delta
# matrix elements in e * Angstrom
self.exmm_rpc = np.array(exmm_rpc)[:,select,:] * u.Bohr
self.expm_rpc = np.array(expm_rpc)[:,select,:] * u.Bohr
# matrix element derivatives in e
self.exdmdr_rpc = (np.array(exdmdr_rpc)[:,select,:] *
u.Bohr / 2 / self.delta)
else:
# did not read
self.exmE_rp = self.expE_rp = self.exF_rp = np.empty((0))
self.exmm_rpc = self.expm_rpc = self.exdmdr_rpc = np.empty((0))
self.timer.stop('me and energy')
self.timer.stop('read excitations')
def read(self, method='standard', direction='central'):
"""Read data from a pre-performed calculation."""
self.timer.start('read')
self.timer.start('vibrations')
Vibrations.read(self, method, direction)
# we now have:
# self.H : Hessian matrix
# self.im : 1./sqrt(masses)
# self.modes : Eigenmodes of the mass weighted Hessian
self.om_Q = self.hnu.real # energies in eV
self.om_v = self.om_Q
# pre-factors for one vibrational excitation
with np.errstate(divide='ignore'):
self.vib01_Q = np.where(self.om_Q > 0,
1. / np.sqrt(2 * self.om_Q), 0)
# -> sqrt(amu) * Angstrom
self.vib01_Q *= np.sqrt(u.Ha * u._me / u._amu) * u.Bohr
self.timer.stop('vibrations')
self.timer.start('excitations')
self.init_parallel_read()
if not hasattr(self, 'ex0E_p'):
if self.overlap:
self.read_excitations_overlap()
else:
self.read_excitations()
self.timer.stop('excitations')
self.timer.stop('read')
def me_Qcc(self, omega, gamma):
"""Full matrix element
Returns
-------
Matrix element in e^2 Angstrom^2 / eV
"""
# Angstrom^2 / sqrt(amu)
elme_Qcc = self.electronic_me_Qcc(omega, gamma)
# Angstrom^3 -> e^2 Angstrom^2 / eV
elme_Qcc /= u.Hartree * u.Bohr # e^2 Angstrom / eV / sqrt(amu)
return elme_Qcc * self.vib01_Q[:, None, None]
def intensity(self, omega, gamma=0.1):
"""Raman intensity
Returns
-------
unit e^4 Angstrom^4 / eV^2
"""
m2 = ResonantRaman.m2
alpha_Qcc = self.me_Qcc(omega, gamma)
if not self.observation: # XXXX remove
"""Simple sum, maybe too simple"""
return m2(alpha_Qcc).sum(axis=1).sum(axis=1)
# XXX enable when appropriate
# if self.observation['orientation'].lower() != 'random':
# raise NotImplementedError('not yet')
# random orientation of the molecular frame
# Woodward & Long,
# Guthmuller, J. J. Chem. Phys. 2016, 144 (6), 64106
alpha2_r, gamma2_r, delta2_r = self._invariants(alpha_Qcc)
if self.observation['geometry'] == '-Z(XX)Z': # Porto's notation
return (45 * alpha2_r + 5 * delta2_r + 4 * gamma2_r) / 45.
elif self.observation['geometry'] == '-Z(XY)Z': # Porto's notation
return gamma2_r / 15.
elif self.observation['scattered'] == 'Z':
# scattered light in direction of incoming light
return (45 * alpha2_r + 5 * delta2_r + 7 * gamma2_r) / 45.
elif self.observation['scattered'] == 'parallel':
# scattered light perendicular and
# polarization in plane
return 6 * gamma2_r / 45.
elif self.observation['scattered'] == 'perpendicular':
# scattered light perendicular and
# polarization out of plane
return (45 * alpha2_r + 5 * delta2_r + 7 * gamma2_r) / 45.
else:
raise NotImplementedError
def _invariants(self, alpha_Qcc):
"""Raman invariants
Parameter
---------
alpha_Qcc: array
Matrix element or polarizability tensor
Reference
---------
Derek A. Long, The Raman Effect, ISBN 0-471-49028-8
Returns
-------
mean polarizability, anisotropy, asymmetric anisotropy
"""
m2 = ResonantRaman.m2
alpha2_r = m2(alpha_Qcc[:, 0, 0] + alpha_Qcc[:, 1, 1] +
alpha_Qcc[:, 2, 2]) / 9.
delta2_r = 3 / 4. * (
m2(alpha_Qcc[:, 0, 1] - alpha_Qcc[:, 1, 0]) +
m2(alpha_Qcc[:, 0, 2] - alpha_Qcc[:, 2, 0]) +
m2(alpha_Qcc[:, 1, 2] - alpha_Qcc[:, 2, 1]))
gamma2_r = (3 / 4. * (m2(alpha_Qcc[:, 0, 1] + alpha_Qcc[:, 1, 0]) +
m2(alpha_Qcc[:, 0, 2] + alpha_Qcc[:, 2, 0]) +
m2(alpha_Qcc[:, 1, 2] + alpha_Qcc[:, 2, 1])) +
(m2(alpha_Qcc[:, 0, 0] - alpha_Qcc[:, 1, 1]) +
m2(alpha_Qcc[:, 0, 0] - alpha_Qcc[:, 2, 2]) +
m2(alpha_Qcc[:, 1, 1] - alpha_Qcc[:, 2, 2])) / 2)
return alpha2_r, gamma2_r, delta2_r
def absolute_intensity(self, omega, gamma=0.1, delta=0):
"""Absolute Raman intensity or Raman scattering factor
Parameter
---------
omega: float
incoming laser energy, unit eV
gamma: float
width (imaginary energy), unit eV
delta: float
pre-factor for asymmetric anisotropy, default 0
References
----------
Porezag and Pederson, PRB 54 (1996) 7830-7836 (delta=0)
Baiardi and Barone, JCTC 11 (2015) 3267-3280 (delta=5)
Returns
-------
raman intensity, unit Ang**4/amu
"""
alpha2_r, gamma2_r, delta2_r = self._invariants(
self.electronic_me_Qcc(omega, gamma))
return 45 * alpha2_r + delta * delta2_r + 7 * gamma2_r
def get_cross_sections(self, omega, gamma=0.1):
"""Returns Raman cross sections for each vibration."""
I_v = self.intensity(omega, gamma)
pre = 1. / 16 / np.pi**2 / u._eps0**2 / u._c**4
# frequency of scattered light
omS_v = omega - self.om_v
return pre * omega * omS_v**3 * I_v
def get_spectrum(self, omega, gamma=0.1,
start=None, end=None, npts=None, width=20,
type='Gaussian', method='standard', direction='central',
intensity_unit='????', normalize=False):
"""Get resonant Raman spectrum.
The method returns wavenumbers in cm^-1 with corresponding
Raman cross section.
Start and end point, and width of the Gaussian/Lorentzian should
be given in cm^-1.
"""
self.type = type.lower()
assert self.type in ['gaussian', 'lorentzian']
frequencies = self.get_frequencies(method, direction).real
intensities = self.get_cross_sections(omega, gamma)
if width is None:
return [frequencies, intensities]
if start is None:
start = min(self.om_v) / u.invcm - 3 * width
if end is None:
end = max(self.om_v) / u.invcm + 3 * width
if not npts:
npts = int((end - start) / width * 10 + 1)
prefactor = 1
if self.type == 'lorentzian':
intensities = intensities * width * np.pi / 2.
if normalize:
prefactor = 2. / width / np.pi
else:
sigma = width / 2. / np.sqrt(2. * np.log(2.))
if normalize:
prefactor = 1. / sigma / np.sqrt(2 * np.pi)
# Make array with spectrum data
spectrum = np.empty(npts)
energies = np.linspace(start, end, npts)
for i, energy in enumerate(energies):
energies[i] = energy
if self.type == 'lorentzian':
spectrum[i] = (intensities * 0.5 * width / np.pi /
((frequencies - energy)**2 +
0.25 * width**2)).sum()
else:
spectrum[i] = (intensities *
np.exp(-(frequencies - energy)**2 /
2. / sigma**2)).sum()
return [energies, prefactor * spectrum]
def write_spectrum(self, omega, gamma,
out='resonant-raman-spectra.dat',
start=200, end=4000,
npts=None, width=10,
type='Gaussian', method='standard',
direction='central'):
"""Write out spectrum to file.
Start and end
point, and width of the Gaussian/Lorentzian should be given
in cm^-1."""
energies, spectrum = self.get_spectrum(omega, gamma,
start, end, npts, width,
type, method, direction)
# Write out spectrum in file. First column is absolute intensities.
outdata = np.empty([len(energies), 3])
outdata.T[0] = energies
outdata.T[1] = spectrum
fd = paropen(out, 'w')
fd.write('# Resonant Raman spectrum\n')
if hasattr(self, '_approx'):
fd.write('# approximation: {0}\n'.format(self._approx))
for key in self.observation:
fd.write('# {0}: {1}\n'.format(key, self.observation[key]))
fd.write('# omega={0:g} eV, gamma={1:g} eV\n'.format(omega, gamma))
if width is not None:
fd.write('# %s folded, width=%g cm^-1\n' % (type.title(), width))
fd.write('# [cm^-1] [a.u.]\n')
for row in outdata:
fd.write('%.3f %15.5g\n' %
(row[0], row[1]))
fd.close()
def summary(self, omega=0, gamma=0,
method='standard', direction='central',
log=sys.stdout):
"""Print summary for given omega [eV]"""
hnu = self.get_energies(method, direction)
intensities = self.absolute_intensity(omega, gamma)
te = int(np.log10(intensities.max())) - 2
scale = 10**(-te)
if not te:
ts = ''
elif te > -2 and te < 3:
ts = str(10**te)
else:
ts = '10^{0}'.format(te)
if isinstance(log, basestring):
log = paropen(log, 'a')
parprint('-------------------------------------', file=log)
parprint(' excitation at ' + str(omega) + ' eV', file=log)
parprint(' gamma ' + str(gamma) + ' eV', file=log)
parprint(' method:', self.method, file=log)
parprint(' approximation:', self.approximation, file=log)
parprint(' Mode Frequency Intensity', file=log)
parprint(' # meV cm^-1 [{0}A^4/amu]'.format(ts), file=log)
parprint('-------------------------------------', file=log)
for n, e in enumerate(hnu):
if e.imag != 0:
c = 'i'
e = e.imag
else:
c = ' '
e = e.real
parprint('%3d %6.1f%s %7.1f%s %9.2f' %
(n, 1000 * e, c, e / u.invcm, c, intensities[n] * scale),
file=log)
parprint('-------------------------------------', file=log)
parprint('Zero-point energy: %.3f eV' % self.get_zero_point_energy(),
file=log)
def __del__(self):
self.timer.write(self.txt)
def start(self, name):
Timer.start(self, name)
self.tau_timers[name] = self.pytau.profileTimer(name)
self.pytau.start(self.tau_timers[name])
class HybridXC(HybridXCBase):
orbital_dependent = True
def __init__(self, name, hybrid=None, xc=None,
alpha=None,
gamma_point=1,
method='standard',
bandstructure=False,
logfilename='-', bands=None,
fcut=1e-10,
molecule=False,
qstride=1,
world=None):
"""Mix standard functionals with exact exchange.
name: str
Name of functional: EXX, PBE0, HSE03, HSE06
hybrid: float
Fraction of exact exchange.
xc: str or XCFunctional object
Standard DFT functional with scaled down exchange.
method: str
Use 'standard' standard formula and 'acdf for
adiabatic-connection dissipation fluctuation formula.
alpha: float
XXX describe
gamma_point: bool
0: Skip k2-k1=0 interactions.
1: Use the alpha method.
2: Integrate the gamma point.
bandstructure: bool
Calculate bandstructure instead of just the total energy.
bands: list of int
List of bands to calculate bandstructure for. Default is
all bands.
molecule: bool
Decouple electrostatic interactions between periodically
repeated images.
fcut: float
Threshold for empty band.
"""
self.alpha = alpha
self.fcut = fcut
self.gamma_point = gamma_point
self.method = method
self.bandstructure = bandstructure
self.bands = bands
self.fd = logfilename
self.write_timing_information = True
HybridXCBase.__init__(self, name, hybrid, xc)
# EXX energies:
self.exx = None # total
self.evv = None # valence-valence (pseudo part)
self.evvacdf = None # valence-valence (pseudo part)
self.devv = None # valence-valence (PAW correction)
self.evc = None # valence-core
self.ecc = None # core-core
self.exx_skn = None # bandstructure
self.qlatest = None
if world is None:
world = mpi.world
self.world = world
self.molecule = molecule
if isinstance(qstride, int):
qstride = [qstride] * 3
self.qstride_c = np.asarray(qstride)
self.timer = Timer()
def log(self, *args, **kwargs):
prnt(file=self.fd, *args, **kwargs)
self.fd.flush()
def calculate_radial(self, rgd, n_sLg, Y_L, v_sg,
dndr_sLg=None, rnablaY_Lv=None,
tau_sg=None, dedtau_sg=None):
return self.xc.calculate_radial(rgd, n_sLg, Y_L, v_sg,
dndr_sLg, rnablaY_Lv)
def calculate_paw_correction(self, setup, D_sp, dEdD_sp=None,
addcoredensity=True, a=None):
return self.xc.calculate_paw_correction(setup, D_sp, dEdD_sp,
addcoredensity, a)
def initialize(self, dens, ham, wfs, occupations):
assert wfs.bd.comm.size == 1
self.xc.initialize(dens, ham, wfs, occupations)
self.dens = dens
self.wfs = wfs
# Make a k-point descriptor that is not distributed
# (self.kd.comm is serial_comm):
self.kd = wfs.kd.copy()
self.fd = logfile(self.fd, self.world.rank)
wfs.initialize_wave_functions_from_restart_file()
def set_positions(self, spos_ac):
self.spos_ac = spos_ac
def calculate(self, gd, n_sg, v_sg=None, e_g=None):
# Normal XC contribution:
exc = self.xc.calculate(gd, n_sg, v_sg, e_g)
# Add EXX contribution:
return exc + self.exx * self.hybrid
def calculate_exx(self):
"""Non-selfconsistent calculation."""
self.timer.start('EXX')
self.timer.start('Initialization')
kd = self.kd
wfs = self.wfs
if fftw.FFTPlan is fftw.NumpyFFTPlan:
self.log('NOT USING FFTW !!')
self.log('Spins:', self.wfs.nspins)
W = max(1, self.wfs.kd.comm.size // self.wfs.nspins)
# Are the k-points distributed?
kparallel = (W > 1)
# Find number of occupied bands:
self.nocc_sk = np.zeros((self.wfs.nspins, kd.nibzkpts), int)
for kpt in self.wfs.kpt_u:
for n, f in enumerate(kpt.f_n):
if abs(f) < self.fcut:
self.nocc_sk[kpt.s, kpt.k] = n
break
else:
self.nocc_sk[kpt.s, kpt.k] = self.wfs.bd.nbands
self.wfs.kd.comm.sum(self.nocc_sk)
noccmin = self.nocc_sk.min()
noccmax = self.nocc_sk.max()
self.log('Number of occupied bands (min, max): %d, %d' %
(noccmin, noccmax))
self.log('Number of valence electrons:', self.wfs.setups.nvalence)
if self.bandstructure:
self.log('Calculating eigenvalue shifts.')
