def interpolate_pseudo_density(self, gridrefinement=2):
gd = self.gd
Fnt_wsg = self.Fnt_wsG.copy()
# Find m for
# gridrefinement = 2**m
m1 = np.log(gridrefinement) / np.log(2.)
m = int(np.round(m1))
# Check if m is really integer
if np.absolute(m - m1) < 1e-8:
for i in range(m):
gd2 = gd.refine()
# Interpolate
interpolator = Transformer(gd, gd2, self.stencil,
dtype=self.dtype)
Fnt2_wsg = gd2.empty((self.nw, self.nspins), dtype=self.dtype)
for w in range(self.nw):
for s in range(self.nspins):
interpolator.apply(Fnt_wsg[w][s], Fnt2_wsg[w][s],
np.ones((3, 2), dtype=complex))
gd = gd2
Fnt_wsg = Fnt2_wsg
else:
raise NotImplementedError
return Fnt_wsg, gd
def interpolate_pseudo_density(self, gridrefinement=2):
gd = self.gd
Fnt_wsg = self.Fnt_wsG.copy()
# Find m for
# gridrefinement = 2**m
m1 = np.log(gridrefinement) / np.log(2.)
m = int(np.round(m1))
# Check if m is really integer
if np.absolute(m - m1) < 1e-8:
for i in range(m):
gd2 = gd.refine()
# Interpolate
interpolator = Transformer(gd,
gd2,
self.stencil,
dtype=self.dtype)
Fnt2_wsg = gd2.empty((self.nw, self.nspins), dtype=self.dtype)
for w in range(self.nw):
for s in range(self.nspins):
interpolator.apply(Fnt_wsg[w][s], Fnt2_wsg[w][s],
np.ones((3, 2), dtype=complex))
gd = gd2
Fnt_wsg = Fnt2_wsg
else:
raise NotImplementedError
return Fnt_wsg, gd
def interpolate_2d(mat):
from gpaw.grid_descriptor import GridDescriptor
from gpaw.transformers import Transformer
nn = 10
N_c = np.zeros([3], dtype=int)
N_c[1:] = mat.shape[:2]
N_c[0] = nn
bmat = np.resize(mat, N_c)
gd = GridDescriptor(N_c, N_c)
finegd = GridDescriptor(N_c * 2, N_c)
interpolator = Transformer(gd, finegd, 3)
fine_bmat = finegd.zeros()
interpolator.apply(bmat, fine_bmat)
return fine_bmat[0]
def new_get_all_electron_density(self, atoms, gridrefinement=2):
"""Return real all-electron density array."""
# Refinement of coarse grid, for representation of the AE-density
if gridrefinement == 1:
gd = self.gd
n_sg = self.nt_sG.copy()
elif gridrefinement == 2:
gd = self.finegd
if self.nt_sg is None:
self.interpolate()
n_sg = self.nt_sg.copy()
elif gridrefinement == 4:
# Extra fine grid
gd = self.finegd.refine()
# Interpolation function for the density:
interpolator = Transformer(self.finegd, gd, 3)
# Transfer the pseudo-density to the fine grid:
n_sg = gd.empty(self.nspins)
if self.nt_sg is None:
self.interpolate()
for s in range(self.nspins):
interpolator.apply(self.nt_sg[s], n_sg[s])
else:
raise NotImplementedError
# Add corrections to pseudo-density to get the AE-density
splines = {}
phi_aj = []
phit_aj = []
nc_a = []
nct_a = []
for a, id in enumerate(self.setups.id_a):
if id in splines:
phi_j, phit_j, nc, nct = splines[id]
else:
# Load splines:
phi_j, phit_j, nc, nct = self.setups[a].get_partial_waves()[:4]
splines[id] = (phi_j, phit_j, nc, nct)
phi_aj.append(phi_j)
phit_aj.append(phit_j)
nc_a.append([nc])
nct_a.append([nct])
# Create localized functions from splines
phi = BasisFunctions(gd, phi_aj)
phit = BasisFunctions(gd, phit_aj)
nc = LFC(gd, nc_a)
nct = LFC(gd, nct_a)
spos_ac = atoms.get_scaled_positions() % 1.0
phi.set_positions(spos_ac)
phit.set_positions(spos_ac)
nc.set_positions(spos_ac)
nct.set_positions(spos_ac)
I_sa = np.zeros((self.nspins, len(atoms)))
a_W = np.empty(len(phi.M_W), np.int32)
W = 0
for a in phi.atom_indices:
nw = len(phi.sphere_a[a].M_w)
a_W[W:W + nw] = a
W += nw
rho_MM = np.zeros((phi.Mmax, phi.Mmax))
for s, I_a in enumerate(I_sa):
M1 = 0
for a, setup in enumerate(self.setups):
ni = setup.ni
D_sp = self.D_asp.get(a)
if D_sp is None:
D_sp = np.empty((self.nspins, ni * (ni + 1) // 2))
else:
I_a[a] = ((setup.Nct - setup.Nc) / self.nspins -
sqrt(4 * pi) *
np.dot(D_sp[s], setup.Delta_pL[:, 0]))
if gd.comm.size > 1:
gd.comm.broadcast(D_sp, self.rank_a[a])
M2 = M1 + ni
rho_MM[M1:M2, M1:M2] = unpack2(D_sp[s])
M1 = M2
phi.lfc.ae_valence_density_correction(rho_MM, n_sg[s], a_W, I_a)
phit.lfc.ae_valence_density_correction(-rho_MM, n_sg[s], a_W, I_a)
a_W = np.empty(len(nc.M_W), np.int32)
W = 0
for a in nc.atom_indices:
nw = len(nc.sphere_a[a].M_w)
a_W[W:W + nw] = a
W += nw
scale = 1.0 / self.nspins
for s, I_a in enumerate(I_sa):
nc.lfc.ae_core_density_correction(scale, n_sg[s], a_W, I_a)
nct.lfc.ae_core_density_correction(-scale, n_sg[s], a_W, I_a)
gd.comm.sum(I_a)
N_c = gd.N_c
g_ac = np.around(N_c * spos_ac).astype(int) % N_c - gd.beg_c
for I, g_c in zip(I_a, g_ac):
if (g_c >= 0).all() and (g_c < gd.n_c).all():
n_sg[s][tuple(g_c)] -= I / gd.dv
return n_sg, gd
def get_all_electron_density(self, atoms, gridrefinement=2):
"""Return real all-electron density array."""
# Refinement of coarse grid, for representation of the AE-density
if gridrefinement == 1:
gd = self.gd
n_sg = self.nt_sG.copy()
elif gridrefinement == 2:
gd = self.finegd
if self.nt_sg is None:
self.interpolate()
n_sg = self.nt_sg.copy()
elif gridrefinement == 4:
# Extra fine grid
gd = self.finegd.refine()
# Interpolation function for the density:
interpolator = Transformer(self.finegd, gd, 3)
# Transfer the pseudo-density to the fine grid:
n_sg = gd.empty(self.nspins)
if self.nt_sg is None:
self.interpolate()
for s in range(self.nspins):
interpolator.apply(self.nt_sg[s], n_sg[s])
else:
raise NotImplementedError
# Add corrections to pseudo-density to get the AE-density
splines = {}
phi_aj = []
phit_aj = []
nc_a = []
nct_a = []
for a, id in enumerate(self.setups.id_a):
if id in splines:
phi_j, phit_j, nc, nct = splines[id]
else:
# Load splines:
phi_j, phit_j, nc, nct = self.setups[a].get_partial_waves()[:4]
splines[id] = (phi_j, phit_j, nc, nct)
phi_aj.append(phi_j)
phit_aj.append(phit_j)
nc_a.append([nc])
nct_a.append([nct])
# Create localized functions from splines
phi = LFC(gd, phi_aj)
phit = LFC(gd, phit_aj)
nc = LFC(gd, nc_a)
nct = LFC(gd, nct_a)
spos_ac = atoms.get_scaled_positions() % 1.0
phi.set_positions(spos_ac)
phit.set_positions(spos_ac)
nc.set_positions(spos_ac)
nct.set_positions(spos_ac)
all_D_asp = []
for a, setup in enumerate(self.setups):
D_sp = self.D_asp.get(a)
if D_sp is None:
ni = setup.ni
D_sp = np.empty((self.nspins, ni * (ni + 1) // 2))
if gd.comm.size > 1:
gd.comm.broadcast(D_sp, self.rank_a[a])
all_D_asp.append(D_sp)
for s in range(self.nspins):
I_a = np.zeros(len(atoms))
nc.add1(n_sg[s], 1.0 / self.nspins, I_a)
nct.add1(n_sg[s], -1.0 / self.nspins, I_a)
phi.add2(n_sg[s], all_D_asp, s, 1.0, I_a)
phit.add2(n_sg[s], all_D_asp, s, -1.0, I_a)
for a, D_sp in self.D_asp.items():
setup = self.setups[a]
I_a[a] -= ((setup.Nc - setup.Nct) / self.nspins +
sqrt(4 * pi) *
np.dot(D_sp[s], setup.Delta_pL[:, 0]))
gd.comm.sum(I_a)
N_c = gd.N_c
g_ac = np.around(N_c * spos_ac).astype(int) % N_c - gd.beg_c
for I, g_c in zip(I_a, g_ac):
if (g_c >= 0).all() and (g_c < gd.n_c).all():
n_sg[s][tuple(g_c)] -= I / gd.dv
return n_sg, gd
class Density:
"""Density object.