# allocate array for eigenvalue shifts:
self.exx_skn = np.zeros((self.wfs.nspins,
kd.nibzkpts,
self.wfs.bd.nbands))
if self.bands is None:
noccmax = self.wfs.bd.nbands
else:
noccmax = max(max(self.bands) + 1, noccmax)
N_c = self.kd.N_c
vol = wfs.gd.dv * wfs.gd.N_c.prod()
if self.alpha is None:
alpha = 6 * vol**(2 / 3.0) / pi**2
else:
alpha = self.alpha
if self.gamma_point == 1:
if alpha == 0.0:
qvol = (2*np.pi)**3 / vol / N_c.prod()
self.gamma = 4*np.pi * (3*qvol / (4*np.pi))**(1/3.) / qvol
else:
self.gamma = self.calculate_gamma(vol, alpha)
else:
kcell_cv = wfs.gd.cell_cv.copy()
kcell_cv[0] *= N_c[0]
kcell_cv[1] *= N_c[1]
kcell_cv[2] *= N_c[2]
self.gamma = madelung(kcell_cv) * vol * N_c.prod() / (4 * np.pi)
self.log('Value of alpha parameter: %.3f Bohr^2' % alpha)
self.log('Value of gamma parameter: %.3f Bohr^2' % self.gamma)
# Construct all possible q=k2-k1 vectors:
Nq_c = (N_c - 1) // self.qstride_c
i_qc = np.indices(Nq_c * 2 + 1, float).transpose(
(1, 2, 3, 0)).reshape((-1, 3))
self.bzq_qc = (i_qc - Nq_c) / N_c * self.qstride_c
self.q0 = ((Nq_c * 2 + 1).prod() - 1) // 2 # index of q=(0,0,0)
assert not self.bzq_qc[self.q0].any()
# Count number of pairs for each q-vector:
self.npairs_q = np.zeros(len(self.bzq_qc), int)
for s in range(kd.nspins):
for k1 in range(kd.nibzkpts):
for k2 in range(kd.nibzkpts):
for K2, q, n1_n, n2 in self.indices(s, k1, k2):
self.npairs_q[q] += len(n1_n)
self.npairs0 = self.npairs_q.sum() # total number of pairs
self.log('Number of pairs:', self.npairs0)
# Distribute q-vectors to Q processors:
Q = self.world.size // self.wfs.kd.comm.size
myrank = self.world.rank // self.wfs.kd.comm.size
rank = 0
N = 0
myq = []
nq = 0
for q, n in enumerate(self.npairs_q):
if n > 0:
nq += 1
if rank == myrank:
myq.append(q)
N += n
if N >= (rank + 1.0) * self.npairs0 / Q:
rank += 1
assert len(myq) > 0, 'Too few q-vectors for too many processes!'
self.bzq_qc = self.bzq_qc[myq]
try:
self.q0 = myq.index(self.q0)
except ValueError:
self.q0 = None
self.log('%d x %d x %d k-points' % tuple(self.kd.N_c))
self.log('Distributing %d IBZ k-points over %d process(es).' %
(kd.nibzkpts, self.wfs.kd.comm.size))
self.log('Distributing %d q-vectors over %d process(es).' % (nq, Q))
# q-point descriptor for my q-vectors:
qd = KPointDescriptor(self.bzq_qc)
# Plane-wave descriptor for all wave-functions:
self.pd = PWDescriptor(wfs.pd.ecut, wfs.gd,
dtype=wfs.pd.dtype, kd=kd)
# Plane-wave descriptor pair-densities:
self.pd2 = PWDescriptor(self.dens.pd2.ecut, self.dens.gd,
dtype=wfs.dtype, kd=qd)
self.log('Cutoff energies:')
self.log(' Wave functions: %10.3f eV' %
(self.pd.ecut * Hartree))
self.log(' Density: %10.3f eV' %
(self.pd2.ecut * Hartree))
# Calculate 1/|G+q|^2 with special treatment of |G+q|=0:
G2_qG = self.pd2.G2_qG
if self.q0 is None:
if self.omega is None:
self.iG2_qG = [1.0 / G2_G for G2_G in G2_qG]
else:
self.iG2_qG = [(1.0 / G2_G *
(1 - np.exp(-G2_G / (4 * self.omega**2))))
for G2_G in G2_qG]
else:
G2_qG[self.q0][0] = 117.0 # avoid division by zero
if self.omega is None:
self.iG2_qG = [1.0 / G2_G for G2_G in G2_qG]
self.iG2_qG[self.q0][0] = self.gamma
else:
self.iG2_qG = [(1.0 / G2_G *
(1 - np.exp(-G2_G / (4 * self.omega**2))))
for G2_G in G2_qG]
self.iG2_qG[self.q0][0] = 1 / (4 * self.omega**2)
G2_qG[self.q0][0] = 0.0 # restore correct value
# Compensation charges:
self.ghat = PWLFC([setup.ghat_l for setup in wfs.setups], self.pd2)
self.ghat.set_positions(self.spos_ac)
if self.molecule:
self.initialize_gaussian()
self.log('Value of beta parameter: %.3f 1/Bohr^2' % self.beta)
self.timer.stop('Initialization')
# Ready ... set ... go:
self.t0 = time()
self.npairs = 0
self.evv = 0.0
self.evvacdf = 0.0
for s in range(self.wfs.nspins):
kpt1_q = [KPoint(self.wfs, noccmax).initialize(kpt)
for kpt in self.wfs.kpt_u if kpt.s == s]
kpt2_q = kpt1_q[:]
if len(kpt1_q) == 0:
# No s-spins on this CPU:
continue
# Send and receive ranks:
srank = self.wfs.kd.get_rank_and_index(
s, (kpt1_q[0].k - 1) % kd.nibzkpts)[0]
rrank = self.wfs.kd.get_rank_and_index(
s, (kpt1_q[-1].k + 1) % kd.nibzkpts)[0]
# Shift k-points kd.nibzkpts - 1 times:
for i in range(kd.nibzkpts):
if i < kd.nibzkpts - 1:
if kparallel:
kpt = kpt2_q[-1].next(self.wfs)
kpt.start_receiving(rrank)
kpt2_q[0].start_sending(srank)
else:
kpt = kpt2_q[0]
self.timer.start('Calculate')
for kpt1, kpt2 in zip(kpt1_q, kpt2_q):
# Loop over all k-points that k2 can be mapped to:
for K2, q, n1_n, n2 in self.indices(s, kpt1.k, kpt2.k):
self.apply(K2, q, kpt1, kpt2, n1_n, n2)
self.timer.stop('Calculate')
if i < kd.nibzkpts - 1:
self.timer.start('Wait')
if kparallel:
kpt.wait()
kpt2_q[0].wait()
self.timer.stop('Wait')
kpt2_q.pop(0)
kpt2_q.append(kpt)
self.evv = self.world.sum(self.evv)
self.evvacdf = self.world.sum(self.evvacdf)
self.calculate_exx_paw_correction()
if self.method == 'standard':
self.exx = self.evv + self.devv + self.evc + self.ecc
elif self.method == 'acdf':
self.exx = self.evvacdf + self.devv + self.evc + self.ecc
else:
1 / 0
self.log('Exact exchange energy:')
for txt, e in [
('core-core', self.ecc),
('valence-core', self.evc),
('valence-valence (pseudo, acdf)', self.evvacdf),
('valence-valence (pseudo, standard)', self.evv),
('valence-valence (correction)', self.devv),
('total (%s)' % self.method, self.exx)]:
self.log(' %-36s %14.6f eV' % (txt + ':', e * Hartree))
self.log('Total time: %10.3f seconds' % (time() - self.t0))
self.npairs = self.world.sum(self.npairs)
assert self.npairs == self.npairs0
self.timer.stop('EXX')
self.timer.write(self.fd)
def calculate_gamma(self, vol, alpha):
if self.molecule:
return 0.0
N_c = self.kd.N_c
offset_c = (N_c + 1) % 2 * 0.5 / N_c
bzq_qc = monkhorst_pack(N_c) + offset_c
qd = KPointDescriptor(bzq_qc)
pd = PWDescriptor(self.wfs.pd.ecut, self.wfs.gd, kd=qd)
gamma = (vol / (2 * pi)**2 * sqrt(pi / alpha) *
self.kd.nbzkpts)
for G2_G in pd.G2_qG:
if G2_G[0] < 1e-7:
G2_G = G2_G[1:]
gamma -= np.dot(np.exp(-alpha * G2_G), G2_G**-1)
return gamma / self.qstride_c.prod()
def indices(self, s, k1, k2):
"""Generator for (K2, q, n1, n2) indices for (k1, k2) pair.
s: int
Spin index.
k1: int
Index of k-point in the IBZ.
k2: int
Index of k-point in the IBZ.
Returns (K, q, n1_n, n2), where K then index of the k-point in
the BZ that k2 is mapped to, q is the index of the q-vector
between K and k1, and n1_n is a list of bands that should be
combined with band n2."""
for K, k in enumerate(self.kd.bz2ibz_k):
if k == k2:
for K, q, n1_n, n2 in self._indices(s, k1, k2, K):
yield K, q, n1_n, n2
def _indices(self, s, k1, k2, K2):
k1_c = self.kd.ibzk_kc[k1]
k2_c = self.kd.bzk_kc[K2]
q_c = k2_c - k1_c
q = abs(self.bzq_qc - q_c).sum(1).argmin()
if abs(self.bzq_qc[q] - q_c).sum() > 1e-7:
return
if self.gamma_point == 0 and q == self.q0:
return
nocc1 = self.nocc_sk[s, k1]
nocc2 = self.nocc_sk[s, k2]
# Is k2 in the IBZ?
is_ibz2 = (self.kd.ibz2bz_k[k2] == K2)
for n2 in range(self.wfs.bd.nbands):
# Find range of n1's (from n1a to n1b-1):
if is_ibz2:
# We get this combination twice, so let's only do half:
if k1 >= k2:
n1a = n2
else:
n1a = n2 + 1
else:
n1a = 0
n1b = self.wfs.bd.nbands
if self.bandstructure:
if n2 >= nocc2:
n1b = min(n1b, nocc1)
else:
if n2 >= nocc2:
break
n1b = min(n1b, nocc1)
if self.bands is not None:
assert self.bandstructure
n1_n = []
for n1 in range(n1a, n1b):
if (n1 in self.bands and n2 < nocc2 or
is_ibz2 and n2 in self.bands and n1 < nocc1):
n1_n.append(n1)
n1_n = np.array(n1_n)
else:
n1_n = np.arange(n1a, n1b)
if len(n1_n) == 0:
continue
yield K2, q, n1_n, n2
def apply(self, K2, q, kpt1, kpt2, n1_n, n2):
k20_c = self.kd.ibzk_kc[kpt2.k]
k2_c = self.kd.bzk_kc[K2]
if k2_c.any():
self.timer.start('Initialize plane waves')
eik2r_R = self.wfs.gd.plane_wave(k2_c)
eik20r_R = self.wfs.gd.plane_wave(k20_c)
self.timer.stop('Initialize plane waves')
else:
eik2r_R = 1.0
eik20r_R = 1.0
w1 = self.kd.weight_k[kpt1.k]
w2 = self.kd.weight_k[kpt2.k]
# Is k2 in the 1. BZ?
is_ibz2 = (self.kd.ibz2bz_k[kpt2.k] == K2)
e_n = self.calculate_interaction(n1_n, n2, kpt1, kpt2, q, K2,
eik20r_R, eik2r_R,
is_ibz2)
e_n *= 1.0 / self.kd.nbzkpts / self.wfs.nspins * self.qstride_c.prod()
if q == self.q0:
e_n[n1_n == n2] *= 0.5
f1_n = kpt1.f_n[n1_n]
eps1_n = kpt1.eps_n[n1_n]
f2 = kpt2.f_n[n2]
eps2 = kpt2.eps_n[n2]
s_n = np.sign(eps2 - eps1_n)
evv = (f1_n * f2 * e_n).sum()
evvacdf = 0.5 * (f1_n * (1 - s_n) * e_n +
f2 * (1 + s_n) * e_n).sum()
self.evv += evv * w1
self.evvacdf += evvacdf * w1
if is_ibz2:
self.evv += evv * w2
self.evvacdf += evvacdf * w2
if self.bandstructure:
x = self.wfs.nspins
self.exx_skn[kpt1.s, kpt1.k, n1_n] += x * f2 * e_n
if is_ibz2:
self.exx_skn[kpt2.s, kpt2.k, n2] += x * np.dot(f1_n, e_n)
def calculate_interaction(self, n1_n, n2, kpt1, kpt2, q, k,
eik20r_R, eik2r_R, is_ibz2):
"""Calculate Coulomb interactions.
For all n1 in the n1_n list, calculate interaction with n2."""
# number of plane waves:
ng1 = self.wfs.ng_k[kpt1.k]
ng2 = self.wfs.ng_k[kpt2.k]
# Transform to real space and apply symmetry operation:
self.timer.start('IFFT1')
if is_ibz2:
u2_R = self.pd.ifft(kpt2.psit_nG[n2, :ng2], kpt2.k)
else:
psit2_R = self.pd.ifft(kpt2.psit_nG[n2, :ng2], kpt2.k) * eik20r_R
self.timer.start('Symmetry transform')
u2_R = self.kd.transform_wave_function(psit2_R, k) / eik2r_R
self.timer.stop()
self.timer.stop()
# Calculate pair densities:
nt_nG = self.pd2.zeros(len(n1_n), q=q)
for n1, nt_G in zip(n1_n, nt_nG):
self.timer.start('IFFT2')
u1_R = self.pd.ifft(kpt1.psit_nG[n1, :ng1], kpt1.k)
self.timer.stop()
nt_R = u1_R.conj() * u2_R
self.timer.start('FFT')
nt_G[:] = self.pd2.fft(nt_R, q)
self.timer.stop()
s = self.kd.sym_k[k]
time_reversal = self.kd.time_reversal_k[k]
k2_c = self.kd.ibzk_kc[kpt2.k]
self.timer.start('Compensation charges')
Q_anL = {} # coefficients for shape functions
for a, P1_ni in kpt1.P_ani.items():
P1_ni = P1_ni[n1_n]
if is_ibz2:
P2_i = kpt2.P_ani[a][n2]
else:
b = self.kd.symmetry.a_sa[s, a]
S_c = (np.dot(self.spos_ac[a], self.kd.symmetry.op_scc[s]) -
self.spos_ac[b])
assert abs(S_c.round() - S_c).max() < 1e-5
if self.ghat.dtype == complex:
x = np.exp(2j * pi * np.dot(k2_c, S_c))
else:
x = 1.0
P2_i = np.dot(self.wfs.setups[a].R_sii[s],
kpt2.P_ani[b][n2]) * x
if time_reversal:
P2_i = P2_i.conj()
D_np = []
for P1_i in P1_ni:
D_ii = np.outer(P1_i.conj(), P2_i)
D_np.append(pack(D_ii))
Q_anL[a] = np.dot(D_np, self.wfs.setups[a].Delta_pL)
self.timer.start('Expand')
if q != self.qlatest:
self.f_IG = self.ghat.expand(q)
self.qlatest = q
self.timer.stop('Expand')
# Add compensation charges:
self.ghat.add(nt_nG, Q_anL, q, self.f_IG)
self.timer.stop('Compensation charges')
if self.molecule and n2 in n1_n:
nn = (n1_n == n2).nonzero()[0][0]
nt_nG[nn] -= self.ngauss_G
else:
nn = None
iG2_G = self.iG2_qG[q]
# Calculate energies:
e_n = np.empty(len(n1_n))
for n, nt_G in enumerate(nt_nG):
e_n[n] = -4 * pi * np.real(self.pd2.integrate(nt_G, nt_G * iG2_G))
self.npairs += 1
if nn is not None:
e_n[nn] -= 2 * (self.pd2.integrate(nt_nG[nn], self.vgauss_G) +
(self.beta / 2 / pi)**0.5)
if self.write_timing_information:
t = (time() - self.t0) / len(n1_n)
self.log('Time for first pair-density: %10.3f seconds' % t)
self.log('Estimated total time: %10.3f seconds' %
(t * self.npairs0 / self.world.size))
self.write_timing_information = False
return e_n
def calculate_exx_paw_correction(self):
self.timer.start('PAW correction')
self.devv = 0.0
self.evc = 0.0
self.ecc = 0.0
deg = 2 // self.wfs.nspins # spin degeneracy
for a, D_sp in self.dens.D_asp.items():
setup = self.wfs.setups[a]
for D_p in D_sp:
D_ii = unpack2(D_p)
ni = len(D_ii)
for i1 in range(ni):
for i2 in range(ni):
A = 0.0
for i3 in range(ni):
p13 = packed_index(i1, i3, ni)
for i4 in range(ni):
p24 = packed_index(i2, i4, ni)
A += setup.M_pp[p13, p24] * D_ii[i3, i4]
self.devv -= D_ii[i1, i2] * A / deg
self.evc -= np.dot(D_p, setup.X_p)
self.ecc += setup.ExxC
if not self.bandstructure:
self.timer.stop('PAW correction')
return
Q = self.world.size // self.wfs.kd.comm.size
self.exx_skn *= Q
for kpt in self.wfs.kpt_u:
for a, D_sp in self.dens.D_asp.items():
setup = self.wfs.setups[a]
for D_p in D_sp:
D_ii = unpack2(D_p)
ni = len(D_ii)
P_ni = kpt.P_ani[a]
for i1 in range(ni):
for i2 in range(ni):
A = 0.0
for i3 in range(ni):
p13 = packed_index(i1, i3, ni)
for i4 in range(ni):
p24 = packed_index(i2, i4, ni)
A += setup.M_pp[p13, p24] * D_ii[i3, i4]
self.exx_skn[kpt.s, kpt.k] -= \
(A * P_ni[:, i1].conj() * P_ni[:, i2]).real
p12 = packed_index(i1, i2, ni)
self.exx_skn[kpt.s, kpt.k] -= \
(P_ni[:, i1].conj() * setup.X_p[p12] *
P_ni[:, i2]).real / self.wfs.nspins
self.world.sum(self.exx_skn)
self.exx_skn *= self.hybrid / Q
self.timer.stop('PAW correction')
def initialize_gaussian(self):
"""Calculate gaussian compensation charge and its potential.
Used to decouple electrostatic interactions between
periodically repeated images for molecular calculations.
Charge containing one electron::
(beta/pi)^(3/2)*exp(-beta*r^2),
its Fourier transform::
exp(-G^2/(4*beta)),
and its potential::
erf(beta^0.5*r)/r.
"""
gd = self.wfs.gd
# Set exponent of exp-function to -19 on the boundary:
self.beta = 4 * 19 * (gd.icell_cv**2).sum(1).max()
# Calculate gaussian:
G_Gv = self.pd2.get_reciprocal_vectors()
G2_G = self.pd2.G2_qG[0]
C_v = gd.cell_cv.sum(0) / 2 # center of cell
self.ngauss_G = np.exp(-1.0 / (4 * self.beta) * G2_G +
1j * np.dot(G_Gv, C_v)) / gd.dv
# Calculate potential from gaussian:
R_Rv = gd.get_grid_point_coordinates().transpose((1, 2, 3, 0))
r_R = ((R_Rv - C_v)**2).sum(3)**0.5
if (gd.N_c % 2 == 0).all():
r_R[tuple(gd.N_c // 2)] = 1.0 # avoid dividing by zero
v_R = erf(self.beta**0.5 * r_R) / r_R
if (gd.N_c % 2 == 0).all():
v_R[tuple(gd.N_c // 2)] = (4 * self.beta / pi)**0.5
self.vgauss_G = self.pd2.fft(v_R)
# Compare self-interaction to analytic result:
assert abs(0.5 * self.pd2.integrate(self.ngauss_G, self.vgauss_G) -
(self.beta / 2 / pi)**0.5) < 1e-6
class HybridXC(HybridXCBase):
orbital_dependent = True
def __init__(self,
name,
hybrid=None,
xc=None,
alpha=None,
gamma_point=1,
method='standard',
bandstructure=False,
logfilename='-',
bands=None,
fcut=1e-10,
molecule=False,
qstride=1,
world=None):
"""Mix standard functionals with exact exchange.
name: str
Name of functional: EXX, PBE0, HSE03, HSE06
hybrid: float
Fraction of exact exchange.
xc: str or XCFunctional object
Standard DFT functional with scaled down exchange.
method: str
Use 'standard' standard formula and 'acdf for
adiabatic-connection dissipation fluctuation formula.
alpha: float
XXX describe
gamma_point: bool
0: Skip k2-k1=0 interactions.
1: Use the alpha method.
2: Integrate the gamma point.
bandstructure: bool
Calculate bandstructure instead of just the total energy.
bands: list of int
List of bands to calculate bandstructure for. Default is
all bands.
molecule: bool
Decouple electrostatic interactions between periodically
repeated images.
fcut: float
Threshold for empty band.
"""
self.alpha = alpha
self.fcut = fcut
self.gamma_point = gamma_point
self.method = method
self.bandstructure = bandstructure
self.bands = bands
self.fd = logfilename
self.write_timing_information = True
HybridXCBase.__init__(self, name, hybrid, xc)
# EXX energies:
self.exx = None # total
self.evv = None # valence-valence (pseudo part)
self.evvacdf = None # valence-valence (pseudo part)
self.devv = None # valence-valence (PAW correction)
self.evc = None # valence-core
self.ecc = None # core-core
self.exx_skn = None # bandstructure
self.qlatest = None
if world is None:
world = mpi.world
self.world = world
self.molecule = molecule
if isinstance(qstride, int):
qstride = [qstride] * 3
self.qstride_c = np.asarray(qstride)
self.timer = Timer()
def log(self, *args, **kwargs):
prnt(file=self.fd, *args, **kwargs)
self.fd.flush()
def calculate_radial(self,
rgd,
n_sLg,
Y_L,
v_sg,
dndr_sLg=None,
rnablaY_Lv=None,
tau_sg=None,
dedtau_sg=None):
return self.xc.calculate_radial(rgd, n_sLg, Y_L, v_sg, dndr_sLg,
rnablaY_Lv)
def calculate_paw_correction(self,
setup,
D_sp,
dEdD_sp=None,
addcoredensity=True,
a=None):
return self.xc.calculate_paw_correction(setup, D_sp, dEdD_sp,
addcoredensity, a)
def initialize(self, dens, ham, wfs, occupations):
assert wfs.bd.comm.size == 1
self.xc.initialize(dens, ham, wfs, occupations)
self.dens = dens
self.wfs = wfs
# Make a k-point descriptor that is not distributed
# (self.kd.comm is serial_comm):
self.kd = wfs.kd.copy()
self.fd = logfile(self.fd, self.world.rank)
wfs.initialize_wave_functions_from_restart_file()
def set_positions(self, spos_ac):
self.spos_ac = spos_ac
def calculate(self, gd, n_sg, v_sg=None, e_g=None):
# Normal XC contribution:
exc = self.xc.calculate(gd, n_sg, v_sg, e_g)
# Add EXX contribution:
return exc + self.exx * self.hybrid
def calculate_exx(self):
"""Non-selfconsistent calculation."""
self.timer.start('EXX')
self.timer.start('Initialization')
kd = self.kd
wfs = self.wfs
if fftw.FFTPlan is fftw.NumpyFFTPlan:
self.log('NOT USING FFTW !!')
self.log('Spins:', self.wfs.nspins)
W = max(1, self.wfs.kd.comm.size // self.wfs.nspins)
# Are the k-points distributed?
kparallel = (W > 1)
# Find number of occupied bands:
self.nocc_sk = np.zeros((self.wfs.nspins, kd.nibzkpts), int)
for kpt in self.wfs.kpt_u:
for n, f in enumerate(kpt.f_n):
if abs(f) < self.fcut:
self.nocc_sk[kpt.s, kpt.k] = n
break
else:
self.nocc_sk[kpt.s, kpt.k] = self.wfs.bd.nbands
self.wfs.kd.comm.sum(self.nocc_sk)
noccmin = self.nocc_sk.min()
noccmax = self.nocc_sk.max()
self.log('Number of occupied bands (min, max): %d, %d' %
(noccmin, noccmax))
self.log('Number of valence electrons:', self.wfs.setups.nvalence)
if self.bandstructure:
self.log('Calculating eigenvalue shifts.')
# allocate array for eigenvalue shifts:
self.exx_skn = np.zeros(
(self.wfs.nspins, kd.nibzkpts, self.wfs.bd.nbands))
if self.bands is None:
noccmax = self.wfs.bd.nbands
else:
noccmax = max(max(self.bands) + 1, noccmax)
N_c = self.kd.N_c
vol = wfs.gd.dv * wfs.gd.N_c.prod()
if self.alpha is None:
alpha = 6 * vol**(2 / 3.0) / pi**2
else:
alpha = self.alpha
if self.gamma_point == 1:
if alpha == 0.0:
qvol = (2 * np.pi)**3 / vol / N_c.prod()
self.gamma = 4 * np.pi * (3 * qvol /
(4 * np.pi))**(1 / 3.) / qvol
else:
self.gamma = self.calculate_gamma(vol, alpha)
else:
kcell_cv = wfs.gd.cell_cv.copy()
kcell_cv[0] *= N_c[0]
kcell_cv[1] *= N_c[1]
kcell_cv[2] *= N_c[2]
self.gamma = madelung(kcell_cv) * vol * N_c.prod() / (4 * np.pi)
self.log('Value of alpha parameter: %.3f Bohr^2' % alpha)
self.log('Value of gamma parameter: %.3f Bohr^2' % self.gamma)
# Construct all possible q=k2-k1 vectors:
Nq_c = (N_c - 1) // self.qstride_c
i_qc = np.indices(Nq_c * 2 + 1, float).transpose((1, 2, 3, 0)).reshape(
(-1, 3))
self.bzq_qc = (i_qc - Nq_c) / N_c * self.qstride_c
self.q0 = ((Nq_c * 2 + 1).prod() - 1) // 2 # index of q=(0,0,0)
assert not self.bzq_qc[self.q0].any()
# Count number of pairs for each q-vector:
self.npairs_q = np.zeros(len(self.bzq_qc), int)
for s in range(kd.nspins):
for k1 in range(kd.nibzkpts):
for k2 in range(kd.nibzkpts):
for K2, q, n1_n, n2 in self.indices(s, k1, k2):
self.npairs_q[q] += len(n1_n)
self.npairs0 = self.npairs_q.sum() # total number of pairs
self.log('Number of pairs:', self.npairs0)
# Distribute q-vectors to Q processors:
Q = self.world.size // self.wfs.kd.comm.size
myrank = self.world.rank // self.wfs.kd.comm.size
rank = 0
N = 0
myq = []
nq = 0
for q, n in enumerate(self.npairs_q):
if n > 0:
nq += 1
if rank == myrank:
myq.append(q)
N += n
if N >= (rank + 1.0) * self.npairs0 / Q:
rank += 1
assert len(myq) > 0, 'Too few q-vectors for too many processes!'
self.bzq_qc = self.bzq_qc[myq]
try:
self.q0 = myq.index(self.q0)
except ValueError:
self.q0 = None
self.log('%d x %d x %d k-points' % tuple(self.kd.N_c))
self.log('Distributing %d IBZ k-points over %d process(es).' %
(kd.nibzkpts, self.wfs.kd.comm.size))
self.log('Distributing %d q-vectors over %d process(es).' % (nq, Q))
# q-point descriptor for my q-vectors:
qd = KPointDescriptor(self.bzq_qc)
# Plane-wave descriptor for all wave-functions:
self.pd = PWDescriptor(wfs.pd.ecut, wfs.gd, dtype=wfs.pd.dtype, kd=kd)
# Plane-wave descriptor pair-densities:
self.pd2 = PWDescriptor(self.dens.pd2.ecut,
self.dens.gd,
dtype=wfs.dtype,
kd=qd)
self.log('Cutoff energies:')
self.log(' Wave functions: %10.3f eV' %
(self.pd.ecut * Hartree))
self.log(' Density: %10.3f eV' %
(self.pd2.ecut * Hartree))
# Calculate 1/|G+q|^2 with special treatment of |G+q|=0:
G2_qG = self.pd2.G2_qG
if self.q0 is None:
if self.omega is None:
self.iG2_qG = [1.0 / G2_G for G2_G in G2_qG]
else:
self.iG2_qG = [
(1.0 / G2_G * (1 - np.exp(-G2_G / (4 * self.omega**2))))
for G2_G in G2_qG
]
else:
G2_qG[self.q0][0] = 117.0 # avoid division by zero
if self.omega is None:
self.iG2_qG = [1.0 / G2_G for G2_G in G2_qG]
self.iG2_qG[self.q0][0] = self.gamma
else:
self.iG2_qG = [
(1.0 / G2_G * (1 - np.exp(-G2_G / (4 * self.omega**2))))
for G2_G in G2_qG
]
self.iG2_qG[self.q0][0] = 1 / (4 * self.omega**2)
G2_qG[self.q0][0] = 0.0 # restore correct value
# Compensation charges:
self.ghat = PWLFC([setup.ghat_l for setup in wfs.setups], self.pd2)
self.ghat.set_positions(self.spos_ac)
if self.molecule:
self.initialize_gaussian()
self.log('Value of beta parameter: %.3f 1/Bohr^2' % self.beta)
self.timer.stop('Initialization')
# Ready ... set ... go:
self.t0 = time()
self.npairs = 0
self.evv = 0.0
self.evvacdf = 0.0
for s in range(self.wfs.nspins):
kpt1_q = [
KPoint(self.wfs, noccmax).initialize(kpt)
for kpt in self.wfs.kpt_u if kpt.s == s
]
kpt2_q = kpt1_q[:]
if len(kpt1_q) == 0:
# No s-spins on this CPU:
continue
# Send and receive ranks:
srank = self.wfs.kd.get_rank_and_index(s, (kpt1_q[0].k - 1) %
kd.nibzkpts)[0]
rrank = self.wfs.kd.get_rank_and_index(s, (kpt1_q[-1].k + 1) %
kd.nibzkpts)[0]
# Shift k-points kd.nibzkpts - 1 times:
for i in range(kd.nibzkpts):
if i < kd.nibzkpts - 1:
if kparallel:
kpt = kpt2_q[-1].next(self.wfs)
kpt.start_receiving(rrank)
kpt2_q[0].start_sending(srank)
else:
kpt = kpt2_q[0]
self.timer.start('Calculate')
for kpt1, kpt2 in zip(kpt1_q, kpt2_q):
# Loop over all k-points that k2 can be mapped to:
for K2, q, n1_n, n2 in self.indices(s, kpt1.k, kpt2.k):
self.apply(K2, q, kpt1, kpt2, n1_n, n2)
self.timer.stop('Calculate')
if i < kd.nibzkpts - 1:
self.timer.start('Wait')
if kparallel:
kpt.wait()
kpt2_q[0].wait()
self.timer.stop('Wait')
kpt2_q.pop(0)
kpt2_q.append(kpt)
self.evv = self.world.sum(self.evv)
self.evvacdf = self.world.sum(self.evvacdf)
self.calculate_exx_paw_correction()
if self.method == 'standard':
self.exx = self.evv + self.devv + self.evc + self.ecc
elif self.method == 'acdf':
self.exx = self.evvacdf + self.devv + self.evc + self.ecc
else:
1 / 0
self.log('Exact exchange energy:')
for txt, e in [('core-core', self.ecc), ('valence-core', self.evc),
('valence-valence (pseudo, acdf)', self.evvacdf),
('valence-valence (pseudo, standard)', self.evv),
('valence-valence (correction)', self.devv),
('total (%s)' % self.method, self.exx)]:
self.log(' %-36s %14.6f eV' % (txt + ':', e * Hartree))
self.log('Total time: %10.3f seconds' % (time() - self.t0))
self.npairs = self.world.sum(self.npairs)
assert self.npairs == self.npairs0
self.timer.stop('EXX')
self.timer.write(self.fd)
def calculate_gamma(self, vol, alpha):
if self.molecule:
return 0.0
N_c = self.kd.N_c
offset_c = (N_c + 1) % 2 * 0.5 / N_c
bzq_qc = monkhorst_pack(N_c) + offset_c
qd = KPointDescriptor(bzq_qc)
pd = PWDescriptor(self.wfs.pd.ecut, self.wfs.gd, kd=qd)
gamma = (vol / (2 * pi)**2 * sqrt(pi / alpha) * self.kd.nbzkpts)
for G2_G in pd.G2_qG:
if G2_G[0] < 1e-7:
G2_G = G2_G[1:]
gamma -= np.dot(np.exp(-alpha * G2_G), G2_G**-1)
return gamma / self.qstride_c.prod()
def indices(self, s, k1, k2):
"""Generator for (K2, q, n1, n2) indices for (k1, k2) pair.
s: int
Spin index.
k1: int
Index of k-point in the IBZ.
k2: int
Index of k-point in the IBZ.
Returns (K, q, n1_n, n2), where K then index of the k-point in
the BZ that k2 is mapped to, q is the index of the q-vector
between K and k1, and n1_n is a list of bands that should be
combined with band n2."""
for K, k in enumerate(self.kd.bz2ibz_k):
if k == k2:
for K, q, n1_n, n2 in self._indices(s, k1, k2, K):
yield K, q, n1_n, n2
def _indices(self, s, k1, k2, K2):
k1_c = self.kd.ibzk_kc[k1]
k2_c = self.kd.bzk_kc[K2]
q_c = k2_c - k1_c
q = abs(self.bzq_qc - q_c).sum(1).argmin()
if abs(self.bzq_qc[q] - q_c).sum() > 1e-7:
return
if self.gamma_point == 0 and q == self.q0:
return
nocc1 = self.nocc_sk[s, k1]
nocc2 = self.nocc_sk[s, k2]
# Is k2 in the IBZ?
is_ibz2 = (self.kd.ibz2bz_k[k2] == K2)
for n2 in range(self.wfs.bd.nbands):
# Find range of n1's (from n1a to n1b-1):
if is_ibz2:
# We get this combination twice, so let's only do half:
if k1 >= k2:
n1a = n2
else:
n1a = n2 + 1
else:
n1a = 0
n1b = self.wfs.bd.nbands
if self.bandstructure:
if n2 >= nocc2:
n1b = min(n1b, nocc1)
else:
if n2 >= nocc2:
break
n1b = min(n1b, nocc1)
if self.bands is not None:
assert self.bandstructure
n1_n = []
for n1 in range(n1a, n1b):
if (n1 in self.bands and n2 < nocc2
or is_ibz2 and n2 in self.bands and n1 < nocc1):
n1_n.append(n1)
n1_n = np.array(n1_n)
else:
n1_n = np.arange(n1a, n1b)
if len(n1_n) == 0:
continue
yield K2, q, n1_n, n2
def apply(self, K2, q, kpt1, kpt2, n1_n, n2):
k20_c = self.kd.ibzk_kc[kpt2.k]
k2_c = self.kd.bzk_kc[K2]
if k2_c.any():
self.timer.start('Initialize plane waves')
eik2r_R = self.wfs.gd.plane_wave(k2_c)
eik20r_R = self.wfs.gd.plane_wave(k20_c)
self.timer.stop('Initialize plane waves')
else:
eik2r_R = 1.0
eik20r_R = 1.0
w1 = self.kd.weight_k[kpt1.k]
w2 = self.kd.weight_k[kpt2.k]
# Is k2 in the 1. BZ?
is_ibz2 = (self.kd.ibz2bz_k[kpt2.k] == K2)
e_n = self.calculate_interaction(n1_n, n2, kpt1, kpt2, q, K2, eik20r_R,
eik2r_R, is_ibz2)
e_n *= 1.0 / self.kd.nbzkpts / self.wfs.nspins * self.qstride_c.prod()
if q == self.q0:
e_n[n1_n == n2] *= 0.5
f1_n = kpt1.f_n[n1_n]
eps1_n = kpt1.eps_n[n1_n]
f2 = kpt2.f_n[n2]
eps2 = kpt2.eps_n[n2]
s_n = np.sign(eps2 - eps1_n)
evv = (f1_n * f2 * e_n).sum()
evvacdf = 0.5 * (f1_n * (1 - s_n) * e_n + f2 * (1 + s_n) * e_n).sum()
self.evv += evv * w1
self.evvacdf += evvacdf * w1
if is_ibz2:
self.evv += evv * w2
self.evvacdf += evvacdf * w2
if self.bandstructure:
x = self.wfs.nspins
self.exx_skn[kpt1.s, kpt1.k, n1_n] += x * f2 * e_n
if is_ibz2:
self.exx_skn[kpt2.s, kpt2.k, n2] += x * np.dot(f1_n, e_n)
def calculate_interaction(self, n1_n, n2, kpt1, kpt2, q, k, eik20r_R,
eik2r_R, is_ibz2):
"""Calculate Coulomb interactions.