Attributes:
=============== =====================================================
``gd`` Grid descriptor for coarse grids.
``finegd`` Grid descriptor for fine grids.
``interpolate`` Function for interpolating the electron density.
``mixer`` ``DensityMixer`` object.
=============== =====================================================
Soft and smooth pseudo functions on uniform 3D grids:
========== =========================================
``nt_sG`` Electron density on the coarse grid.
``nt_sg`` Electron density on the fine grid.
``nt_g`` Electron density on the fine grid.
``rhot_g`` Charge density on the fine grid.
``nct_G`` Core electron-density on the coarse grid.
========== =========================================
"""
def __init__(self, gd, finegd, nspins, charge):
"""Create the Density object."""
self.gd = gd
self.finegd = finegd
self.nspins = nspins
self.charge = float(charge)
self.charge_eps = 1e-7
self.D_asp = None
self.Q_aL = None
self.nct_G = None
self.nt_sG = None
self.rhot_g = None
self.nt_sg = None
self.nt_g = None
self.rank_a = None
self.mixer = BaseMixer()
self.timer = nulltimer
self.allocated = False
def initialize(self, setups, stencil, timer, magmom_a, hund):
self.timer = timer
self.setups = setups
self.hund = hund
self.magmom_a = magmom_a
# Interpolation function for the density:
self.interpolator = Transformer(self.gd, self.finegd, stencil,
allocate=False)
spline_aj = []
for setup in setups:
if setup.nct is None:
spline_aj.append([])
else:
spline_aj.append([setup.nct])
self.nct = LFC(self.gd, spline_aj,
integral=[setup.Nct for setup in setups],
forces=True, cut=True)
self.ghat = LFC(self.finegd, [setup.ghat_l for setup in setups],
integral=sqrt(4 * pi), forces=True)
if self.allocated:
self.allocated = False
self.allocate()
def allocate(self):
assert not self.allocated
self.interpolator.allocate()
self.allocated = True
def reset(self):
# TODO: reset other parameters?
self.nt_sG = None
def set_positions(self, spos_ac, rank_a=None):
if not self.allocated:
self.allocate()
self.nct.set_positions(spos_ac)
self.ghat.set_positions(spos_ac)
self.mixer.reset()
self.nct_G = self.gd.zeros()
self.nct.add(self.nct_G, 1.0 / self.nspins)
#self.nt_sG = None
self.nt_sg = None
self.nt_g = None
self.rhot_g = None
self.Q_aL = None
# If both old and new atomic ranks are present, start a blank dict if
# it previously didn't exist but it will needed for the new atoms.
if (self.rank_a is not None and rank_a is not None and
self.D_asp is None and (rank_a == self.gd.comm.rank).any()):
self.D_asp = {}
if self.rank_a is not None and self.D_asp is not None:
self.timer.start('Redistribute')
requests = []
flags = (self.rank_a != rank_a)
my_incoming_atom_indices = np.argwhere(np.bitwise_and(flags, \
rank_a == self.gd.comm.rank)).ravel()
my_outgoing_atom_indices = np.argwhere(np.bitwise_and(flags, \
self.rank_a == self.gd.comm.rank)).ravel()
for a in my_incoming_atom_indices:
# Get matrix from old domain:
ni = self.setups[a].ni
D_sp = np.empty((self.nspins, ni * (ni + 1) // 2))
requests.append(self.gd.comm.receive(D_sp, self.rank_a[a],
tag=a, block=False))
assert a not in self.D_asp
self.D_asp[a] = D_sp
for a in my_outgoing_atom_indices:
# Send matrix to new domain:
D_sp = self.D_asp.pop(a)
requests.append(self.gd.comm.send(D_sp, rank_a[a],
tag=a, block=False))
self.gd.comm.waitall(requests)
self.timer.stop('Redistribute')
self.rank_a = rank_a
def calculate_pseudo_density(self, wfs):
"""Calculate nt_sG from scratch.
nt_sG will be equal to nct_G plus the contribution from
wfs.add_to_density().
"""
wfs.calculate_density_contribution(self.nt_sG)
self.nt_sG += self.nct_G
def update(self, wfs):
self.timer.start('Density')
self.timer.start('Pseudo density')
self.calculate_pseudo_density(wfs)
self.timer.stop('Pseudo density')
self.timer.start('Atomic density matrices')
wfs.calculate_atomic_density_matrices(self.D_asp)
self.timer.stop('Atomic density matrices')
self.timer.start('Multipole moments')
comp_charge = self.calculate_multipole_moments()
self.timer.stop('Multipole moments')
if isinstance(wfs, LCAOWaveFunctions):
self.timer.start('Normalize')
self.normalize(comp_charge)
self.timer.stop('Normalize')
self.timer.start('Mix')
self.mix(comp_charge)
self.timer.stop('Mix')
self.timer.stop('Density')
def normalize(self, comp_charge=None):
"""Normalize pseudo density."""
if comp_charge is None:
comp_charge = self.calculate_multipole_moments()
pseudo_charge = self.gd.integrate(self.nt_sG).sum()
if pseudo_charge + self.charge + comp_charge != 0:
if pseudo_charge != 0:
x = -(self.charge + comp_charge) / pseudo_charge
self.nt_sG *= x
else:
# Use homogeneous background:
self.nt_sG[:] = (self.charge + comp_charge) * self.gd.dv
def calculate_pseudo_charge(self, comp_charge):
self.nt_g = self.nt_sg.sum(axis=0)
self.rhot_g = self.nt_g.copy()
self.ghat.add(self.rhot_g, self.Q_aL)
if debug:
charge = self.finegd.integrate(self.rhot_g) + self.charge
if abs(charge) > self.charge_eps:
raise RuntimeError('Charge not conserved: excess=%.9f' %
charge)
def mix(self, comp_charge):
if not self.mixer.mix_rho:
self.mixer.mix(self)
comp_charge = None
self.interpolate(comp_charge)
self.calculate_pseudo_charge(comp_charge)
if self.mixer.mix_rho:
self.mixer.mix(self)
def interpolate(self, comp_charge=None):
"""Interpolate pseudo density to fine grid."""
if comp_charge is None:
comp_charge = self.calculate_multipole_moments()
if self.nt_sg is None:
self.nt_sg = self.finegd.empty(self.nspins)
for s in range(self.nspins):
self.interpolator.apply(self.nt_sG[s], self.nt_sg[s])
# With periodic boundary conditions, the interpolation will
# conserve the number of electrons.
if not self.gd.pbc_c.all():
# With zero-boundary conditions in one or more directions,
# this is not the case.
pseudo_charge = -(self.charge + comp_charge)
if abs(pseudo_charge) > 1.0e-14:
x = pseudo_charge / self.finegd.integrate(self.nt_sg).sum()
self.nt_sg *= x
def calculate_multipole_moments(self):
"""Calculate multipole moments of compensation charges.
Returns the total compensation charge in units of electron
charge, so the number will be negative because of the
dominating contribution from the nuclear charge."""
comp_charge = 0.0
self.Q_aL = {}
for a, D_sp in self.D_asp.items():
Q_L = self.Q_aL[a] = np.dot(D_sp.sum(0), self.setups[a].Delta_pL)
Q_L[0] += self.setups[a].Delta0
comp_charge += Q_L[0]
return self.gd.comm.sum(comp_charge) * sqrt(4 * pi)
def initialize_from_atomic_densities(self, basis_functions):
"""Initialize D_asp, nt_sG and Q_aL from atomic densities.
nt_sG is initialized from atomic orbitals, and will
be constructed with the specified magnetic moments and
obeying Hund's rules if ``hund`` is true."""