For all n1 in the n1_n list, calculate interaction with n2."""
# number of plane waves:
ng1 = self.wfs.ng_k[kpt1.k]
ng2 = self.wfs.ng_k[kpt2.k]
# Transform to real space and apply symmetry operation:
self.timer.start('IFFT1')
if is_ibz2:
u2_R = self.pd.ifft(kpt2.psit_nG[n2, :ng2], kpt2.k)
else:
psit2_R = self.pd.ifft(kpt2.psit_nG[n2, :ng2], kpt2.k) * eik20r_R
self.timer.start('Symmetry transform')
u2_R = self.kd.transform_wave_function(psit2_R, k) / eik2r_R
self.timer.stop()
self.timer.stop()
# Calculate pair densities:
nt_nG = self.pd2.zeros(len(n1_n), q=q)
for n1, nt_G in zip(n1_n, nt_nG):
self.timer.start('IFFT2')
u1_R = self.pd.ifft(kpt1.psit_nG[n1, :ng1], kpt1.k)
self.timer.stop()
nt_R = u1_R.conj() * u2_R
self.timer.start('FFT')
nt_G[:] = self.pd2.fft(nt_R, q)
self.timer.stop()
s = self.kd.sym_k[k]
time_reversal = self.kd.time_reversal_k[k]
k2_c = self.kd.ibzk_kc[kpt2.k]
self.timer.start('Compensation charges')
Q_anL = {} # coefficients for shape functions
for a, P1_ni in kpt1.P_ani.items():
P1_ni = P1_ni[n1_n]
if is_ibz2:
P2_i = kpt2.P_ani[a][n2]
else:
b = self.kd.symmetry.a_sa[s, a]
S_c = (np.dot(self.spos_ac[a], self.kd.symmetry.op_scc[s]) -
self.spos_ac[b])
assert abs(S_c.round() - S_c).max() < 1e-5
if self.ghat.dtype == complex:
x = np.exp(2j * pi * np.dot(k2_c, S_c))
else:
x = 1.0
P2_i = np.dot(self.wfs.setups[a].R_sii[s],
kpt2.P_ani[b][n2]) * x
if time_reversal:
P2_i = P2_i.conj()
D_np = []
for P1_i in P1_ni:
D_ii = np.outer(P1_i.conj(), P2_i)
D_np.append(pack(D_ii))
Q_anL[a] = np.dot(D_np, self.wfs.setups[a].Delta_pL)
self.timer.start('Expand')
if q != self.qlatest:
self.f_IG = self.ghat.expand(q)
self.qlatest = q
self.timer.stop('Expand')
# Add compensation charges:
self.ghat.add(nt_nG, Q_anL, q, self.f_IG)
self.timer.stop('Compensation charges')
if self.molecule and n2 in n1_n:
nn = (n1_n == n2).nonzero()[0][0]
nt_nG[nn] -= self.ngauss_G
else:
nn = None
iG2_G = self.iG2_qG[q]
# Calculate energies:
e_n = np.empty(len(n1_n))
for n, nt_G in enumerate(nt_nG):
e_n[n] = -4 * pi * np.real(self.pd2.integrate(nt_G, nt_G * iG2_G))
self.npairs += 1
if nn is not None:
e_n[nn] -= 2 * (self.pd2.integrate(nt_nG[nn], self.vgauss_G) +
(self.beta / 2 / pi)**0.5)
if self.write_timing_information:
t = (time() - self.t0) / len(n1_n)
self.log('Time for first pair-density: %10.3f seconds' % t)
self.log('Estimated total time: %10.3f seconds' %
(t * self.npairs0 / self.world.size))
self.write_timing_information = False
return e_n
def calculate_exx_paw_correction(self):
self.timer.start('PAW correction')
self.devv = 0.0
self.evc = 0.0
self.ecc = 0.0
deg = 2 // self.wfs.nspins # spin degeneracy
for a, D_sp in self.dens.D_asp.items():
setup = self.wfs.setups[a]
for D_p in D_sp:
D_ii = unpack2(D_p)
ni = len(D_ii)
for i1 in range(ni):
for i2 in range(ni):
A = 0.0
for i3 in range(ni):
p13 = packed_index(i1, i3, ni)
for i4 in range(ni):
p24 = packed_index(i2, i4, ni)
A += setup.M_pp[p13, p24] * D_ii[i3, i4]
self.devv -= D_ii[i1, i2] * A / deg
self.evc -= np.dot(D_p, setup.X_p)
self.ecc += setup.ExxC
if not self.bandstructure:
self.timer.stop('PAW correction')
return
Q = self.world.size // self.wfs.kd.comm.size
self.exx_skn *= Q
for kpt in self.wfs.kpt_u:
for a, D_sp in self.dens.D_asp.items():
setup = self.wfs.setups[a]
for D_p in D_sp:
D_ii = unpack2(D_p)
ni = len(D_ii)
P_ni = kpt.P_ani[a]
for i1 in range(ni):
for i2 in range(ni):
A = 0.0
for i3 in range(ni):
p13 = packed_index(i1, i3, ni)
for i4 in range(ni):
p24 = packed_index(i2, i4, ni)
A += setup.M_pp[p13, p24] * D_ii[i3, i4]
self.exx_skn[kpt.s, kpt.k] -= \
(A * P_ni[:, i1].conj() * P_ni[:, i2]).real
p12 = packed_index(i1, i2, ni)
self.exx_skn[kpt.s, kpt.k] -= \
(P_ni[:, i1].conj() * setup.X_p[p12] *
P_ni[:, i2]).real / self.wfs.nspins
self.world.sum(self.exx_skn)
self.exx_skn *= self.hybrid / Q
self.timer.stop('PAW correction')
def initialize_gaussian(self):
"""Calculate gaussian compensation charge and its potential.
Used to decouple electrostatic interactions between
periodically repeated images for molecular calculations.
Charge containing one electron::
(beta/pi)^(3/2)*exp(-beta*r^2),
its Fourier transform::
exp(-G^2/(4*beta)),
and its potential::
erf(beta^0.5*r)/r.
"""
gd = self.wfs.gd
# Set exponent of exp-function to -19 on the boundary:
self.beta = 4 * 19 * (gd.icell_cv**2).sum(1).max()
# Calculate gaussian:
G_Gv = self.pd2.get_reciprocal_vectors()
G2_G = self.pd2.G2_qG[0]
C_v = gd.cell_cv.sum(0) / 2 # center of cell
self.ngauss_G = np.exp(-1.0 / (4 * self.beta) * G2_G +
1j * np.dot(G_Gv, C_v)) / gd.dv
# Calculate potential from gaussian:
R_Rv = gd.get_grid_point_coordinates().transpose((1, 2, 3, 0))
r_R = ((R_Rv - C_v)**2).sum(3)**0.5
if (gd.N_c % 2 == 0).all():
r_R[tuple(gd.N_c // 2)] = 1.0 # avoid dividing by zero
v_R = erf(self.beta**0.5 * r_R) / r_R
if (gd.N_c % 2 == 0).all():
v_R[tuple(gd.N_c // 2)] = (4 * self.beta / pi)**0.5
self.vgauss_G = self.pd2.fft(v_R)
# Compare self-interaction to analytic result:
assert abs(0.5 * self.pd2.integrate(self.ngauss_G, self.vgauss_G) -
(self.beta / 2 / pi)**0.5) < 1e-6
class LrTDDFT(ExcitationList):
"""Linear Response TDDFT excitation class
Input parameters:
calculator:
the calculator object after a ground state calculation
nspins:
number of spins considered in the calculation
Note: Valid only for unpolarised ground state calculation
eps:
Minimal occupation difference for a transition (default 0.001)
istart:
First occupied state to consider
jend:
Last unoccupied state to consider
xc:
Exchange-Correlation approximation in the Kernel
derivative_level:
0: use Exc, 1: use vxc, 2: use fxc if available
filename:
read from a file
"""
def __init__(self, calculator=None, **kwargs):
self.timer = Timer()
self.set(**kwargs)
if isinstance(calculator, str):
ExcitationList.__init__(self, None, self.txt)
self.filename = calculator
else:
ExcitationList.__init__(self, calculator, self.txt)
if self.filename is not None:
return self.read(self.filename)
if self.eh_comm is None:
self.eh_comm = mpi.serial_comm
elif isinstance(self.eh_comm, (mpi.world.__class__,
mpi.serial_comm.__class__)):
# Correct type already.
pass
else:
# world should be a list of ranks:
self.eh_comm = mpi.world.new_communicator(np.asarray(eh_comm))
if calculator is not None and calculator.initialized:
if not isinstance(calculator.wfs, FDWaveFunctions):
raise RuntimeError(
'Linear response TDDFT supported only in real space mode')
if calculator.wfs.kd.comm.size > 1:
err_txt = 'Spin parallelization with Linear response '
err_txt += "TDDFT. Use parallel = {'domain' : 'domain_only'} "
err_txt += 'calculator parameter.'
raise NotImplementedError(err_txt)
if self.xc == 'GS':
self.xc = calculator.hamiltonian.xc.name
if calculator.input_parameters.mode != 'lcao':
calculator.converge_wave_functions()
if calculator.density.nct_G is None:
spos_ac = calculator.initialize_positions()
calculator.wfs.initialize(calculator.density,
calculator.hamiltonian, spos_ac)
self.update(calculator)
def set(self, **kwargs):
defaults = {
'nspins': None,
'eps': 0.001,
'istart': 0,
'jend': sys.maxsize,
'energy_range': None,
'xc': 'GS',
'derivative_level': 1,
'numscale': 0.00001,
'txt': None,
'filename': None,
'finegrid': 2,
'force_ApmB': False, # for tests
'eh_comm': None # parallelization over eh-pairs
}
changed = False
for key, value in defaults.items():
if hasattr(self, key):
value = getattr(self, key) # do not overwrite
setattr(self, key, kwargs.pop(key, value))
if value != getattr(self, key):
changed = True
for key in kwargs:
raise KeyError('Unknown key ' + key)
return changed
def set_calculator(self, calculator):
self.calculator = calculator
# self.force_ApmB = parameters['force_ApmB']
self.force_ApmB = None # XXX
def analyse(self, what=None, out=None, min=0.1):
"""Print info about the transitions.
Parameters:
1. what: I list of excitation indicees, None means all
2. out : I where to send the output, None means sys.stdout
3. min : I minimal contribution to list (0<min<1)
"""
if what is None:
what = range(len(self))
elif isinstance(what, int):
what = [what]
if out is None:
out = sys.stdout
for i in what:
print(str(i) + ':', self[i].analyse(min=min), file=out)
def update(self, calculator=None, **kwargs):
changed = self.set(**kwargs)
if calculator is not None:
changed = True
self.set_calculator(calculator)
if not changed:
return
self.forced_update()
def forced_update(self):
"""Recalc yourself."""
if not self.force_ApmB:
Om = OmegaMatrix
name = 'LrTDDFT'
if self.xc:
xc = XC(self.xc)
if hasattr(xc, 'hybrid') and xc.hybrid > 0.0:
Om = ApmB
name = 'LrTDDFThyb'
else:
Om = ApmB
name = 'LrTDDFThyb'
self.kss = KSSingles(calculator=self.calculator,
nspins=self.nspins,
eps=self.eps,
istart=self.istart,
jend=self.jend,
energy_range=self.energy_range,
txt=self.txt)
self.Om = Om(self.calculator, self.kss,
self.xc, self.derivative_level, self.numscale,
finegrid=self.finegrid, eh_comm=self.eh_comm,
txt=self.txt)
self.name = name
def diagonalize(self, istart=None, jend=None,
energy_range=None, TDA=False):
self.timer.start('diagonalize')
self.timer.start('omega')
self.Om.diagonalize(istart, jend, energy_range, TDA)
self.timer.stop('omega')
# remove old stuff
self.timer.start('clean')
while len(self):
self.pop()
self.timer.stop('clean')
print('LrTDDFT digonalized:', file=self.txt)
self.timer.start('build')
for j in range(len(self.Om.kss)):
self.append(LrTDDFTExcitation(self.Om, j))
print(' ', str(self[-1]), file=self.txt)
self.timer.stop('build')
self.timer.stop('diagonalize')
def get_Om(self):
return self.Om
def read(self, filename=None, fh=None):
"""Read myself from a file"""
if fh is None:
if filename.endswith('.gz'):
try:
import gzip
f = gzip.open(filename)
except:
f = open(filename, 'r')
else:
f = open(filename, 'r')
self.filename = filename
else:
f = fh
self.filename = None
# get my name
s = f.readline().replace('\n', '')
self.name = s.split()[1]
self.xc = f.readline().replace('\n', '').split()[0]
values = f.readline().split()
self.eps = float(values[0])
if len(values) > 1:
self.derivative_level = int(values[1])
self.numscale = float(values[2])
self.finegrid = int(values[3])
else:
# old writing style, use old defaults
self.numscale = 0.001
self.kss = KSSingles(filehandle=f)
if self.name == 'LrTDDFT':
self.Om = OmegaMatrix(kss=self.kss, filehandle=f,
txt=self.txt)
else:
self.Om = ApmB(kss=self.kss, filehandle=f,
txt=self.txt)
self.Om.Kss(self.kss)
# check if already diagonalized
p = f.tell()
s = f.readline()
if s != '# Eigenvalues\n':
# go back to previous position
f.seek(p)
else:
# load the eigenvalues
n = int(f.readline().split()[0])
for i in range(n):
self.append(LrTDDFTExcitation(string=f.readline()))
# load the eigenvectors
f.readline()
for i in range(n):
values = f.readline().split()
weights = [float(val) for val in values]
self[i].f = np.array(weights)
self[i].kss = self.kss
if fh is None:
f.close()
# update own variables
self.istart = self.Om.fullkss.istart
self.jend = self.Om.fullkss.jend
def singlets_triplets(self):
"""Split yourself into a singlet and triplet object"""
slr = LrTDDFT(None, nspins=self.nspins, eps=self.eps,
istart=self.istart, jend=self.jend, xc=self.xc,
derivative_level=self.derivative_level,
numscale=self.numscale)
tlr = LrTDDFT(None, nspins=self.nspins, eps=self.eps,
istart=self.istart, jend=self.jend, xc=self.xc,
derivative_level=self.derivative_level,
numscale=self.numscale)
slr.Om, tlr.Om = self.Om.singlets_triplets()
for lr in [slr, tlr]:
lr.kss = lr.Om.fullkss
return slr, tlr
def single_pole_approximation(self, i, j):
"""Return the excitation according to the
single pole approximation. See e.g.:
Grabo et al, Theochem 501 (2000) 353-367
"""
for ij, kss in enumerate(self.kss):
if kss.i == i and kss.j == j:
return sqrt(self.Om.full[ij][ij]) * Hartree
return self.Om.full[ij][ij] / kss.energy * Hartree
def __str__(self):
string = ExcitationList.__str__(self)
string += '# derived from:\n'
string += self.Om.kss.__str__()
return string
def write(self, filename=None, fh=None):
"""Write current state to a file.
'filename' is the filename. If the filename ends in .gz,
the file is automatically saved in compressed gzip format.
'fh' is a filehandle. This can be used to write into already
opened files.