# XXX does this work with blacs? What should be distributed?
# Apparently this doesn't use blacs at all, so it's serial
# with respect to the blacs distribution. That means it works
# but is not particularly efficient (not that this is a time
# consuming step)
f_sM = np.empty((self.nspins, basis_functions.Mmax))
self.D_asp = {}
f_asi = {}
for a in basis_functions.atom_indices:
c = self.charge / len(self.setups) # distribute on all atoms
f_si = self.setups[a].calculate_initial_occupation_numbers(
self.magmom_a[a], self.hund, charge=c, nspins=self.nspins)
if a in basis_functions.my_atom_indices:
self.D_asp[a] = self.setups[a].initialize_density_matrix(f_si)
f_asi[a] = f_si
self.nt_sG = self.gd.zeros(self.nspins)
basis_functions.add_to_density(self.nt_sG, f_asi)
self.nt_sG += self.nct_G
self.calculate_normalized_charges_and_mix()
def initialize_from_wavefunctions(self, wfs):
"""Initialize D_asp, nt_sG and Q_aL from wave functions."""
self.nt_sG = self.gd.empty(self.nspins)
self.calculate_pseudo_density(wfs)
self.D_asp = {}
my_atom_indices = np.argwhere(wfs.rank_a == self.gd.comm.rank).ravel()
for a in my_atom_indices:
ni = self.setups[a].ni
self.D_asp[a] = np.empty((self.nspins, ni * (ni + 1) // 2))
wfs.calculate_atomic_density_matrices(self.D_asp)
self.calculate_normalized_charges_and_mix()
def initialize_directly_from_arrays(self, nt_sG, D_asp):
"""Set D_asp and nt_sG directly."""
self.nt_sG = nt_sG
self.D_asp = D_asp
#self.calculate_normalized_charges_and_mix()
# No calculate multipole moments? Tests will fail because of
# improperly initialized mixer
def calculate_normalized_charges_and_mix(self):
comp_charge = self.calculate_multipole_moments()
self.normalize(comp_charge)
self.mix(comp_charge)
def set_mixer(self, mixer):
if mixer is not None:
if self.nspins == 1 and isinstance(mixer, MixerSum):
raise RuntimeError('Cannot use MixerSum with nspins==1')
self.mixer = mixer
else:
if self.gd.pbc_c.any():
beta = 0.1
weight = 50.0
else:
beta = 0.25
weight = 1.0
if self.nspins == 2:
self.mixer = MixerSum(beta=beta, weight=weight)
else:
self.mixer = Mixer(beta=beta, weight=weight)
self.mixer.initialize(self)
def estimate_magnetic_moments(self):
magmom_a = np.zeros_like(self.magmom_a)
if self.nspins == 2:
for a, D_sp in self.D_asp.items():
magmom_a[a] = np.dot(D_sp[0] - D_sp[1], self.setups[a].N0_p)
self.gd.comm.sum(magmom_a)
return magmom_a
def get_correction(self, a, spin):
"""Integrated atomic density correction.
Get the integrated correction to the pseuso density relative to
the all-electron density.
"""
setup = self.setups[a]
return sqrt(4 * pi) * (
np.dot(self.D_asp[a][spin], setup.Delta_pL[:, 0])
+ setup.Delta0 / self.nspins)
def get_density_array(self):
XXX
# XXX why not replace with get_spin_density and get_total_density?
"""Return pseudo-density array."""
if self.nspins == 2:
return self.nt_sG
else:
return self.nt_sG[0]
def get_all_electron_density(self, atoms, gridrefinement=2):
"""Return real all-electron density array."""
# Refinement of coarse grid, for representation of the AE-density
if gridrefinement == 1:
gd = self.gd
n_sg = self.nt_sG.copy()
elif gridrefinement == 2:
gd = self.finegd
if self.nt_sg is None:
self.interpolate()
n_sg = self.nt_sg.copy()
elif gridrefinement == 4:
# Extra fine grid
gd = self.finegd.refine()
# Interpolation function for the density:
interpolator = Transformer(self.finegd, gd, 3)
# Transfer the pseudo-density to the fine grid:
n_sg = gd.empty(self.nspins)
if self.nt_sg is None:
self.interpolate()
for s in range(self.nspins):
interpolator.apply(self.nt_sg[s], n_sg[s])
else:
raise NotImplementedError
# Add corrections to pseudo-density to get the AE-density
splines = {}
phi_aj = []
phit_aj = []
nc_a = []
nct_a = []
for a, id in enumerate(self.setups.id_a):
if id in splines:
phi_j, phit_j, nc, nct = splines[id]
else:
# Load splines:
phi_j, phit_j, nc, nct = self.setups[a].get_partial_waves()[:4]
splines[id] = (phi_j, phit_j, nc, nct)
phi_aj.append(phi_j)
phit_aj.append(phit_j)
nc_a.append([nc])
nct_a.append([nct])
# Create localized functions from splines
phi = LFC(gd, phi_aj)
phit = LFC(gd, phit_aj)
nc = LFC(gd, nc_a)
nct = LFC(gd, nct_a)
spos_ac = atoms.get_scaled_positions() % 1.0
phi.set_positions(spos_ac)
phit.set_positions(spos_ac)
nc.set_positions(spos_ac)
nct.set_positions(spos_ac)
all_D_asp = []
for a, setup in enumerate(self.setups):
D_sp = self.D_asp.get(a)
if D_sp is None:
ni = setup.ni
D_sp = np.empty((self.nspins, ni * (ni + 1) // 2))
if gd.comm.size > 1:
gd.comm.broadcast(D_sp, self.rank_a[a])
all_D_asp.append(D_sp)
for s in range(self.nspins):
I_a = np.zeros(len(atoms))
nc.add1(n_sg[s], 1.0 / self.nspins, I_a)
nct.add1(n_sg[s], -1.0 / self.nspins, I_a)
phi.add2(n_sg[s], all_D_asp, s, 1.0, I_a)
phit.add2(n_sg[s], all_D_asp, s, -1.0, I_a)
for a, D_sp in self.D_asp.items():
setup = self.setups[a]
I_a[a] -= ((setup.Nc - setup.Nct) / self.nspins +
sqrt(4 * pi) *
np.dot(D_sp[s], setup.Delta_pL[:, 0]))
gd.comm.sum(I_a)
N_c = gd.N_c
g_ac = np.around(N_c * spos_ac).astype(int) % N_c - gd.beg_c
for I, g_c in zip(I_a, g_ac):
if (g_c >= 0).all() and (g_c < gd.n_c).all():
n_sg[s][tuple(g_c)] -= I / gd.dv
return n_sg, gd
def new_get_all_electron_density(self, atoms, gridrefinement=2):
"""Return real all-electron density array."""