"""
if mpi.rank == mpi.MASTER:
if fh is None:
if filename.endswith('.gz'):
try:
import gzip
f = gzip.open(filename, 'wb')
except:
f = open(filename, 'w')
else:
f = open(filename, 'w')
else:
f = fh
f.write('# ' + self.name + '\n')
xc = self.xc
if xc is None:
xc = 'RPA'
if self.calculator is not None:
xc += ' ' + self.calculator.get_xc_functional()
f.write(xc + '\n')
f.write('%g %d %g %d' % (self.eps, int(self.derivative_level),
self.numscale, int(self.finegrid)) + '\n')
self.kss.write(fh=f)
self.Om.write(fh=f)
if len(self):
f.write('# Eigenvalues\n')
istart = self.istart
if istart is None:
istart = self.kss.istart
jend = self.jend
if jend is None:
jend = self.kss.jend
f.write('%d %d %d' % (len(self), istart, jend) + '\n')
for ex in self:
f.write(ex.outstring())
f.write('# Eigenvectors\n')
for ex in self:
for w in ex.f:
f.write('%g ' % w)
f.write('\n')
if fh is None:
f.close()
class ResonantRaman(Vibrations):
"""Class for calculating vibrational modes and
resonant Raman intensities using finite difference.
atoms:
Atoms object
Excitations:
Class to calculate the excitations. The class object is
initialized as::
Excitations(atoms.get_calculator())
or by reading form a file as::
Excitations('filename', **exkwargs)
The file is written by calling the method
Excitations.write('filename').
"""
def __init__(self, atoms, Excitations,
indices=None,
gsname='rraman', # name for ground state calculations
exname=None, # name for excited state calculations
delta=0.01,
nfree=2,
directions=None,
exkwargs={}, # kwargs to be passed to Excitations
txt='-'):
assert(nfree == 2)
Vibrations.__init__(self, atoms, indices, gsname, delta, nfree)
self.name = gsname + '-d%.3f' % delta
if exname is None:
exname = gsname
self.exname = exname + '-d%.3f' % delta
if directions is None:
self.directions = np.array([0, 1, 2])
else:
self.directions = np.array(directions)
self.exobj = Excitations
self.exkwargs = exkwargs
self.timer = Timer()
self.txt = get_txt(txt, rank)
def calculate(self, filename, fd):
"""Call ground and excited state calculation"""
self.timer.start('Ground state')
forces = self.atoms.get_forces()
if rank == 0:
pickle.dump(forces, fd)
fd.close()
self.timer.stop('Ground state')
self.timer.start('Excitations')
basename, _ = os.path.splitext(filename)
excitations = self.exobj(self.atoms.get_calculator())
excitations.write(basename + '.excitations')
self.timer.stop('Excitations')
def get_intensity_tensor(self, omega, gamma=0.1):
if not hasattr(self, 'modes'):
self.read()
if not hasattr(self, 'ex0'):
eu = units.Hartree
def get_me_tensor(exname, n, form='v'):
def outer(ex):
me = ex.get_dipole_me(form=form)
return np.outer(me, me.conj())
ex_p = self.exobj(exname, **self.exkwargs)
if len(ex_p) != n:
raise RuntimeError(
('excitations {0} of wrong length: {1} != {2}' +
' exkwargs={3}').format(
exname, len(ex_p), n, self.exkwargs))
m_ccp = np.empty((3, 3, len(ex_p)), dtype=complex)
for p, ex in enumerate(ex_p):
m_ccp[:, :, p] = outer(ex)
return m_ccp
self.timer.start('reading excitations')
ex_p = self.exobj(self.exname + '.eq.excitations',
**self.exkwargs)
n = len(ex_p)
self.ex0 = np.array([ex.energy * eu for ex in ex_p])
self.exminus = []
self.explus = []
for a in self.indices:
for i in 'xyz':
name = '%s.%d%s' % (self.exname, a, i)
self.exminus.append(get_me_tensor(
name + '-.excitations', n))
self.explus.append(get_me_tensor(
name + '+.excitations', n))
self.timer.stop('reading excitations')
self.timer.start('amplitudes')
self.timer.start('init')
ndof = 3 * len(self.indices)
amplitudes = np.zeros((ndof, 3, 3), dtype=complex)
pre = 1. / (2 * self.delta)
self.timer.stop('init')
def kappa(me_ccp, e_p, omega, gamma, form='v'):
"""Kappa tensor after Profeta and Mauri
PRB 63 (2001) 245415"""
result = (me_ccp / (e_p - omega - 1j * gamma) +
me_ccp.conj() / (e_p + omega + 1j * gamma))
return result.sum(2)
r = 0
for a in self.indices:
for i in 'xyz':
amplitudes[r] = pre * (
kappa(self.explus[r], self.ex0, omega, gamma) -
kappa(self.exminus[r], self.ex0, omega, gamma))
r += 1
self.timer.stop('amplitudes')
# map to modes
am = np.dot(amplitudes.T, self.modes.T).T
return omega**4 * (am * am.conj()).real
def get_intensities(self, omega, gamma=0.1):
return self.get_intensity_tensor(omega, gamma).sum(axis=1).sum(axis=1)
def get_spectrum(self, omega, gamma=0.1,
start=200, end=4000, npts=None, width=4,
type='Gaussian', method='standard', direction='central',
intensity_unit='????', normalize=False):
"""Get resonant Raman spectrum.
The method returns wavenumbers in cm^-1 with corresponding
absolute infrared intensity.
Start and end point, and width of the Gaussian/Lorentzian should
be given in cm^-1.
normalize=True ensures the integral over the peaks to give the
intensity.
"""
self.type = type.lower()
assert self.type in ['gaussian', 'lorentzian']
if not npts:
npts = (end - start) / width * 10 + 1
frequencies = self.get_frequencies(method, direction).real
intensities = self.get_intensities(omega, gamma)
prefactor = 1
if type == 'lorentzian':
intensities = intensities * width * np.pi / 2.
if normalize:
prefactor = 2. / width / np.pi
else:
sigma = width / 2. / np.sqrt(2. * np.log(2.))
if normalize:
prefactor = 1. / sigma / np.sqrt(2 * np.pi)
#Make array with spectrum data
spectrum = np.empty(npts, np.float)
energies = np.empty(npts, np.float)
ediff = (end - start) / float(npts - 1)
energies = np.arange(start, end + ediff / 2, ediff)
for i, energy in enumerate(energies):
energies[i] = energy
if type == 'lorentzian':
spectrum[i] = (intensities * 0.5 * width / np.pi / (
(frequencies - energy)**2 + 0.25 * width**2)).sum()
else:
spectrum[i] = (intensities *
np.exp(-(frequencies - energy)**2 /
2. / sigma**2)).sum()
return [energies, prefactor * spectrum]
def write_spectra(self, omega, gamma,
out='resonant-raman-spectra.dat',
start=200, end=4000,
npts=None, width=10,
type='Gaussian', method='standard',
direction='central'):
"""Write out spectrum to file.
First column is the wavenumber in cm^-1, the second column the
absolute infrared intensities, and
the third column the absorbance scaled so that data runs
from 1 to 0. Start and end
point, and width of the Gaussian/Lorentzian should be given
in cm^-1."""
energies, spectrum = self.get_spectrum(omega, gamma,
start, end, npts, width,
type, method, direction)
#Write out spectrum in file. First column is absolute intensities.
outdata = np.empty([len(energies), 3])
outdata.T[0] = energies
outdata.T[1] = spectrum
fd = open(out, 'w')
fd.write('# Resonat Raman spectrum\n')
fd.write('# omega={0:g} eV, gamma={1:g} eV\n'.format(omega, gamma))
fd.write('# %s folded, width=%g cm^-1\n' % (type.title(), width))
fd.write('# [cm^-1] [a.u.]\n')
for row in outdata:
fd.write('%.3f %15.5g\n' %
(row[0], row[1]))
fd.close()
def summary(self, omega, gamma=0.1,
method='standard', direction='central',
intensity_unit='(D/A)2/amu', log=sys.stdout):
"""Print summary for given omega [eV]"""
hnu = self.get_energies(method, direction)
s = 0.01 * units._e / units._c / units._hplanck
intensities = self.get_intensities(omega, gamma)
if isinstance(log, str):
log = paropen(log, 'a')
parprint('-------------------------------------', file=log)
parprint(' excitation at ' + str(omega) + ' eV', file=log)
parprint(' gamma ' + str(gamma) + ' eV\n', file=log)
parprint(' Mode Frequency Intensity', file=log)
parprint(' # meV cm^-1 [a.u.]', file=log)
parprint('-------------------------------------', file=log)
for n, e in enumerate(hnu):
if e.imag != 0:
c = 'i'
e = e.imag
else:
c = ' '
e = e.real
parprint('%3d %6.1f%s %7.1f%s %9.3g' %
(n, 1000 * e, c, s * e, c, intensities[n]),
file=log)
parprint('-------------------------------------', file=log)
parprint('Zero-point energy: %.3f eV' % self.get_zero_point_energy(),
file=log)
def __del__(self):
self.timer.write(self.txt)
def get_xc(self):
"""Add xc part of the coupling matrix"""
# shorthands
paw = self.paw
wfs = paw.wfs
gd = paw.density.finegd
comm = gd.comm
eh_comm = self.eh_comm
fg = self.finegrid is 2
kss = self.fullkss
nij = len(kss)
Om_xc = self.Om
# initialize densities
# nt_sg is the smooth density on the fine grid with spin index
if kss.nvspins == 2:
# spin polarised ground state calc.
nt_sg = paw.density.nt_sg
else:
# spin unpolarised ground state calc.
if kss.npspins == 2:
# construct spin polarised densities
nt_sg = np.array([.5 * paw.density.nt_sg[0],
.5 * paw.density.nt_sg[0]])
else:
nt_sg = paw.density.nt_sg
# check if D_sp have been changed before
D_asp = self.paw.density.D_asp
for a, D_sp in D_asp.items():
if len(D_sp) != kss.npspins:
if len(D_sp) == 1:
D_asp[a] = np.array([0.5 * D_sp[0], 0.5 * D_sp[0]])
else:
D_asp[a] = np.array([D_sp[0] + D_sp[1]])
# restrict the density if needed
if fg:
nt_s = nt_sg
else:
nt_s = self.gd.zeros(nt_sg.shape[0])
for s in range(nt_sg.shape[0]):
self.restrict(nt_sg[s], nt_s[s])
gd = paw.density.gd
# initialize vxc or fxc
if self.derivativeLevel == 0:
raise NotImplementedError
if kss.npspins == 2:
v_g = nt_sg[0].copy()
else:
v_g = nt_sg.copy()
elif self.derivativeLevel == 1:
pass
elif self.derivativeLevel == 2:
fxc_sg = np.zeros(nt_sg.shape)
self.xc.calculate_fxc(gd, nt_sg, fxc_sg)
else:
raise ValueError('derivativeLevel can only be 0,1,2')
# self.paw.my_nuclei = []
ns = self.numscale
xc = self.xc
print('XC', nij, 'transitions', file=self.txt)
for ij in range(eh_comm.rank, nij, eh_comm.size):
print('XC kss[' + '%d' % ij + ']', file=self.txt)
timer = Timer()
timer.start('init')
timer2 = Timer()
if self.derivativeLevel >= 1:
# vxc is available
# We use the numerical two point formula for calculating
# the integral over fxc*n_ij. The results are
# vvt_s smooth integral
# nucleus.I_sp atom based correction matrices (pack2)
# stored on each nucleus
timer2.start('init v grids')
vp_s = np.zeros(nt_s.shape, nt_s.dtype.char)
vm_s = np.zeros(nt_s.shape, nt_s.dtype.char)
if kss.npspins == 2: # spin polarised
nv_s = nt_s.copy()
nv_s[kss[ij].pspin] += ns * kss[ij].get(fg)
xc.calculate(gd, nv_s, vp_s)
nv_s = nt_s.copy()
nv_s[kss[ij].pspin] -= ns * kss[ij].get(fg)
xc.calculate(gd, nv_s, vm_s)
else: # spin unpolarised
nv = nt_s + ns * kss[ij].get(fg)
xc.calculate(gd, nv, vp_s)
nv = nt_s - ns * kss[ij].get(fg)
xc.calculate(gd, nv, vm_s)
vvt_s = (0.5 / ns) * (vp_s - vm_s)
timer2.stop()
# initialize the correction matrices
timer2.start('init v corrections')
I_asp = {}
for a, P_ni in wfs.kpt_u[kss[ij].spin].P_ani.items():
# create the modified density matrix
Pi_i = P_ni[kss[ij].i]
Pj_i = P_ni[kss[ij].j]
P_ii = np.outer(Pi_i, Pj_i)
# we need the symmetric form, hence we can pack
P_p = pack(P_ii)
D_sp = self.paw.density.D_asp[a].copy()
D_sp[kss[ij].pspin] -= ns * P_p
setup = wfs.setups[a]
I_sp = np.zeros_like(D_sp)
self.xc.calculate_paw_correction(setup, D_sp, I_sp)
I_sp *= -1.0
D_sp = self.paw.density.D_asp[a].copy()
D_sp[kss[ij].pspin] += ns * P_p
self.xc.calculate_paw_correction(setup, D_sp, I_sp)
I_sp /= 2.0 * ns
I_asp[a] = I_sp
timer2.stop()
timer.stop()
t0 = timer.get_time('init')
timer.start(ij)
for kq in range(ij, nij):
weight = self.weight_Kijkq(ij, kq)
if self.derivativeLevel == 0:
# only Exc is available
if kss.npspins == 2: # spin polarised
nv_g = nt_sg.copy()
nv_g[kss[ij].pspin] += kss[ij].get(fg)
nv_g[kss[kq].pspin] += kss[kq].get(fg)
Excpp = xc.get_energy_and_potential(
nv_g[0], v_g, nv_g[1], v_g)
nv_g = nt_sg.copy()
nv_g[kss[ij].pspin] += kss[ij].get(fg)
nv_g[kss[kq].pspin] -= kss[kq].get(fg)
Excpm = xc.get_energy_and_potential(
nv_g[0], v_g, nv_g[1], v_g)
nv_g = nt_sg.copy()
nv_g[kss[ij].pspin] -=\
kss[ij].get(fg)
nv_g[kss[kq].pspin] +=\
kss[kq].get(fg)
Excmp = xc.get_energy_and_potential(
nv_g[0], v_g, nv_g[1], v_g)
nv_g = nt_sg.copy()
nv_g[kss[ij].pspin] -= \
kss[ij].get(fg)
nv_g[kss[kq].pspin] -=\
kss[kq].get(fg)
Excpp = xc.get_energy_and_potential(
nv_g[0], v_g, nv_g[1], v_g)
else: # spin unpolarised
nv_g = nt_sg + ns * kss[ij].get(fg)\
+ ns * kss[kq].get(fg)
Excpp = xc.get_energy_and_potential(nv_g, v_g)
nv_g = nt_sg + ns * kss[ij].get(fg)\
- ns * kss[kq].get(fg)
Excpm = xc.get_energy_and_potential(nv_g, v_g)
nv_g = nt_sg - ns * kss[ij].get(fg)\
+ ns * kss[kq].get(fg)
Excmp = xc.get_energy_and_potential(nv_g, v_g)
nv_g = nt_sg - ns * kss[ij].get(fg)\
- ns * kss[kq].get(fg)
Excmm = xc.get_energy_and_potential(nv_g, v_g)
Om_xc[ij, kq] += weight *\
0.25 * \
(Excpp - Excmp - Excpm + Excmm) / (ns * ns)
elif self.derivativeLevel == 1:
# vxc is available
timer2.start('integrate')
Om_xc[ij, kq] += weight *\
self.gd.integrate(kss[kq].get(fg) *
vvt_s[kss[kq].pspin])
timer2.stop()
timer2.start('integrate corrections')
Exc = 0.
for a, P_ni in wfs.kpt_u[kss[kq].spin].P_ani.items():
# create the modified density matrix
Pk_i = P_ni[kss[kq].i]
Pq_i = P_ni[kss[kq].j]
P_ii = np.outer(Pk_i, Pq_i)
# we need the symmetric form, hence we can pack
# use pack as I_sp used pack2
P_p = pack(P_ii)
Exc += np.dot(I_asp[a][kss[kq].pspin], P_p)
Om_xc[ij, kq] += weight * self.gd.comm.sum(Exc)
timer2.stop()
elif self.derivativeLevel == 2:
# fxc is available
if kss.npspins == 2: # spin polarised
Om_xc[ij, kq] += weight *\
gd.integrate(kss[ij].get(fg) *
kss[kq].get(fg) *
fxc_sg[kss[ij].pspin, kss[kq].pspin])
else: # spin unpolarised
Om_xc[ij, kq] += weight *\
gd.integrate(kss[ij].get(fg) *
kss[kq].get(fg) *
fxc_sg)
# XXX still numeric derivatives for local terms
timer2.start('integrate corrections')
Exc = 0.
for a, P_ni in wfs.kpt_u[kss[kq].spin].P_ani.items():
# create the modified density matrix
Pk_i = P_ni[kss[kq].i]
Pq_i = P_ni[kss[kq].j]
P_ii = np.outer(Pk_i, Pq_i)
# we need the symmetric form, hence we can pack
# use pack as I_sp used pack2
P_p = pack(P_ii)
Exc += np.dot(I_asp[a][kss[kq].pspin], P_p)
Om_xc[ij, kq] += weight * self.gd.comm.sum(Exc)
timer2.stop()
if ij != kq:
Om_xc[kq, ij] = Om_xc[ij, kq]
timer.stop()
# timer2.write()
if ij < (nij - 1):
print('XC estimated time left',
self.time_left(timer, t0, ij, nij), file=self.txt)
class RPACorrelation:
def __init__(self, calc, xc='RPA', filename=None,
skip_gamma=False, qsym=True, nlambda=None,
nfrequencies=16, frequency_max=800.0, frequency_scale=2.0,
frequencies=None, weights=None,
world=mpi.world, nblocks=1, wstc=False,
txt=sys.stdout):
if isinstance(calc, str):
calc = GPAW(calc, txt=None, communicator=mpi.serial_comm)
self.calc = calc
if world.rank != 0:
txt = devnull
elif isinstance(txt, str):
txt = open(txt, 'w')
self.fd = txt
self.timer = Timer()
if frequencies is None:
frequencies, weights = get_gauss_legendre_points(nfrequencies,
frequency_max,
frequency_scale)
user_spec = False
else:
assert weights is not None
user_spec = True
self.omega_w = frequencies / Hartree
self.weight_w = weights / Hartree
if nblocks > 1:
assert len(self.omega_w) % nblocks == 0
assert wstc
self.wstc = wstc
self.nblocks = nblocks
self.world = world
self.skip_gamma = skip_gamma
self.ibzq_qc = None
self.weight_q = None
self.initialize_q_points(qsym)
# Energies for all q-vetors and cutoff energies:
self.energy_qi = []
self.filename = filename
self.print_initialization(xc, frequency_scale, nlambda, user_spec)
def initialize_q_points(self, qsym):
kd = self.calc.wfs.kd
self.bzq_qc = kd.get_bz_q_points(first=True)
if not qsym:
self.ibzq_qc = self.bzq_qc
self.weight_q = np.ones(len(self.bzq_qc)) / len(self.bzq_qc)
else:
U_scc = kd.symmetry.op_scc
self.ibzq_qc = kd.get_ibz_q_points(self.bzq_qc, U_scc)[0]
self.weight_q = kd.q_weights
def read(self):
lines = open(self.filename).readlines()[1:]
n = 0
self.energy_qi = []
nq = len(lines) // len(self.ecut_i)
for q_c in self.ibzq_qc[:nq]:
self.energy_qi.append([])
for ecut in self.ecut_i:
q1, q2, q3, ec, energy = [float(x)
for x in lines[n].split()]
self.energy_qi[-1].append(energy / Hartree)
n += 1
if (abs(q_c - (q1, q2, q3)).max() > 1e-4 or
abs(int(ecut * Hartree) - ec) > 0):
self.energy_qi = []
return
print('Read %d q-points from file: %s' % (nq, self.filename),
file=self.fd)
print(file=self.fd)
def write(self):
if self.world.rank == 0 and self.filename:
fd = open(self.filename, 'w')
print('#%9s %10s %10s %8s %12s' %
('q1', 'q2', 'q3', 'E_cut', 'E_c(q)'), file=fd)
for energy_i, q_c in zip(self.energy_qi, self.ibzq_qc):
for energy, ecut in zip(energy_i, self.ecut_i):
print('%10.4f %10.4f %10.4f %8d %r' %
(tuple(q_c) + (ecut * Hartree, energy * Hartree)),
file=fd)
def calculate(self, ecut, nbands=None, spin=False):
"""Calculate RPA correlation energy for one or several cutoffs.
ecut: float or list of floats
Plane-wave cutoff(s).
nbands: int
Number of bands (defaults to number of plane-waves).
spin: bool
Separate spin in response funtion.
(Only needed for beyond RPA methods that inherit this function).
"""
p = functools.partial(print, file=self.fd)
if isinstance(ecut, (float, int)):
ecut = ecut * (1 + 0.5 * np.arange(6))**(-2 / 3)
self.ecut_i = np.asarray(np.sort(ecut)) / Hartree
ecutmax = max(self.ecut_i)
if nbands is None:
p('Response function bands : Equal to number of plane waves')
else:
p('Response function bands : %s' % nbands)
p('Plane wave cutoffs (eV) :', end='')
for e in self.ecut_i:
p(' {0:.3f}'.format(e * Hartree), end='')
p()
p()
if self.filename and os.path.isfile(self.filename):
self.read()
self.world.barrier()
chi0 = Chi0(self.calc, 1j * Hartree * self.omega_w, eta=0.0,
intraband=False, hilbert=False,
txt=self.fd, timer=self.timer, world=self.world,
no_optical_limit=self.wstc,
nblocks=self.nblocks)
self.blockcomm = chi0.blockcomm
wfs = self.calc.wfs
if self.wstc:
with self.timer('WSTC-init'):
p('Using Wigner-Seitz truncated Coulomb potential.')
self.wstc = WignerSeitzTruncatedCoulomb(
wfs.gd.cell_cv, wfs.kd.N_c, self.fd)
nq = len(self.energy_qi)
nw = len(self.omega_w)
nGmax = max(count_reciprocal_vectors(ecutmax, wfs.gd, q_c)
for q_c in self.ibzq_qc[nq:])
mynGmax = (nGmax + self.nblocks - 1) // self.nblocks
nx = (1 + spin) * nw * mynGmax * nGmax
A1_x = np.empty(nx, complex)
if self.nblocks > 1:
A2_x = np.empty(nx, complex)
else:
A2_x = None
self.timer.start('RPA')
for q_c in self.ibzq_qc[nq:]:
if np.allclose(q_c, 0.0) and self.skip_gamma:
self.energy_qi.append(len(self.ecut_i) * [0.0])
self.write()
p('Not calculating E_c(q) at Gamma')
p()
continue
thisqd = KPointDescriptor([q_c])
pd = PWDescriptor(ecutmax, wfs.gd, complex, thisqd)
nG = pd.ngmax
mynG = (nG + self.nblocks - 1) // self.nblocks
chi0.Ga = self.blockcomm.rank * mynG
chi0.Gb = min(chi0.Ga + mynG, nG)
shape = (1 + spin, nw, chi0.Gb - chi0.Ga, nG)
chi0_swGG = A1_x[:np.prod(shape)].reshape(shape)
chi0_swGG[:] = 0.0
if self.wstc or np.allclose(q_c, 0.0):
# Wings (x=0,1) and head (G=0) for optical limit and three
# directions (v=0,1,2):
chi0_swxvG = np.zeros((1 + spin, nw, 2, 3, nG), complex)
chi0_swvv = np.zeros((1 + spin, nw, 3, 3), complex)
else:
chi0_swxvG = None
chi0_swvv = None
Q_aGii = chi0.initialize_paw_corrections(pd)
# First not completely filled band:
m1 = chi0.nocc1
p('# %s - %s' % (len(self.energy_qi), ctime().split()[-2]))
p('q = [%1.3f %1.3f %1.3f]' % tuple(q_c))
energy_i = []
for ecut in self.ecut_i:
if ecut == ecutmax:
# Nothing to cut away:
cut_G = None
m2 = nbands or nG
else:
cut_G = np.arange(nG)[pd.G2_qG[0] <= 2 * ecut]
m2 = len(cut_G)
p('E_cut = %d eV / Bands = %d:' % (ecut * Hartree, m2))
self.fd.flush()
energy = self.calculate_q(chi0, pd,
chi0_swGG, chi0_swxvG, chi0_swvv,
Q_aGii, m1, m2, cut_G, A2_x)
energy_i.append(energy)
m1 = m2
a = 1 / chi0.kncomm.size
if ecut < ecutmax and a != 1.0:
# Chi0 will be summed again over chicomm, so we divide
# by its size:
chi0_swGG *= a
if chi0_swxvG is not None:
chi0_swxvG *= a
chi0_swvv *= a
self.energy_qi.append(energy_i)
self.write()
p()
e_i = np.dot(self.weight_q, np.array(self.energy_qi))
p('==========================================================')
p()
p('Total correlation energy:')
for e_cut, e in zip(self.ecut_i, e_i):
p('%6.0f: %6.4f eV' % (e_cut * Hartree, e * Hartree))
p()
self.energy_qi = [] # important if another calculation is performed
if len(e_i) > 1:
self.extrapolate(e_i)
p('Calculation completed at: ', ctime())
p()
self.timer.stop('RPA')
self.timer.write(self.fd)
self.fd.flush()
return e_i * Hartree
@timer('chi0(q)')
def calculate_q(self, chi0, pd,
chi0_swGG, chi0_swxvG, chi0_swvv, Q_aGii, m1, m2, cut_G,
A2_x):
chi0_wGG = chi0_swGG[0]
if chi0_swxvG is not None:
chi0_wxvG = chi0_swxvG[0]
chi0_wvv = chi0_swvv[0]
else:
chi0_wxvG = None
chi0_wvv = None
chi0._calculate(pd, chi0_wGG, chi0_wxvG, chi0_wvv,
Q_aGii, m1, m2, [0, 1])
print('E_c(q) = ', end='', file=self.fd)
chi0_wGG = chi0.redistribute(chi0_wGG, A2_x)
if not pd.kd.gamma or self.wstc:
e = self.calculate_energy(pd, chi0_wGG, cut_G)
print('%.3f eV' % (e * Hartree), file=self.fd)
self.fd.flush()
else:
e = 0.0
for v in range(3):
chi0_wGG[:, 0] = chi0_wxvG[:, 0, v]
chi0_wGG[:, :, 0] = chi0_wxvG[:, 1, v]
chi0_wGG[:, 0, 0] = chi0_wvv[:, v, v]
ev = self.calculate_energy(pd, chi0_wGG, cut_G)
e += ev
print('%.3f' % (ev * Hartree), end='', file=self.fd)
if v < 2:
print('/', end='', file=self.fd)
else:
print(' eV', file=self.fd)
self.fd.flush()
e /= 3
return e
@timer('Energy')
def calculate_energy(self, pd, chi0_wGG, cut_G):
"""Evaluate correlation energy from chi0."""
if self.wstc:
invG_G = (self.wstc.get_potential(pd) / (4 * pi))**0.5
else:
G_G = pd.G2_qG[0]**0.5 # |G+q|
if pd.kd.gamma:
G_G[0] = 1.0
invG_G = 1.0 / G_G
if cut_G is not None:
invG_G = invG_G[cut_G]
nG = len(invG_G)
e_w = []
for chi0_GG in chi0_wGG:
if cut_G is not None:
chi0_GG = chi0_GG.take(cut_G, 0).take(cut_G, 1)
e_GG = (np.eye(nG) -
4 * np.pi * chi0_GG * invG_G * invG_G[:, np.newaxis])
e = np.log(np.linalg.det(e_GG)) + nG - np.trace(e_GG)
e_w.append(e.real)
E_w = np.zeros_like(self.omega_w)
self.blockcomm.all_gather(np.array(e_w), E_w)
energy = np.dot(E_w, self.weight_w) / (2 * np.pi)
self.E_w = E_w
return energy
def extrapolate(self, e_i):
print('Extrapolated energies:', file=self.fd)
ex_i = []
for i in range(len(e_i) - 1):
e1, e2 = e_i[i:i + 2]
x1, x2 = self.ecut_i[i:i + 2]**-1.5
ex = (e1 * x2 - e2 * x1) / (x2 - x1)
ex_i.append(ex)
print(' %4.0f -%4.0f: %5.3f eV' % (self.ecut_i[i] * Hartree,
self.ecut_i[i + 1] * Hartree,
ex * Hartree),
file=self.fd)
print(file=self.fd)
self.fd.flush()
return e_i * Hartree
def print_initialization(self, xc, frequency_scale, nlambda, user_spec):
p = functools.partial(print, file=self.fd)
p('----------------------------------------------------------')
p('Non-self-consistent %s correlation energy' % xc)
p('----------------------------------------------------------')
p('Started at: ', ctime())
p()
p('Atoms :',
self.calc.atoms.get_chemical_formula(mode='hill'))
p('Ground state XC functional :', self.calc.hamiltonian.xc.name)
p('Valence electrons :', self.calc.wfs.setups.nvalence)
p('Number of bands :', self.calc.wfs.bd.nbands)
p('Number of spins :', self.calc.wfs.nspins)
p('Number of k-points :', len(self.calc.wfs.kd.bzk_kc))
p('Number of irreducible k-points :', len(self.calc.wfs.kd.ibzk_kc))
p('Number of q-points :', len(self.bzq_qc))
p('Number of irreducible q-points :', len(self.ibzq_qc))
p()
for q, weight in zip(self.ibzq_qc, self.weight_q):
p(' q: [%1.4f %1.4f %1.4f] - weight: %1.3f' %
(q[0], q[1], q[2], weight))
p()
p('----------------------------------------------------------')
p('----------------------------------------------------------')
p()
if nlambda is None:
p('Analytical coupling constant integration')
else:
p('Numerical coupling constant integration using', nlambda,
'Gauss-Legendre points')
p()
p('Frequencies')
if not user_spec:
p(' Gauss-Legendre integration with %s frequency points' %
len(self.omega_w))
p(' Transformed from [0,oo] to [0,1] using e^[-aw^(1/B)]')
p(' Highest frequency point at %5.1f eV and B=%1.1f' %
(self.omega_w[-1] * Hartree, frequency_scale))
else:
p(' User specified frequency integration with',
len(self.omega_w), 'frequency points')
p()
p('Parallelization')
p(' Total number of CPUs : % s' % self.world.size)
p(' G-vector decomposition : % s' % self.nblocks)
p(' K-point/band decomposition : % s' %
(self.world.size // self.nblocks))
p()
def get_rpa(self):
"""calculate RPA part of the omega matrix"""
# shorthands
kss = self.fullkss
finegrid = self.finegrid
wfs = self.paw.wfs
eh_comm = self.eh_comm
# calculate omega matrix
nij = len(kss)
print('RPA', nij, 'transitions', file=self.txt)
Om = self.Om
for ij in range(eh_comm.rank, nij, eh_comm.size):
print('RPA kss[' + '%d' % ij + ']=', kss[ij], file=self.txt)
timer = Timer()
timer.start('init')
timer2 = Timer()
# smooth density including compensation charges
timer2.start('with_compensation_charges 0')
rhot_p = kss[ij].with_compensation_charges(
finegrid is not 0)
timer2.stop()
# integrate with 1/|r_1-r_2|
timer2.start('poisson')
phit_p = np.zeros(rhot_p.shape, rhot_p.dtype.char)
self.poisson.solve(phit_p, rhot_p, charge=None)
timer2.stop()
timer.stop()
t0 = timer.get_time('init')
timer.start(ij)
if finegrid == 1:
rhot = kss[ij].with_compensation_charges()
phit = self.gd.zeros()
# print "shapes 0=",phit.shape,rhot.shape
self.restrict(phit_p, phit)
else:
phit = phit_p
rhot = rhot_p
for kq in range(ij, nij):
if kq != ij:
# smooth density including compensation charges
timer2.start('kq with_compensation_charges')
rhot = kss[kq].with_compensation_charges(
finegrid is 2)
timer2.stop()
pre = 2 * sqrt(kss[ij].get_energy() * kss[kq].get_energy() *
kss[ij].get_weight() * kss[kq].get_weight())
I = self.Coulomb_integral_kss(kss[ij], kss[kq],
rhot, phit, timer2)
Om[ij, kq] = pre * I
if ij == kq:
Om[ij, kq] += kss[ij].get_energy() ** 2
else:
Om[kq, ij] = Om[ij, kq]
timer.stop()
# timer2.write()
if ij < (nij - 1):
t = timer.get_time(ij) # time for nij-ij calculations
t = .5 * t * \
(nij - ij) # estimated time for n*(n+1)/2, n=nij-(ij+1)
print('RPA estimated time left',
self.timestring(t0 * (nij - ij - 1) + t), file=self.txt)
def get_rpa(self):
"""Calculate RPA and Hartree-fock part of the A+-B matrices."""