# Refinement of coarse grid, for representation of the AE-density
if gridrefinement == 1:
gd = self.gd
n_sg = self.nt_sG.copy()
elif gridrefinement == 2:
gd = self.finegd
if self.nt_sg is None:
self.interpolate()
n_sg = self.nt_sg.copy()
elif gridrefinement == 4:
# Extra fine grid
gd = self.finegd.refine()
# Interpolation function for the density:
interpolator = Transformer(self.finegd, gd, 3)
# Transfer the pseudo-density to the fine grid:
n_sg = gd.empty(self.nspins)
if self.nt_sg is None:
self.interpolate()
for s in range(self.nspins):
interpolator.apply(self.nt_sg[s], n_sg[s])
else:
raise NotImplementedError
# Add corrections to pseudo-density to get the AE-density
splines = {}
phi_aj = []
phit_aj = []
nc_a = []
nct_a = []
for a, id in enumerate(self.setups.id_a):
if id in splines:
phi_j, phit_j, nc, nct = splines[id]
else:
# Load splines:
phi_j, phit_j, nc, nct = self.setups[a].get_partial_waves()[:4]
splines[id] = (phi_j, phit_j, nc, nct)
phi_aj.append(phi_j)
phit_aj.append(phit_j)
nc_a.append([nc])
nct_a.append([nct])
# Create localized functions from splines
phi = BasisFunctions(gd, phi_aj)
phit = BasisFunctions(gd, phit_aj)
nc = LFC(gd, nc_a)
nct = LFC(gd, nct_a)
spos_ac = atoms.get_scaled_positions() % 1.0
phi.set_positions(spos_ac)
phit.set_positions(spos_ac)
nc.set_positions(spos_ac)
nct.set_positions(spos_ac)
I_sa = np.zeros((self.nspins, len(atoms)))
a_W = np.empty(len(phi.M_W), np.int32)
W = 0
for a in phi.atom_indices:
nw = len(phi.sphere_a[a].M_w)
a_W[W:W + nw] = a
W += nw
rho_MM = np.zeros((phi.Mmax, phi.Mmax))
for s, I_a in enumerate(I_sa):
M1 = 0
for a, setup in enumerate(self.setups):
ni = setup.ni
D_sp = self.D_asp.get(a)
if D_sp is None:
D_sp = np.empty((self.nspins, ni * (ni + 1) // 2))
else:
I_a[a] = ((setup.Nct - setup.Nc) / self.nspins -
sqrt(4 * pi) *
np.dot(D_sp[s], setup.Delta_pL[:, 0]))
if gd.comm.size > 1:
gd.comm.broadcast(D_sp, self.rank_a[a])
M2 = M1 + ni
rho_MM[M1:M2, M1:M2] = unpack2(D_sp[s])
M1 = M2
phi.lfc.ae_valence_density_correction(rho_MM, n_sg[s], a_W, I_a)
phit.lfc.ae_valence_density_correction(-rho_MM, n_sg[s], a_W, I_a)
a_W = np.empty(len(nc.M_W), np.int32)
W = 0
for a in nc.atom_indices:
nw = len(nc.sphere_a[a].M_w)
a_W[W:W + nw] = a
W += nw
scale = 1.0 / self.nspins
for s, I_a in enumerate(I_sa):
nc.lfc.ae_core_density_correction(scale, n_sg[s], a_W, I_a)
nct.lfc.ae_core_density_correction(-scale, n_sg[s], a_W, I_a)
gd.comm.sum(I_a)
N_c = gd.N_c
g_ac = np.around(N_c * spos_ac).astype(int) % N_c - gd.beg_c
for I, g_c in zip(I_a, g_ac):
if (g_c >= 0).all() and (g_c < gd.n_c).all():
n_sg[s][tuple(g_c)] -= I / gd.dv
return n_sg, gd
if extra_parameters.get('usenewlfc', True):
get_all_electron_density = new_get_all_electron_density
def estimate_memory(self, mem):
nspins = self.nspins
nbytes = self.gd.bytecount()
nfinebytes = self.finegd.bytecount()
arrays = mem.subnode('Arrays')
for name, size in [('nt_sG', nbytes * nspins),
('nt_sg', nfinebytes * nspins),
('nt_g', nfinebytes),
('rhot_g', nfinebytes),
('nct_G', nbytes)]:
arrays.subnode(name, size)
lfs = mem.subnode('Localized functions')
for name, obj in [('nct', self.nct),
('ghat', self.ghat)]:
obj.estimate_memory(lfs.subnode(name))
self.mixer.estimate_memory(mem.subnode('Mixer'), self.gd)
# TODO
# The implementation of interpolator memory use is not very
# accurate; 20 MiB vs 13 MiB estimated in one example, probably
# worse for parallel calculations.
self.interpolator.estimate_memory(mem.subnode('Interpolator'))
def get_spin_contamination(self, atoms, majority_spin=0):
"""Calculate the spin contamination.
Spin contamination is defined as the integral over the
spin density difference, where it is negative (i.e. the
minority spin density is larger than the majority spin density.
"""
if majority_spin == 0:
smaj = 0
smin = 1
else:
smaj = 1
smin = 0
nt_sg, gd = self.get_all_electron_density(atoms)
dt_sg = nt_sg[smin] - nt_sg[smaj]
dt_sg = np.where(dt_sg > 0, dt_sg, 0.0)
return gd.integrate(dt_sg)
class ResponseCalculator:
"""This class is a calculator for the sc density variation.
From the given perturbation, the set of coupled equations for the
first-order density response is solved self-consistently.
Parameters
----------
max_iter: int
Maximum number of iterations in the self-consistent evaluation of
the density variation.
tolerance_sc: float
Tolerance for the self-consistent loop measured in terms of
integrated absolute change of the density derivative between two
iterations.
tolerance_sternheimer: float
Tolerance for the solution of the Sternheimer equation -- passed to
the ``LinearSolver``.
beta: float (0 < beta < 1)
Mixing coefficient.
nmaxold: int
Length of history for the mixer.
weight: int
Weight for the mixer metric (=1 -> no metric used).
"""
parameters = {'verbose': False,
'max_iter': 100,
'max_iter_krylov': 1000,
'krylov_solver': 'cg',
'tolerance_sc': 1.0e-5,
'tolerance_sternheimer': 1.0e-4,
'use_pc': True,
'beta': 0.1,
'nmaxold': 6,
'weight': 50
}
def __init__(self, calc, wfs, poisson_solver=None, dtype=float, **kwargs):
"""Store calculator etc.
Parameters
----------
calc: Calculator
Calculator instance containing a ground-state calculation
(calc.set_positions must have been called before this point!).
wfs: WaveFunctions
Class taking care of wave-functions, projectors, k-point related
quantities and symmetries.
poisson_solver: PoissonSolver
Multigrid or FFT poisson solver (not required if the
``Perturbation`` to be solved for has a ``solve_poisson`` member
function).
dtype: ...
dtype of the density response.
"""
# Store ground-state quantities
self.hamiltonian = calc.hamiltonian
self.density = calc.density
self.wfs = wfs
# Get list of k-point containers
self.kpt_u = wfs.kpt_u
# Poisson solver
if poisson_solver is None:
# Solver must be provided by the perturbation
self.poisson = None
self.solve_poisson = None
else:
self.poisson = poisson_solver
self.solve_poisson = self.poisson.solve_neutral
# Store grid-descriptors
self.gd = calc.density.gd
self.finegd = calc.density.finegd
# dtype for ground-state wave-functions
self.gs_dtype = calc.wfs.dtype
# dtype for the perturbing potential and density
self.dtype = dtype
# Grid transformer -- convert array from coarse to fine grid
self.interpolator = Transformer(self.gd, self.finegd, nn=3,
dtype=self.dtype, allocate=False)
# Grid transformer -- convert array from fine to coarse grid
self.restrictor = Transformer(self.finegd, self.gd, nn=3,
dtype=self.dtype, allocate=False)
# Sternheimer operator
self.sternheimer_operator = None
# Krylov solver
self.linear_solver = None
# Phases for transformer objects - since the perturbation determines
# the form of the density response this is obtained from the
# perturbation in the ``__call__`` member function below.
self.phase_cd = None
# Array attributes
self.nt1_G = None
self.vHXC1_G = None
self.nt1_g = None
self.vH1_g = None
# Perturbation
self.perturbation = None
# Number of occupied bands
nvalence = calc.wfs.nvalence
self.nbands = nvalence/2 + nvalence%2
assert self.nbands <= calc.wfs.nbands
self.initialized = False
self.parameters = {}
self.set(**kwargs)
def clean(self):
"""Cleanup before call to ``__call__``."""
self.perturbation = None
self.solve_poisson = None
self.nt1_G = None
self.vHXC1_G = None
self.nt1_g = None
self.vH1_g = None
def __call__(self, perturbation):
"""Calculate density response (derivative) to perturbation.
Parameters
----------
perturbation: Perturbation
Class implementing the perturbing potential. Must provide an
``apply`` member function implementing the multiplication of the
perturbing potential to a (set of) state vector(s).
"""
assert self.initialized, ("Linear response calculator "
"not initizalized.")
self.clean()
if self.poisson is None:
assert hasattr(perturbation, 'solve_poisson')
self.solve_poisson = perturbation.solve_poisson
# Store perturbation - used in other member functions
self.perturbation = perturbation
# Reset mixer
self.mixer.reset()
# Reset wave-functions
self.wfs.reset()
# Set phase attribute for Transformer objects
self.phase_cd = self.perturbation.get_phase_cd()
# Parameters for the SC-loop
p = self.parameters
max_iter = p['max_iter']
tolerance = p['tolerance_sc']
for iter in range(max_iter):
if iter == 0:
self.first_iteration()
else:
print "iter:%3i\t" % iter,
norm = self.iteration()
print "abs-norm: %6.3e\t" % norm,
print ("integrated density response (abs): % 5.2e (%5.2e) "
% (self.gd.integrate(self.nt1_G.real),
self.gd.integrate(np.absolute(self.nt1_G))))
if norm < tolerance:
print ("self-consistent loop converged in %i iterations"
% iter)
break
if iter == max_iter:
raise RuntimeError, ("self-consistent loop did not converge "
"in %i iterations" % iter)
def set(self, **kwargs):
"""Set parameters for calculation."""