# shorthands
kss = self.fullkss
finegrid = self.finegrid
yukawa = hasattr(self.xc, 'rsf') and (self.xc.rsf == 'Yukawa')
# calculate omega matrix
nij = len(kss)
print('RPAhyb', nij, 'transitions', file=self.txt)
AmB = np.zeros((nij, nij))
ApB = self.ApB
# storage place for Coulomb integrals
integrals = {}
if yukawa:
rsf_integrals = {}
# setup things for IVOs
if self.xc.excitation is not None or self.xc.excited != 0:
sin_tri_weight = 1
if self.xc.excitation is not None:
ex_type = self.xc.excitation.lower()
if ex_type == 'singlet':
sin_tri_weight = 2
elif ex_type == 'triplet':
sin_tri_weight = 0
h**o = int(self.paw.get_number_of_electrons() // 2)
ivo_l = h**o - self.xc.excited - 1
else:
ivo_l = None
for ij in range(nij):
print('RPAhyb kss[' + '%d' % ij + ']=', kss[ij], file=self.txt)
timer = Timer()
timer.start('init')
timer2 = Timer()
# smooth density including compensation charges
timer2.start('with_compensation_charges 0')
rhot_p = kss[ij].with_compensation_charges(finegrid != 0)
timer2.stop()
# integrate with 1/|r_1-r_2|
timer2.start('poisson')
phit_p = np.zeros(rhot_p.shape, rhot_p.dtype)
self.poisson.solve(phit_p, rhot_p, charge=None)
timer2.stop()
timer.stop()
t0 = timer.get_time('init')
timer.start(ij)
if finegrid == 1:
rhot = kss[ij].with_compensation_charges()
phit = self.gd.zeros()
self.restrict(phit_p, phit)
else:
phit = phit_p
rhot = rhot_p
for kq in range(ij, nij):
if kq != ij:
# smooth density including compensation charges
timer2.start('kq with_compensation_charges')
rhot = kss[kq].with_compensation_charges(finegrid == 2)
timer2.stop()
pre = self.weight_Kijkq(ij, kq)
timer2.start('integrate')
I = self.Coulomb_integral_kss(kss[ij], kss[kq], phit, rhot)
if kss[ij].spin == kss[kq].spin:
name = self.Coulomb_integral_name(kss[ij].i, kss[ij].j,
kss[kq].i, kss[kq].j,
kss[ij].spin)
integrals[name] = I
ApB[ij, kq] = pre * I
timer2.stop()
if ij == kq:
epsij = kss[ij].get_energy() / kss[ij].get_weight()
AmB[ij, kq] += epsij
ApB[ij, kq] += epsij
timer.stop()
# timer2.write()
if ij < (nij - 1):
print('RPAhyb estimated time left',
self.time_left(timer, t0, ij, nij),
file=self.txt)
# add HF parts and apply symmetry
if hasattr(self.xc, 'hybrid'):
weight = self.xc.hybrid
else:
weight = 0.0
for ij in range(nij):
print('HF kss[' + '%d' % ij + ']', file=self.txt)
timer = Timer()
timer.start('init')
timer.stop()
t0 = timer.get_time('init')
timer.start(ij)
i = kss[ij].i
j = kss[ij].j
s = kss[ij].spin
for kq in range(ij, nij):
if kss[ij].pspin == kss[kq].pspin:
k = kss[kq].i
q = kss[kq].j
ikjq = self.Coulomb_integral_ijkq(i, k, j, q, s, integrals)
iqkj = self.Coulomb_integral_ijkq(i, q, k, j, s, integrals)
if yukawa: # Yukawa integrals might be caches
ikjq -= self.Coulomb_integral_ijkq(
i, k, j, q, s, rsf_integrals, yukawa)
iqkj -= self.Coulomb_integral_ijkq(
i, q, k, j, s, rsf_integrals, yukawa)
ApB[ij, kq] -= weight * (ikjq + iqkj)
AmB[ij, kq] -= weight * (ikjq - iqkj)
ApB[kq, ij] = ApB[ij, kq]
AmB[kq, ij] = AmB[ij, kq]
timer.stop()
if ij < (nij - 1):
print('HF estimated time left',
self.time_left(timer, t0, ij, nij),
file=self.txt)
if ivo_l is not None:
# IVO RPA after Berman, Kaldor, Chem. Phys. 43 (3) 1979
# doi: 10.1016/0301-0104(79)85205-2
l = ivo_l
for ij in range(nij):
i = kss[ij].i
j = kss[ij].j
s = kss[ij].spin
for kq in range(ij, nij):
if kss[kq].i == i and kss[ij].pspin == kss[kq].pspin:
k = kss[kq].i
q = kss[kq].j
jqll = self.Coulomb_integral_ijkq(
j, q, l, l, s, integrals)
jllq = self.Coulomb_integral_ijkq(
j, l, l, q, s, integrals)
if yukawa:
jqll -= self.Coulomb_integral_ijkq(
j, q, l, l, s, rsf_integrals, yukawa)
jllq -= self.Coulomb_integral_ijkq(
j, l, l, q, s, rsf_integrals, yukawa)
jllq *= sin_tri_weight
ApB[ij, kq] += weight * (jqll - jllq)
AmB[ij, kq] += weight * (jqll - jllq)
ApB[kq, ij] = ApB[ij, kq]
AmB[kq, ij] = AmB[ij, kq]
return AmB
class PAW(PAWTextOutput):
"""This is the main calculation object for doing a PAW calculation."""
def __init__(self, filename=None, timer=None,
read_projections=True, **kwargs):
"""ASE-calculator interface.
The following parameters can be used: nbands, xc, kpts,
spinpol, gpts, h, charge, symmetry, width, mixer,
hund, lmax, fixdensity, convergence, txt, parallel,
communicator, dtype, softgauss and stencils.
If you don't specify any parameters, you will get:
Defaults: neutrally charged, LDA, gamma-point calculation, a
reasonable grid-spacing, zero Kelvin electronic temperature,
and the number of bands will be equal to the number of atomic
orbitals present in the setups. Only occupied bands are used
in the convergence decision. The calculation will be
spin-polarized if and only if one or more of the atoms have
non-zero magnetic moments. Text output will be written to
standard output.
For a non-gamma point calculation, the electronic temperature
will be 0.1 eV (energies are extrapolated to zero Kelvin) and
all symmetries will be used to reduce the number of
**k**-points."""
PAWTextOutput.__init__(self)
self.grid_descriptor_class = GridDescriptor
self.input_parameters = InputParameters()
if timer is None:
self.timer = Timer()
else:
self.timer = timer
self.scf = None
self.forces = ForceCalculator(self.timer)
self.stress_vv = None
self.dipole_v = None
self.magmom_av = None
self.wfs = EmptyWaveFunctions()
self.occupations = None
self.density = None
self.hamiltonian = None
self.atoms = None
self.iter = 0
self.initialized = False
self.nbands_parallelization_adjustment = None # Somehow avoid this?
# Possibly read GPAW keyword arguments from file:
if filename is not None and filename.endswith('.gkw'):
from gpaw.utilities.kwargs import load
parameters = load(filename)
parameters.update(kwargs)
kwargs = parameters
filename = None # XXX
if filename is not None:
comm = kwargs.get('communicator', mpi.world)
reader = gpaw.io.open(filename, 'r', comm)
self.atoms = gpaw.io.read_atoms(reader)
par = self.input_parameters
par.read(reader)
# _changed_keywords contains those keywords that have been
# changed by set() since last time initialize() was called.
self._changed_keywords = set()
self.set(**kwargs)
# Here in the beginning, effectively every keyword has been changed.
self._changed_keywords.update(self.input_parameters)
if filename is not None:
# Setups are not saved in the file if the setups were not loaded
# *from* files in the first place
if par.setups is None:
if par.idiotproof:
raise RuntimeError('Setups not specified in file. Use '
'idiotproof=False to proceed anyway.')
else:
par.setups = {None: 'paw'}
if par.basis is None:
if par.idiotproof:
raise RuntimeError('Basis not specified in file. Use '
'idiotproof=False to proceed anyway.')
else:
par.basis = {}
self.initialize()
self.read(reader, read_projections)
if self.hamiltonian.xc.type == 'GLLB':
self.occupations.calculate(self.wfs)
self.print_cell_and_parameters()
self.observers = []
def read(self, reader, read_projections=True):
gpaw.io.read(self, reader, read_projections)
def set(self, **kwargs):
"""Change parameters for calculator.
Examples::
calc.set(xc='PBE')
calc.set(nbands=20, kpts=(4, 1, 1))
"""
p = self.input_parameters
self._changed_keywords.update(kwargs)
if (kwargs.get('h') is not None) and (kwargs.get('gpts') is not None):
raise TypeError("""You can't use both "gpts" and "h"!""")
if 'h' in kwargs:
p['gpts'] = None
if 'gpts' in kwargs:
p['h'] = None
# Special treatment for dictionary parameters:
for name in ['convergence', 'parallel']:
if kwargs.get(name) is not None:
tmp = p[name]
for key in kwargs[name]:
if key not in tmp:
raise KeyError('Unknown subparameter "%s" in '
'dictionary parameter "%s"' % (key,
name))
tmp.update(kwargs[name])
kwargs[name] = tmp
self.initialized = False
for key in kwargs:
if key == 'basis' and str(p['mode']) == 'fd': # umm what about PW?
# The second criterion seems buggy, will not touch it. -Ask
continue
if key == 'eigensolver':
self.wfs.set_eigensolver(None)
if key in ['fixmom', 'mixer',
'verbose', 'txt', 'hund', 'random',
'eigensolver', 'idiotproof', 'notify']:
continue
if key in ['convergence', 'fixdensity', 'maxiter']:
self.scf = None
continue
# More drastic changes:
self.scf = None
self.wfs.set_orthonormalized(False)
if key in ['lmax', 'width', 'stencils', 'external', 'xc',
'poissonsolver']:
self.hamiltonian = None
self.occupations = None
elif key in ['occupations']:
self.occupations = None
elif key in ['charge']:
self.hamiltonian = None
self.density = None
self.wfs = EmptyWaveFunctions()
self.occupations = None
elif key in ['kpts', 'nbands', 'usesymm', 'symmetry']:
self.wfs = EmptyWaveFunctions()
self.occupations = None
elif key in ['h', 'gpts', 'setups', 'spinpol', 'realspace',
'parallel', 'communicator', 'dtype', 'mode']:
self.density = None
self.occupations = None
self.hamiltonian = None
self.wfs = EmptyWaveFunctions()
elif key in ['basis']:
self.wfs = EmptyWaveFunctions()
elif key in ['parsize', 'parsize_bands', 'parstride_bands']:
name = {'parsize': 'domain',
'parsize_bands': 'band',
'parstride_bands': 'stridebands'}[key]
raise DeprecationWarning(
'Keyword argument has been moved ' +
"to the 'parallel' dictionary keyword under '%s'." % name)
else:
raise TypeError("Unknown keyword argument: '%s'" % key)
p.update(kwargs)
def calculate(self, atoms=None, converge=False,
force_call_to_set_positions=False):
"""Update PAW calculaton if needed.
Returns True/False whether a calculation was performed or not."""
self.timer.start('Initialization')
if atoms is None:
atoms = self.atoms
if self.atoms is None:
# First time:
self.initialize(atoms)
self.set_positions(atoms)
elif (len(atoms) != len(self.atoms) or
(atoms.get_atomic_numbers() !=
self.atoms.get_atomic_numbers()).any() or
(atoms.get_initial_magnetic_moments() !=
self.atoms.get_initial_magnetic_moments()).any() or
(atoms.get_cell() != self.atoms.get_cell()).any() or
(atoms.get_pbc() != self.atoms.get_pbc()).any()):
# Drastic changes:
self.wfs = EmptyWaveFunctions()
self.occupations = None
self.density = None
self.hamiltonian = None
self.scf = None
self.initialize(atoms)
self.set_positions(atoms)
elif not self.initialized:
self.initialize(atoms)
self.set_positions(atoms)
elif (atoms.get_positions() != self.atoms.get_positions()).any():
self.density.reset()
self.set_positions(atoms)
elif not self.scf.converged:
# Do not call scf.check_convergence() here as it overwrites
# scf.converged, and setting scf.converged is the only
# 'practical' way for a user to force the calculation to proceed
self.set_positions(atoms)
elif force_call_to_set_positions:
self.set_positions(atoms)
self.timer.stop('Initialization')
if self.scf.converged:
return False
else:
self.print_cell_and_parameters()
self.timer.start('SCF-cycle')
for iter in self.scf.run(self.wfs, self.hamiltonian, self.density,
self.occupations, self.forces):
self.iter = iter
self.call_observers(iter)
self.print_iteration(iter)
self.timer.stop('SCF-cycle')
if self.scf.converged:
self.call_observers(iter, final=True)
self.print_converged(iter)
elif converge:
self.txt.write(oops)
raise KohnShamConvergenceError(
'Did not converge! See text output for help.')
return True
def initialize_positions(self, atoms=None):
"""Update the positions of the atoms."""
if atoms is None:
atoms = self.atoms
else:
# Save the state of the atoms:
self.atoms = atoms.copy()
self.check_atoms()
spos_ac = atoms.get_scaled_positions() % 1.0
self.wfs.set_positions(spos_ac)
self.density.set_positions(spos_ac, self.wfs.rank_a)
self.hamiltonian.set_positions(spos_ac, self.wfs.rank_a)
return spos_ac
def set_positions(self, atoms=None):
"""Update the positions of the atoms and initialize wave functions."""
spos_ac = self.initialize_positions(atoms)
self.wfs.initialize(self.density, self.hamiltonian, spos_ac)
self.wfs.eigensolver.reset()
self.scf.reset()
self.forces.reset()
self.stress_vv = None
self.dipole_v = None
self.magmom_av = None
self.print_positions()
def initialize(self, atoms=None):
"""Inexpensive initialization."""
if atoms is None:
atoms = self.atoms
else:
# Save the state of the atoms:
self.atoms = atoms.copy()
par = self.input_parameters
world = par.communicator
if world is None:
world = mpi.world
elif hasattr(world, 'new_communicator'):
# Check for whether object has correct type already
#
# Using isinstance() is complicated because of all the
# combinations, serial/parallel/debug...
pass
else:
# world should be a list of ranks:
world = mpi.world.new_communicator(np.asarray(world))
self.wfs.world = world
if 'txt' in self._changed_keywords:
self.set_txt(par.txt)
self.verbose = par.verbose
natoms = len(atoms)
cell_cv = atoms.get_cell() / Bohr
pbc_c = atoms.get_pbc()
Z_a = atoms.get_atomic_numbers()
magmom_av = atoms.get_initial_magnetic_moments()
self.check_atoms()
# Generate new xc functional only when it is reset by set
# XXX sounds like this should use the _changed_keywords dictionary.
if self.hamiltonian is None or self.hamiltonian.xc is None:
if isinstance(par.xc, str):
xc = XC(par.xc)
else:
xc = par.xc
else:
xc = self.hamiltonian.xc
mode = par.mode
if mode == 'fd':
mode = FD()
elif mode == 'pw':
mode = pw.PW()
elif mode == 'lcao':
mode = LCAO()
else:
assert hasattr(mode, 'name'), str(mode)
if xc.orbital_dependent and mode.name == 'lcao':
raise NotImplementedError('LCAO mode does not support '
'orbital-dependent XC functionals.')
if par.realspace is None:
realspace = (mode.name != 'pw')
else:
realspace = par.realspace
if mode.name == 'pw':
assert not realspace
if par.filter is None and mode.name != 'pw':
gamma = 1.6
if par.gpts is not None:
h = ((np.linalg.inv(cell_cv)**2).sum(0)**-0.5
/ par.gpts).max()
else:
h = (par.h or 0.2) / Bohr
def filter(rgd, rcut, f_r, l=0):
gcut = np.pi / h - 2 / rcut / gamma
f_r[:] = rgd.filter(f_r, rcut * gamma, gcut, l)
else:
filter = par.filter
setups = Setups(Z_a, par.setups, par.basis, par.lmax, xc,
filter, world)
if magmom_av.ndim == 1:
collinear = True
magmom_av, magmom_a = np.zeros((natoms, 3)), magmom_av
magmom_av[:, 2] = magmom_a
else:
collinear = False
magnetic = magmom_av.any()
spinpol = par.spinpol
if par.hund:
if natoms != 1:
raise ValueError('hund=True arg only valid for single atoms!')
spinpol = True
magmom_av[0] = (0, 0, setups[0].get_hunds_rule_moment(par.charge))
if spinpol is None:
spinpol = magnetic
elif magnetic and not spinpol:
raise ValueError('Non-zero initial magnetic moment for a ' +
'spin-paired calculation!')
if collinear:
nspins = 1 + int(spinpol)
ncomp = 1
else:
nspins = 1
ncomp = 2
if par.usesymm != 'default':
warnings.warn('Use "symmetry" keyword instead of ' +
'"usesymm" keyword')
par.symmetry = usesymm2symmetry(par.usesymm)
symm = par.symmetry
if symm == 'off':
symm = {'point_group': False, 'time_reversal': False}
bzkpts_kc = kpts2ndarray(par.kpts, self.atoms)
kd = KPointDescriptor(bzkpts_kc, nspins, collinear)
m_av = magmom_av.round(decimals=3) # round off
id_a = zip(setups.id_a, *m_av.T)
symmetry = Symmetry(id_a, cell_cv, atoms.pbc, **symm)
kd.set_symmetry(atoms, symmetry, comm=world)
setups.set_symmetry(symmetry)
if par.gpts is not None:
N_c = np.array(par.gpts)
else:
h = par.h
if h is not None:
h /= Bohr
N_c = get_number_of_grid_points(cell_cv, h, mode, realspace,
kd.symmetry)
symmetry.check_grid(N_c)
width = par.width
if width is None:
if pbc_c.any():
width = 0.1 # eV
else:
width = 0.0
else:
assert par.occupations is None
if hasattr(self, 'time') or par.dtype == complex:
dtype = complex
else:
if kd.gamma:
dtype = float
else:
dtype = complex
nao = setups.nao
nvalence = setups.nvalence - par.charge
M_v = magmom_av.sum(0)
M = np.dot(M_v, M_v) ** 0.5
nbands = par.nbands
orbital_free = any(setup.orbital_free for setup in setups)
if orbital_free:
nbands = 1
if isinstance(nbands, basestring):
if nbands[-1] == '%':
basebands = int(nvalence + M + 0.5) // 2
nbands = int((float(nbands[:-1]) / 100) * basebands)
else:
raise ValueError('Integer Expected: Only use a string '
'if giving a percentage of occupied bands')
if nbands is None:
nbands = 0
for setup in setups:
nbands_from_atom = setup.get_default_nbands()
# Any obscure setup errors?
if nbands_from_atom < -(-setup.Nv // 2):
raise ValueError('Bad setup: This setup requests %d'
' bands but has %d electrons.'