# Check for legal input parameters
for key, value in kwargs.items():
if not key in ResponseCalculator.parameters:
raise TypeError("Unknown keyword argument: '%s'" % key)
# Insert default values if not given
for key, value in ResponseCalculator.parameters.items():
if key not in kwargs:
kwargs[key] = value
self.parameters.update(kwargs)
def initialize(self, spos_ac):
"""Make the object ready for a calculation."""
# Parameters
p = self.parameters
beta = p['beta']
nmaxold = p['nmaxold']
weight = p['weight']
use_pc = p['use_pc']
tolerance_sternheimer = p['tolerance_sternheimer']
max_iter_krylov = p['max_iter_krylov']
krylov_solver = p['krylov_solver']
# Initialize WaveFunctions attribute
self.wfs.initialize(spos_ac)
# Initialize interpolator and restrictor
self.interpolator.allocate()
self.restrictor.allocate()
# Initialize mixer
# weight = 1 -> no metric is used
self.mixer = BaseMixer(beta=beta, nmaxold=nmaxold,
weight=weight, dtype=self.dtype)
self.mixer.initialize_metric(self.gd)
# Linear operator in the Sternheimer equation
self.sternheimer_operator = \
SternheimerOperator(self.hamiltonian, self.wfs, self.gd,
dtype=self.gs_dtype)
# Preconditioner for the Sternheimer equation
if p['use_pc']:
pc = ScipyPreconditioner(self.gd,
self.sternheimer_operator.project,
dtype=self.gs_dtype)
else:
pc = None
#XXX K-point of the pc must be set in the k-point loop -> store a ref.
self.pc = pc
# Linear solver for the solution of Sternheimer equation
self.linear_solver = ScipyLinearSolver(method=krylov_solver,
preconditioner=pc,
tolerance=tolerance_sternheimer,
max_iter=max_iter_krylov)
self.initialized = True
def first_iteration(self):
"""Perform first iteration of sc-loop."""
self.wave_function_variations()
self.density_response()
self.mixer.mix(self.nt1_G, [], phase_cd=self.phase_cd)
self.interpolate_density()
def iteration(self):
"""Perform iteration."""
# Update variation in the effective potential
self.effective_potential_variation()
# Update wave function variations
self.wave_function_variations()
# Update density
self.density_response()
# Mix - supply phase_cd here for metric inside the mixer
self.mixer.mix(self.nt1_G, [], phase_cd=self.phase_cd)
norm = self.mixer.get_charge_sloshing()
self.interpolate_density()
return norm
def interpolate_density(self):
"""Interpolate density derivative onto the fine grid."""
self.nt1_g = self.finegd.zeros(dtype=self.dtype)
self.interpolator.apply(self.nt1_G, self.nt1_g, phases=self.phase_cd)
def effective_potential_variation(self):
"""Calculate derivative of the effective potential (Hartree + XC)."""
# Hartree part
vHXC1_g = self.finegd.zeros(dtype=self.dtype)
self.solve_poisson(vHXC1_g, self.nt1_g)
# Store for evaluation of second order derivative
self.vH1_g = vHXC1_g.copy()
# XC part
nt_sg = self.density.nt_sg
fxct_sg = np.zeros_like(nt_sg)
self.hamiltonian.xc.calculate_fxc(self.finegd, nt_sg, fxct_sg)
vHXC1_g += fxct_sg[0] * self.nt1_g
# Transfer to coarse grid
self.vHXC1_G = self.gd.zeros(dtype=self.dtype)
self.restrictor.apply(vHXC1_g, self.vHXC1_G, phases=self.phase_cd)
def wave_function_variations(self):
"""Calculate variation in the wave-functions.
Parameters
----------
v1_G: ndarray
Variation of the local effective potential (Hartree + XC).
"""
verbose = self.parameters['verbose']
if verbose:
print "Calculating wave function variations"
if self.perturbation.has_q():
q_c = self.perturbation.get_q()
kplusq_k = self.wfs.kd.find_k_plus_q(q_c)
else:
kplusq_k = None
# Calculate wave-function variations for all k-points.
for kpt in self.kpt_u:
k = kpt.k
if verbose:
print "k-point %2.1i" % k
# Index of k+q vector
if kplusq_k is None:
kplusq = k
kplusqpt = kpt
else:
kplusq = kplusq_k[k]
kplusqpt = self.kpt_u[kplusq]
# Ground-state and first-order wave-functions
psit_nG = kpt.psit_nG
psit1_nG = kpt.psit1_nG
# Update the SternheimerOperator
self.sternheimer_operator.set_k(k)
self.sternheimer_operator.set_kplusq(kplusq)
# Update preconditioner
if self.pc is not None:
# k+q
self.pc.set_kpt(kplusqpt)
# Right-hand side of Sternheimer equations
# k and k+q
# XXX should only be done once for all k-points but maybe too cheap
# to bother ??
rhs_nG = self.gd.zeros(n=self.nbands, dtype=self.gs_dtype)
self.perturbation.apply(psit_nG, rhs_nG, self.wfs, k, kplusq)
if self.vHXC1_G is not None:
rhs_nG += self.vHXC1_G * psit_nG
# Project out occupied subspace
self.sternheimer_operator.project(rhs_nG)
# Loop over occupied bands
for n in range(self.nbands):
# Update band index in SternheimerOperator
self.sternheimer_operator.set_band(n)
# Get view of the Bloch function derivative
psit1_G = psit1_nG[n]
# Rhs of Sternheimer equation
rhs_G = -1 * rhs_nG[n]
# Solve Sternheimer equation
iter, info = self.linear_solver.solve(self.sternheimer_operator,
psit1_G, rhs_G)
if verbose:
print "\tBand %2.1i -" % n,
if info == 0:
if verbose:
print "linear solver converged in %i iterations" % iter
elif info > 0:
assert False, ("linear solver did not converge in maximum "
"number (=%i) of iterations for "
"k-point number %d" % (iter, k))
else:
assert False, ("linear solver failed to converge")
def density_response(self):
"""Calculate density response from variation in the wave-functions."""
# Density might be complex
self.nt1_G = self.gd.zeros(dtype=self.dtype)
for kpt in self.kpt_u:
# The weight of the k-points includes spin-degeneracy
w = kpt.weight
# Wave functions
psit_nG = kpt.psit_nG
psit1_nG = kpt.psit1_nG
for psit_G, psit1_G in zip(psit_nG, psit1_nG):
# NOTICE: this relies on the automatic down-cast of the complex
# array on the rhs to a real array when the lhs is real !!
# Factor 2 for time-reversal symmetry
self.nt1_G += 2 * w * psit_G.conj() * psit1_G
class HybridXC(HybridXCBase):
def __init__(self,
name,
hybrid=None,
xc=None,
finegrid=False,
unocc=False,
omega=None,
excitation=None,
excited=0,
stencil=2):
"""Mix standard functionals with exact exchange.
finegrid: boolean
Use fine grid for energy functional evaluations ?
unocc: boolean
Apply vxx also to unoccupied states ?
omega: float
RSF mixing parameter
excitation: string:
Apply operator for improved virtual orbitals
to unocc states? Possible modes:
singlet: excitations to singlets
triplet: excitations to triplets
average: average between singlets and tripletts
see f.e. http://dx.doi.org/10.1021/acs.jctc.8b00238
excited: number
Band to excite from - counted from H**O downwards
"""
self.finegrid = finegrid
self.unocc = unocc
self.excitation = excitation
self.excited = excited
HybridXCBase.__init__(self,
name,
hybrid=hybrid,
xc=xc,
omega=omega,
stencil=stencil)
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, density, hamiltonian, wfs, occupations):
assert wfs.kd.gamma
self.xc.initialize(density, hamiltonian, wfs, occupations)
self.kpt_comm = wfs.kd.comm
self.nspins = wfs.nspins
self.setups = wfs.setups
self.density = density
self.kpt_u = wfs.kpt_u
self.exx_s = np.zeros(self.nspins)
self.ekin_s = np.zeros(self.nspins)
self.nocc_s = np.empty(self.nspins, int)
self.gd = density.gd
self.redistributor = density.redistributor
use_charge_center = hamiltonian.poisson.use_charge_center
# XXX How do we construct a copy of the Poisson solver of the
# Hamiltonian? We don't know what class it is, etc., but gd
# may differ.
# XXX One might consider using a charged centered compensation
# charge for the PoissonSolver in the case of EXX as standard
self.poissonsolver = PoissonSolver('fd',
eps=1e-11,
use_charge_center=use_charge_center)
# self.poissonsolver = hamiltonian.poisson
if self.finegrid:
self.finegd = self.gd.refine()
# XXX Taking restrictor from Hamiltonian will not work in PW mode,
# will it? I think this supports only real-space mode.
# self.restrictor = hamiltonian.restrictor
self.restrictor = Transformer(self.finegd, self.gd, 3)
self.interpolator = Transformer(self.gd, self.finegd, 3)
else:
self.finegd = self.gd
self.ghat = LFC(self.finegd,
[setup.ghat_l for setup in density.setups],
integral=np.sqrt(4 * np.pi),
forces=True)
self.poissonsolver.set_grid_descriptor(self.finegd)
if self.rsf == 'Yukawa':
omega2 = self.omega**2
self.screened_poissonsolver = HelmholtzSolver(
k2=-omega2,
eps=1e-11,
nn=3,
use_charge_center=use_charge_center)
self.screened_poissonsolver.set_grid_descriptor(self.finegd)
def set_positions(self, spos_ac):
self.ghat.set_positions(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)
# Note that the quantities passed are on the
# density/Hamiltonian grids!
# They may be distributed differently from own quantities.
self.ekin = self.kpt_comm.sum(self.ekin_s.sum())
return exc + self.kpt_comm.sum(self.exx_s.sum())
def calculate_exx(self):
for kpt in self.kpt_u:
self.apply_orbital_dependent_hamiltonian(kpt, kpt.psit_nG)
def apply_orbital_dependent_hamiltonian(self,
kpt,
psit_nG,
Htpsit_nG=None,
dH_asp=None):
if kpt.f_n is None:
return
deg = 2 // self.nspins # Spin degeneracy
hybrid = self.hybrid
P_ani = kpt.P_ani
setups = self.setups
is_cam = self.is_cam
vt_g = self.finegd.empty()
if self.gd is not self.finegd:
vt_G = self.gd.empty()
if self.rsf == 'Yukawa':
y_vt_g = self.finegd.empty()
# if self.gd is not self.finegd:
# y_vt_G = self.gd.empty()
nocc = int(ceil(kpt.f_n.sum())) // (3 - self.nspins)
if self.excitation is not None:
ex_band = nocc - self.excited - 1
if self.excitation == 'singlet':
ex_weight = -1
elif self.excitation == 'triplet':
ex_weight = +1
else:
ex_weight = 0
if self.unocc or self.excitation is not None:
nbands = len(kpt.f_n)
else:
nbands = nocc
self.nocc_s[kpt.s] = nocc
if Htpsit_nG is not None:
kpt.vt_nG = self.gd.empty(nbands)
kpt.vxx_ani = {}
kpt.vxx_anii = {}
for a, P_ni in P_ani.items():
I = P_ni.shape[1]
kpt.vxx_ani[a] = np.zeros((nbands, I))
kpt.vxx_anii[a] = np.zeros((nbands, I, I))
exx = 0.0
ekin = 0.0
# XXXX nbands can be different numbers on different cpus!
# That means some will execute the loop and others not.
# And deadlocks with augment-grids.
# Determine pseudo-exchange
for n1 in range(nbands):
psit1_G = psit_nG[n1]
f1 = kpt.f_n[n1] / deg
for n2 in range(n1, nbands):
psit2_G = psit_nG[n2]
f2 = kpt.f_n[n2] / deg
if n1 != n2 and f1 == 0 and f1 == f2:
continue # Don't work on double unocc. bands
# Double count factor:
dc = (1 + (n1 != n2)) * deg
nt_G, rhot_g = self.calculate_pair_density(
n1, n2, psit_nG, P_ani)
vt_g[:] = 0.0
# XXXXX This will go wrong because we are solving the
# Poisson equation on the distribution of gd, not finegd
# Or maybe it's fixed now
self.poissonsolver.solve(vt_g,
-rhot_g,
charge=-float(n1 == n2),
eps=1e-12,
zero_initial_phi=True)
vt_g *= hybrid
if self.rsf == 'Yukawa':
y_vt_g[:] = 0.0
self.screened_poissonsolver.solve(y_vt_g,
-rhot_g,
charge=-float(n1 == n2),
eps=1e-12,
zero_initial_phi=True)
if is_cam: # Cam like correction
y_vt_g *= self.cam_beta
else:
y_vt_g *= hybrid
vt_g -= y_vt_g
if self.gd is self.finegd:
vt_G = vt_g
else:
self.restrictor.apply(vt_g, vt_G)
# Integrate the potential on fine and coarse grids
int_fine = self.finegd.integrate(vt_g * rhot_g)
int_coarse = self.gd.integrate(vt_G * nt_G)
if self.gd.comm.rank == 0: # only add to energy on master CPU
exx += 0.5 * dc * f1 * f2 * int_fine
ekin -= dc * f1 * f2 * int_coarse
if Htpsit_nG is not None:
Htpsit_nG[n1] += f2 * vt_G * psit2_G
if n1 == n2:
kpt.vt_nG[n1] = f1 * vt_G
if self.excitation is not None and n1 == ex_band:
Htpsit_nG[nocc:] += f1 * vt_G * psit_nG[nocc:]
else:
if self.excitation is None or n1 != ex_band \
or n2 < nocc:
Htpsit_nG[n2] += f1 * vt_G * psit1_G
else:
Htpsit_nG[n2] += f1 * ex_weight * vt_G * psit1_G
# Update the vxx_uni and vxx_unii vectors of the nuclei,
# used to determine the atomic hamiltonian, and the
# residuals
v_aL = self.ghat.dict()
self.ghat.integrate(vt_g, v_aL)
for a, v_L in v_aL.items():
v_ii = unpack(np.dot(setups[a].Delta_pL, v_L))
v_ni = kpt.vxx_ani[a]
v_nii = kpt.vxx_anii[a]
P_ni = P_ani[a]
v_ni[n1] += f2 * np.dot(v_ii, P_ni[n2])
if n1 != n2:
if self.excitation is None or n1 != ex_band or \
n2 < nocc:
v_ni[n2] += f1 * np.dot(v_ii, P_ni[n1])
else:
v_ni[n2] += f1 * ex_weight * \
np.dot(v_ii, P_ni[n1])
else:
# XXX Check this:
v_nii[n1] = f1 * v_ii
if self.excitation is not None and n1 == ex_band:
for nuoc in range(nocc, nbands):
v_ni[nuoc] += f1 * \
np.dot(v_ii, P_ni[nuoc])
def calculate_vv(ni, D_ii, M_pp, weight, addme=False):
"""Calculate the local corrections depending on Mpp."""