% (nbands_from_atom, setup.Nv))
nbands += nbands_from_atom
nbands = min(nao, nbands)
elif nbands > nao and mode.name == 'lcao':
raise ValueError('Too many bands for LCAO calculation: '
'%d bands and only %d atomic orbitals!' %
(nbands, nao))
if nvalence < 0:
raise ValueError(
'Charge %f is not possible - not enough valence electrons' %
par.charge)
if nbands <= 0:
nbands = int(nvalence + M + 0.5) // 2 + (-nbands)
if nvalence > 2 * nbands and not orbital_free:
raise ValueError('Too few bands! Electrons: %f, bands: %d'
% (nvalence, nbands))
nbands *= ncomp
if par.width is not None:
self.text('**NOTE**: please start using '
'occupations=FermiDirac(width).')
if par.fixmom:
self.text('**NOTE**: please start using '
'occupations=FermiDirac(width, fixmagmom=True).')
if self.occupations is None:
if par.occupations is None:
# Create object for occupation numbers:
if orbital_free:
width = 0.0 # even for PBC
self.occupations = occupations.TFOccupations(width,
par.fixmom)
else:
self.occupations = occupations.FermiDirac(width,
par.fixmom)
else:
self.occupations = par.occupations
# If occupation numbers are changed, and we have wave functions,
# recalculate the occupation numbers
if self.wfs is not None and not isinstance(
self.wfs,
EmptyWaveFunctions):
self.occupations.calculate(self.wfs)
self.occupations.magmom = M_v[2]
cc = par.convergence
if mode.name == 'lcao':
niter_fixdensity = 0
else:
niter_fixdensity = None
if self.scf is None:
force_crit = cc['forces']
if force_crit is not None:
force_crit /= Hartree / Bohr
self.scf = SCFLoop(
cc['eigenstates'] / Hartree**2 * nvalence,
cc['energy'] / Hartree * max(nvalence, 1),
cc['density'] * nvalence,
par.maxiter, par.fixdensity,
niter_fixdensity,
force_crit)
parsize_kpt = par.parallel['kpt']
parsize_domain = par.parallel['domain']
parsize_bands = par.parallel['band']
if not realspace:
pbc_c = np.ones(3, bool)
if not self.wfs:
if parsize_domain == 'domain only': # XXX this was silly!
parsize_domain = world.size
parallelization = mpi.Parallelization(world,
nspins * kd.nibzkpts)
ndomains = None
if parsize_domain is not None:
ndomains = np.prod(parsize_domain)
if mode.name == 'pw':
if ndomains > 1:
raise ValueError('Planewave mode does not support '
'domain decomposition.')
ndomains = 1
parallelization.set(kpt=parsize_kpt,
domain=ndomains,
band=parsize_bands)
comms = parallelization.build_communicators()
domain_comm = comms['d']
kpt_comm = comms['k']
band_comm = comms['b']
kptband_comm = comms['D']
domainband_comm = comms['K']
self.comms = comms
kd.set_communicator(kpt_comm)
parstride_bands = par.parallel['stridebands']
# Unfortunately we need to remember that we adjusted the
# number of bands so we can print a warning if it differs
# from the number specified by the user. (The number can
# be inferred from the input parameters, but it's tricky
# because we allow negative numbers)
self.nbands_parallelization_adjustment = -nbands % band_comm.size
nbands += self.nbands_parallelization_adjustment
# I would like to give the following error message, but apparently
# there are cases, e.g. gpaw/test/gw_ppa.py, which involve
# nbands > nao and are supposed to work that way.
#if nbands > nao:
# raise ValueError('Number of bands %d adjusted for band '
# 'parallelization %d exceeds number of atomic '
# 'orbitals %d. This problem can be fixed '
# 'by reducing the number of bands a bit.'
# % (nbands, band_comm.size, nao))
bd = BandDescriptor(nbands, band_comm, parstride_bands)
if (self.density is not None and
self.density.gd.comm.size != domain_comm.size):
# Domain decomposition has changed, so we need to
# reinitialize density and hamiltonian:
if par.fixdensity:
raise RuntimeError(
'Density reinitialization conflict ' +
'with "fixdensity" - specify domain decomposition.')
self.density = None
self.hamiltonian = None
# Construct grid descriptor for coarse grids for wave functions:
gd = self.grid_descriptor_class(N_c, cell_cv, pbc_c,
domain_comm, parsize_domain)
# do k-point analysis here? XXX
args = (gd, nvalence, setups, bd, dtype, world, kd,
kptband_comm, self.timer)
if par.parallel['sl_auto']:
# Choose scalapack parallelization automatically
for key, val in par.parallel.items():
if (key.startswith('sl_') and key != 'sl_auto'
and val is not None):
raise ValueError("Cannot use 'sl_auto' together "
"with '%s'" % key)
max_scalapack_cpus = bd.comm.size * gd.comm.size
nprow = max_scalapack_cpus
npcol = 1
# Get a sort of reasonable number of columns/rows
while npcol < nprow and nprow % 2 == 0:
npcol *= 2
nprow //= 2
assert npcol * nprow == max_scalapack_cpus
# ScaLAPACK creates trouble if there aren't at least a few
# whole blocks; choose block size so there will always be
# several blocks. This will crash for small test systems,
# but so will ScaLAPACK in any case
blocksize = min(-(-nbands // 4), 64)
sl_default = (nprow, npcol, blocksize)
else:
sl_default = par.parallel['sl_default']
if mode.name == 'lcao':
# Layouts used for general diagonalizer
sl_lcao = par.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
lcaoksl = get_KohnSham_layouts(sl_lcao, 'lcao',
gd, bd, domainband_comm, dtype,
nao=nao, timer=self.timer)
self.wfs = mode(collinear, lcaoksl, *args)
elif mode.name == 'fd' or mode.name == 'pw':
# buffer_size keyword only relevant for fdpw
buffer_size = par.parallel['buffer_size']
# Layouts used for diagonalizer
sl_diagonalize = par.parallel['sl_diagonalize']
if sl_diagonalize is None:
sl_diagonalize = sl_default
diagksl = get_KohnSham_layouts(sl_diagonalize, 'fd', # XXX
# choice of key 'fd' not so nice
gd, bd, domainband_comm, dtype,
buffer_size=buffer_size,
timer=self.timer)
# Layouts used for orthonormalizer
sl_inverse_cholesky = par.parallel['sl_inverse_cholesky']
if sl_inverse_cholesky is None:
sl_inverse_cholesky = sl_default
if sl_inverse_cholesky != sl_diagonalize:
message = 'sl_inverse_cholesky != sl_diagonalize ' \
'is not implemented.'
raise NotImplementedError(message)
orthoksl = get_KohnSham_layouts(sl_inverse_cholesky, 'fd',
gd, bd, domainband_comm, dtype,
buffer_size=buffer_size,
timer=self.timer)
# Use (at most) all available LCAO for initialization
lcaonbands = min(nbands, nao)
try:
lcaobd = BandDescriptor(lcaonbands, band_comm,
parstride_bands)
except RuntimeError:
initksl = None
else:
# Layouts used for general diagonalizer
# (LCAO initialization)
sl_lcao = par.parallel['sl_lcao']
if sl_lcao is None:
sl_lcao = sl_default
initksl = get_KohnSham_layouts(sl_lcao, 'lcao',
gd, lcaobd, domainband_comm,
dtype, nao=nao,
timer=self.timer)
if hasattr(self, 'time'):
assert mode.name == 'fd'
from gpaw.tddft import TimeDependentWaveFunctions
self.wfs = TimeDependentWaveFunctions(
par.stencils[0],
diagksl,
orthoksl,
initksl,
gd,
nvalence,
setups,
bd,
world,
kd,
kptband_comm,
self.timer)
elif mode.name == 'fd':
self.wfs = mode(par.stencils[0], diagksl,
orthoksl, initksl, *args)
else:
assert mode.name == 'pw'
self.wfs = mode(diagksl, orthoksl, initksl, *args)
else:
self.wfs = mode(self, *args)
else:
self.wfs.set_setups(setups)
if not self.wfs.eigensolver:
# Number of bands to converge:
nbands_converge = cc['bands']
if nbands_converge == 'all':
nbands_converge = nbands
elif nbands_converge != 'occupied':
assert isinstance(nbands_converge, int)
if nbands_converge < 0:
nbands_converge += nbands
eigensolver = get_eigensolver(par.eigensolver, mode,
par.convergence)
eigensolver.nbands_converge = nbands_converge
# XXX Eigensolver class doesn't define an nbands_converge property
if isinstance(xc, SIC):
eigensolver.blocksize = 1
self.wfs.set_eigensolver(eigensolver)
if self.density is None:
gd = self.wfs.gd
if par.stencils[1] != 9:
# Construct grid descriptor for fine grids for densities
# and potentials:
finegd = gd.refine()
else:
# Special case (use only coarse grid):
finegd = gd
if realspace:
self.density = RealSpaceDensity(
gd, finegd, nspins, par.charge + setups.core_charge,
collinear, par.stencils[1])
else:
self.density = pw.ReciprocalSpaceDensity(
gd, finegd, nspins, par.charge + setups.core_charge,
collinear)
self.density.initialize(setups, self.timer, magmom_av, par.hund)
self.density.set_mixer(par.mixer)
if self.hamiltonian is None:
gd, finegd = self.density.gd, self.density.finegd
if realspace:
self.hamiltonian = RealSpaceHamiltonian(
gd, finegd, nspins, setups, self.timer, xc,
world, self.wfs.kptband_comm, par.external,
collinear, par.poissonsolver, par.stencils[1])
else:
self.hamiltonian = pw.ReciprocalSpaceHamiltonian(
gd, finegd, self.density.pd2, self.density.pd3,
nspins, setups, self.timer, xc, world,
self.wfs.kptband_comm, par.external, collinear)
xc.initialize(self.density, self.hamiltonian, self.wfs,
self.occupations)
self.text()
self.print_memory_estimate(self.txt, maxdepth=memory_estimate_depth)
self.txt.flush()
self.timer.print_info(self)
if dry_run:
self.dry_run()
if realspace and \
self.hamiltonian.poisson.get_description() == 'FDTD+TDDFT':
self.hamiltonian.poisson.set_density(self.density)
self.hamiltonian.poisson.print_messages(self.text)
self.txt.flush()
self.initialized = True
self._changed_keywords.clear()
def dry_run(self):
# Can be overridden like in gpaw.atom.atompaw
self.print_cell_and_parameters()
self.print_positions()
self.txt.flush()
raise SystemExit
def linearize_to_xc(self, newxc):
"""Linearize Hamiltonian to difference XC functional.
Used in real time TDDFT to perform calculations with various kernels.
"""
if isinstance(newxc, str):
newxc = XC(newxc)
self.txt.write('Linearizing xc-hamiltonian to ' + str(newxc))
newxc.initialize(self.density, self.hamiltonian, self.wfs,
self.occupations)
self.hamiltonian.linearize_to_xc(newxc, self.density)
def restore_state(self):
"""After restart, calculate fine density and poisson solution.
These are not initialized by default.
TODO: Is this really the most efficient way?
"""
spos_ac = self.atoms.get_scaled_positions() % 1.0
self.density.set_positions(spos_ac, self.wfs.rank_a)
self.density.interpolate_pseudo_density()
self.density.calculate_pseudo_charge()
self.hamiltonian.set_positions(spos_ac, self.wfs.rank_a)
self.hamiltonian.update(self.density)
def attach(self, function, n=1, *args, **kwargs):
"""Register observer function.
Call *function* using *args* and
*kwargs* as arguments.
If *n* is positive, then
*function* will be called every *n* iterations + the
final iteration if it would not be otherwise
If *n* is negative, then *function* will only be
called on iteration *abs(n)*.
If *n* is 0, then *function* will only be called
on convergence"""
try:
slf = function.im_self
except AttributeError:
pass
else:
if slf is self:
# function is a bound method of self. Store the name
# of the method and avoid circular reference:
function = function.im_func.func_name
self.observers.append((function, n, args, kwargs))
def call_observers(self, iter, final=False):
"""Call all registered callback functions."""
for function, n, args, kwargs in self.observers:
call = False
# Call every n iterations, including the last
if n > 0:
if ((iter % n) == 0) != final:
call = True
# Call only on iteration n
elif n < 0 and not final:
if iter == abs(n):
call = True
# Call only on convergence
elif n == 0 and final:
call = True
if call:
if isinstance(function, str):
function = getattr(self, function)
function(*args, **kwargs)
def get_reference_energy(self):
return self.wfs.setups.Eref * Hartree
def write(self, filename, mode='', cmr_params={}, **kwargs):
"""Write state to file.
use mode='all' to write the wave functions. cmr_params is a
dictionary that allows you to specify parameters for CMR
(Computational Materials Repository).
"""
self.timer.start('IO')
gpaw.io.write(self, filename, mode, cmr_params=cmr_params, **kwargs)
self.timer.stop('IO')
def get_myu(self, k, s):
"""Return my u corresponding to a certain kpoint and spin - or None"""
# very slow, but we are sure that we have it
for u in range(len(self.wfs.kpt_u)):
if self.wfs.kpt_u[u].k == k and self.wfs.kpt_u[u].s == s:
return u
return None
def get_homo_lumo(self):
"""Return H**O and LUMO eigenvalues."""
return self.occupations.get_homo_lumo(self.wfs) * Hartree
def estimate_memory(self, mem):
"""Estimate memory use of this object."""
for name, obj in [('Density', self.density),
('Hamiltonian', self.hamiltonian),
('Wavefunctions', self.wfs),
]:
obj.estimate_memory(mem.subnode(name))
def print_memory_estimate(self, txt=None, maxdepth=-1):
"""Print estimated memory usage for PAW object and components.
maxdepth is the maximum nesting level of displayed components.
The PAW object must be initialize()'d, but needs not have large
arrays allocated."""
# NOTE. This should work with --dry-run=N
#
# However, the initial overhead estimate is wrong if this method
# is called within a real mpirun/gpaw-python context.
if txt is None:
txt = self.txt
txt.write('Memory estimate\n')
txt.write('---------------\n')
mem_init = maxrss() # initial overhead includes part of Hamiltonian!
txt.write('Process memory now: %.2f MiB\n' % (mem_init / 1024.0**2))
mem = MemNode('Calculator', 0)
try:
self.estimate_memory(mem)
except AttributeError as m:
txt.write('Attribute error: %r' % m)
txt.write('Some object probably lacks estimate_memory() method')
txt.write('Memory breakdown may be incomplete')
mem.calculate_size()
mem.write(txt, maxdepth=maxdepth)
def converge_wave_functions(self):
"""Converge the wave-functions if not present."""
if not self.wfs or not self.scf:
self.initialize()
else:
self.wfs.initialize_wave_functions_from_restart_file()
spos_ac = self.atoms.get_scaled_positions() % 1.0
self.wfs.set_positions(spos_ac)
no_wave_functions = (self.wfs.kpt_u[0].psit_nG is None)
converged = self.scf.check_convergence(self.density,
self.wfs.eigensolver, self.wfs,
self.hamiltonian, self.forces)
if no_wave_functions or not converged:
self.wfs.eigensolver.error = np.inf
self.scf.converged = False
# is the density ok ?
error = self.density.mixer.get_charge_sloshing()
criterion = (self.input_parameters['convergence']['density']
* self.wfs.nvalence)
if error < criterion and not self.hamiltonian.xc.orbital_dependent:
self.scf.fix_density()
self.calculate()
def diagonalize_full_hamiltonian(self, nbands=None, scalapack=None, expert=False):
self.wfs.diagonalize_full_hamiltonian(self.hamiltonian, self.atoms,
self.occupations, self.txt,
nbands, scalapack, expert)
def check_atoms(self):
"""Check that atoms objects are identical on all processors."""
if not mpi.compare_atoms(self.atoms, comm=self.wfs.world):
raise RuntimeError('Atoms objects on different processors ' +
'are not identical!')