dexx = 0
dekin = 0
if not addme:
addsign = -2.0
else:
addsign = 2.0
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 += M_pp[p13, p24] * D_ii[i3, i4]
p12 = packed_index(i1, i2, ni)
if Htpsit_nG is not None:
dH_p[p12] += addsign * weight / \
deg * A / ((i1 != i2) + 1)
dekin += 2 * weight / deg * D_ii[i1, i2] * A
dexx -= weight / deg * D_ii[i1, i2] * A
return (dexx, dekin)
# Apply the atomic corrections to the energy and the Hamiltonian
# matrix
for a, P_ni in P_ani.items():
setup = setups[a]
if Htpsit_nG is not None:
# Add non-trivial corrections the Hamiltonian matrix
h_nn = symmetrize(
np.inner(P_ni[:nbands], kpt.vxx_ani[a][:nbands]))
ekin -= np.dot(kpt.f_n[:nbands], h_nn.diagonal())
dH_p = dH_asp[a][kpt.s]
# Get atomic density and Hamiltonian matrices
D_p = self.density.D_asp[a][kpt.s]
D_ii = unpack2(D_p)
ni = len(D_ii)
# Add atomic corrections to the valence-valence exchange energy
# --
# > D C D
# -- ii iiii ii
(dexx, dekin) = calculate_vv(ni, D_ii, setup.M_pp, hybrid)
ekin += dekin
exx += dexx
if self.rsf is not None:
Mg_pp = setup.calculate_yukawa_interaction(self.omega)
if is_cam:
(dexx, dekin) = calculate_vv(ni,
D_ii,
Mg_pp,
self.cam_beta,
addme=True)
else:
(dexx, dekin) = calculate_vv(ni,
D_ii,
Mg_pp,
hybrid,
addme=True)
ekin -= dekin
exx -= dexx
# Add valence-core exchange energy
# --
# > X D
# -- ii ii
if setup.X_p is not None:
exx -= hybrid * np.dot(D_p, setup.X_p)
if Htpsit_nG is not None:
dH_p -= hybrid * setup.X_p
ekin += hybrid * np.dot(D_p, setup.X_p)
if self.rsf == 'Yukawa' and setup.X_pg is not None:
if is_cam:
thybrid = self.cam_beta # 0th order
else:
thybrid = hybrid
exx += thybrid * np.dot(D_p, setup.X_pg)
if Htpsit_nG is not None:
dH_p += thybrid * setup.X_pg
ekin -= thybrid * np.dot(D_p, setup.X_pg)
elif self.rsf == 'Yukawa' and setup.X_pg is None:
thybrid = exp(-3.62e-2 * self.omega) # educated guess
if is_cam:
thybrid *= self.cam_beta
else:
thybrid *= hybrid
exx += thybrid * np.dot(D_p, setup.X_p)
if Htpsit_nG is not None:
dH_p += thybrid * setup.X_p
ekin -= thybrid * np.dot(D_p, setup.X_p)
# Add core-core exchange energy
if kpt.s == 0:
if self.rsf is None or is_cam:
if is_cam:
exx += self.cam_alpha * setup.ExxC
else:
exx += hybrid * setup.ExxC
self.exx_s[kpt.s] = self.gd.comm.sum(exx)
self.ekin_s[kpt.s] = self.gd.comm.sum(ekin)
def correct_hamiltonian_matrix(self, kpt, H_nn):
if not hasattr(kpt, 'vxx_ani'):
return
# if self.gd.comm.rank > 0:
# H_nn[:] = 0.0
nocc = self.nocc_s[kpt.s]
nbands = len(kpt.vt_nG)
for a, P_ni in kpt.P_ani.items():
H_nn[:nbands, :nbands] += symmetrize(
np.inner(P_ni[:nbands], kpt.vxx_ani[a]))
# self.gd.comm.sum(H_nn)
if not self.unocc or self.excitation is not None:
H_nn[:nocc, nocc:] = 0.0
H_nn[nocc:, :nocc] = 0.0
def calculate_pair_density(self, n1, n2, psit_nG, P_ani):
Q_aL = {}
for a, P_ni in P_ani.items():
P1_i = P_ni[n1]
P2_i = P_ni[n2]
D_ii = np.outer(P1_i, P2_i.conj()).real
D_p = pack(D_ii)
Q_aL[a] = np.dot(D_p, self.setups[a].Delta_pL)
nt_G = psit_nG[n1] * psit_nG[n2]
if self.finegd is self.gd:
nt_g = nt_G
else:
nt_g = self.finegd.empty()
self.interpolator.apply(nt_G, nt_g)
rhot_g = nt_g.copy()
self.ghat.add(rhot_g, Q_aL)
return nt_G, rhot_g
def add_correction(self,
kpt,
psit_xG,
Htpsit_xG,
P_axi,
c_axi,
n_x,
calculate_change=False):
if kpt.f_n is None:
return
if self.unocc or self.excitation is not None:
nocc = len(kpt.vt_nG)
else:
nocc = self.nocc_s[kpt.s]
if calculate_change:
for x, n in enumerate(n_x):
if n < nocc:
Htpsit_xG[x] += kpt.vt_nG[n] * psit_xG[x]
for a, P_xi in P_axi.items():
c_axi[a][x] += np.dot(kpt.vxx_anii[a][n], P_xi[x])
else:
for a, c_xi in c_axi.items():
c_xi[:nocc] += kpt.vxx_ani[a][:nocc]
def rotate(self, kpt, U_nn):
if kpt.f_n is None:
return
U_nn = U_nn.T.copy()
nocc = self.nocc_s[kpt.s]
if len(kpt.vt_nG) == nocc:
U_nn = U_nn[:nocc, :nocc]
gemm(1.0, kpt.vt_nG.copy(), U_nn, 0.0, kpt.vt_nG)
for v_ni in kpt.vxx_ani.values():
gemm(1.0, v_ni.copy(), U_nn, 0.0, v_ni)
for v_nii in kpt.vxx_anii.values():
gemm(1.0, v_nii.copy(), U_nn, 0.0, v_nii)
class TimeDependentHamiltonian():
def __init__(self, calc):
#initialization
self.calc = calc
self.wfs = calc.wfs
self.ham = calc.hamiltonian
self.den = calc.density
self.occ = calc.occupations
#initialization plane and grid descriptors from GPAW calculation
self.pd = calc.wfs.pd
self.gd = calc.wfs.gd
self.volume = np.abs(np.linalg.det(self.gd.cell_cv))
#number of k-points
self.nq = len(calc.wfs.kpt_u)
#number of bands
self.nbands = calc.get_number_of_bands()
#number of electrons
self.nelectrons = calc.get_number_of_electrons()
#kinetic operator
self.kinetic = np.zeros((self.nq, self.nbands, self.nbands),
dtype=complex)
#overlap operator
self.overlap = np.zeros((self.nq, self.nbands, self.nbands),
dtype=complex)
#local momentum operator
self.local_moment = np.zeros((3, self.nq, self.nbands, self.nbands),
dtype=complex)
#nonlocal momentum operator
self.nonlocal_moment = np.zeros((3, self.nq, self.nbands, self.nbands),
dtype=complex)
#Fermi-Dirac occupation
self.f_n = np.zeros((self.nq, self.nbands), dtype=float)
#ground state Kohn-Sham orbitals wavefunctions
psi_gs = []
#ground state Kohn-Sham orbitals density
den_gs = []
for kpt in self.wfs.kpt_u:
self.overlap[kpt.q] = np.eye(self.nbands)
self.f_n[kpt.q] = kpt.f_n
kinetic = 0.5 * self.pd.G2_qG[kpt.q] # |G+q|^2/2
gradient = self.pd.get_reciprocal_vectors(kpt.q)
psi = []
den = []
for n in range(self.nbands):
psi.append(self.pd.ifft(kpt.psit_nG[n], kpt.q))
den.append(np.abs(psi[-1])**2)
for m in range(self.nbands):
self.kinetic[kpt.q, n, m] = self.pd.integrate(
kpt.psit_nG[n], kinetic * kpt.psit_nG[m])
#calculation local momentum
#<psi_qn|\nabla|psi_qm>
for i in range(3):
self.local_moment[i, kpt.q, n, m] = self.pd.integrate(
kpt.psit_nG[n], gradient[:, i] * kpt.psit_nG[m])
psi_gs.append(psi)
den_gs.append(den)
self.psi_gs = np.array(psi_gs)
self.den_gs = np.array(den_gs, dtype=float)
#real space grid points
self.r = self.gd.get_grid_point_coordinates()
#initialization local and nonlocal part of pseudopotential
self.init_potential()
self.proj = np.zeros((self.nq, self.nbands, self.norb), dtype=complex)
self.proj_r = np.zeros((3, self.nq, self.nbands, self.norb),
dtype=complex)
self.density = self.den.nt_sG.copy()
#initialization charge density (ion+electrons) for Hartree potential
self.ion_density = calc.hamiltonian.poisson.pd.ifft(
calc.density.rhot_q) - calc.density.nt_sg[0]
#plane wave descriptor for Hartree potential
self.pd0 = self.ham.poisson.pd
#reciprocal |G|^2 vectors for Hartree potential V(G)=4pi/|G|^2
self.G2 = self.ham.poisson.G2_q
self.G = self.pd0.get_reciprocal_vectors()
#fine to coarse and coarse to fine grids transformers (for correct calculation local potential)
self.fine_to_coarse = Transformer(calc.density.finegd, calc.density.gd,
3)
self.coarse_to_fine = Transformer(calc.density.gd, calc.density.finegd,
3)
#initialization local potenital from ground state density
self.update_local_potential()
self.update_gauge([0, 0, 0])
#----------------------------------------------------------------------------------------------------
def init_potential(self):
#initialization of nonlocal part of pseudopotential
# V_NL=|chi_i> V_i <chi_i|
spline_aj = []
for setup in self.wfs.setups:
spline_aj.append(setup.pt_j)
self.lfc = PWLFC(spline_aj, self.pd)
self.lfc.set_positions(self.calc.spos_ac) #set position of atoms
proj_G = []
proj_r = [] #collect chi_i in real space using FFT
for kpt in self.wfs.kpt_u:
proj_G.append(self.lfc.expand(kpt.q))
proj = []
n_i = proj_G[-1].shape[1]
for i in range(n_i):
proj.append(self.pd.ifft(proj_G[-1][:, i].copy(), kpt.q))
proj_r.append(proj)
self.chi = np.array(proj_r) / self.gd.dv
s = 0 # s=0 because we perform spin-paired calculation
V = [] #collect V
for a in range(len(self.wfs.setups)):
dH_ii = unpack(self.ham.dH_asp[a][s])
V.append(dH_ii.diagonal())
V = np.array(V)
self.V = V.ravel()
self.norb = self.V.size # number of orbitals in nonlocal potential
#initialization of local part of pseudopotential
V = self.ham.vbar.pd.zeros()
self.ham.vbar.add(V)
self.Vloc = self.ham.vbar.pd.ifft(V)
#----------------------------------------------------------------------------------------------------
def update_density(self, wfn):
self.density[0] = np.zeros_like(self.density[0])
fast_density(self.density[0], wfn, self.den_gs)
self.occupation = np.sum(np.abs(wfn)**2, axis=2)
self.update_local_potential()
#----------------------------------------------------------------------------------------------------
def update_gauge(self, A):
#update projections p_qno=<chi_qo|psi_qn>
phase = np.exp(1j * np.einsum('ixyz,i->xyz', self.r, A))
fast_projections(self.proj, self.chi, phase, self.psi_gs, self.gd.dv)
#update interaction hamiltonian
#H_I=\nabla*A+0.5*A^2
self.interaction = np.einsum(
'i,iqnm->qnm', A,
self.local_moment) + 0.5 * np.linalg.norm(A)**2 * self.overlap
#calculation nonlocal momentum operator
# I_NL=-i[r,V_NL]=-i sum_o V_o (r|chi_o><chi_o - |chi_o><chi_o|r)
for i in range(3):
fast_projections(self.proj_r[0], self.chi, self.r[i] * phase,
self.psi_gs, self.gd.dv)
self.nonlocal_moment = -1j * (np.einsum(
'o,iqno,qmo->iqnm', self.V, self.proj_r.conj(), self.proj) -
np.einsum('o,qno,iqmo->iqnm', self.V,
self.proj.conj(), self.proj_r))
self.moment = self.local_moment + self.nonlocal_moment
#----------------------------------------------------------------------------------------------------
def update_local_potential(self):
#tranform density from coarse to fine grids
density = self.coarse_to_fine.apply(self.density.copy())
#calculate XC potential
VXC = np.zeros_like(density)
self.ham.xc.calculate(self.pd0.gd, density, VXC)
# calculate Hartree potential
charge_density = density + self.ion_density
VH = 4 * np.pi * self.pd0.fft(charge_density) / self.G2
VH = self.pd0.ifft(VH)
#transform Hartree and XC potential from fine to coarse grids
self.VXC = self.fine_to_coarse.apply(VXC[0])
self.VH = self.fine_to_coarse.apply(VH)
#----------------------------------------------------------------------------------------------------
def calculate_nonlocal(self):
#calculation nonlocal part of Hamiltonian
return np.einsum('o,qno,qmo->qnm', self.V, self.proj.conj(), self.proj)
#----------------------------------------------------------------------------------------------------
def calculate_local(self):
#calculation local part of Hamiltonian
local = np.zeros((self.nq, self.nbands, self.nbands), dtype=complex)
return fast_local(local, self.Vloc + self.VXC + self.VH, self.psi_gs,
self.gd.dv)
#----------------------------------------------------------------------------------------------------
def calculate_kinetic(self):
#calculation kinetic part of Hamiltonian
return self.kinetic
#----------------------------------------------------------------------------------------------------
def hamiltonian(self):
#calculation hamiltonian
return self.calculate_kinetic() + self.calculate_local(
) + self.calculate_nonlocal() + self.interaction
#----------------------------------------------------------------------------------------------------
def calculate_current(self, wfn):
return np.einsum('iqnm,qne,qme->i', self.moment, wfn.conj(),
wfn) / self.volume / self.nq
class HybridXC(HybridXCBase):
def __init__(self,
name,
hybrid=None,
xc=None,
finegrid=False,
unocc=False):
"""Mix standard functionals with exact exchange.
finegrid: boolean
Use fine grid for energy functional evaluations ?
unocc: boolean
Apply vxx also to unoccupied states ?
"""
self.finegrid = finegrid
self.unocc = unocc
HybridXCBase.__init__(self, name, hybrid, xc)
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, density, hamiltonian, wfs, occupations):
assert wfs.kd.gamma
self.xc.initialize(density, hamiltonian, wfs, occupations)
self.kpt_comm = wfs.kd.comm
self.nspins = wfs.nspins
self.setups = wfs.setups
self.density = density
self.kpt_u = wfs.kpt_u
self.exx_s = np.zeros(self.nspins)
self.ekin_s = np.zeros(self.nspins)
self.nocc_s = np.empty(self.nspins, int)
self.gd = density.gd
self.redistributor = density.redistributor
# XXX How do we construct a copy of the Poisson solver of the
# Hamiltonian? We don't know what class it is, etc., but gd
# may differ.
self.poissonsolver = PoissonSolver(eps=1e-11)
#self.poissonsolver = hamiltonian.poisson
if self.finegrid:
self.finegd = self.gd.refine()
# XXX Taking restrictor from Hamiltonian will not work in PW mode,
# will it? I think this supports only real-space mode.
#self.restrictor = hamiltonian.restrictor
self.restrictor = Transformer(self.finegd, self.gd, 3)
self.interpolator = Transformer(self.gd, self.finegd, 3)
else:
self.finegd = self.gd
self.ghat = LFC(self.finegd,
[setup.ghat_l for setup in density.setups],
integral=np.sqrt(4 * np.pi),
forces=True)
self.poissonsolver.set_grid_descriptor(self.finegd)
self.poissonsolver.initialize()
def set_positions(self, spos_ac):
self.ghat.set_positions(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)
# Note that the quantities passed are on the density/Hamiltonian grids!
# They may be distributed differently from own quantities.
self.ekin = self.kpt_comm.sum(self.ekin_s.sum())
return exc + self.kpt_comm.sum(self.exx_s.sum())
def calculate_exx(self):
for kpt in self.kpt_u:
self.apply_orbital_dependent_hamiltonian(kpt, kpt.psit_nG)
def apply_orbital_dependent_hamiltonian(self,
kpt,
psit_nG,
Htpsit_nG=None,
dH_asp=None):
if kpt.f_n is None:
return
deg = 2 // self.nspins # Spin degeneracy
hybrid = self.hybrid
P_ani = kpt.P_ani
setups = self.setups
vt_g = self.finegd.empty()
if self.gd is not self.finegd:
vt_G = self.gd.empty()
nocc = int(kpt.f_n.sum()) // (3 - self.nspins)
if self.unocc:
nbands = len(kpt.f_n)
else:
nbands = nocc
self.nocc_s[kpt.s] = nocc
if Htpsit_nG is not None:
kpt.vt_nG = self.gd.empty(nbands)
kpt.vxx_ani = {}
kpt.vxx_anii = {}
for a, P_ni in P_ani.items():
I = P_ni.shape[1]
kpt.vxx_ani[a] = np.zeros((nbands, I))
kpt.vxx_anii[a] = np.zeros((nbands, I, I))
exx = 0.0
ekin = 0.0
# XXXX nbands can be different numbers on different cpus!
# That means some will execute the loop and others not.
# And deadlocks with augment-grids.
# Determine pseudo-exchange
for n1 in range(nbands):
psit1_G = psit_nG[n1]
f1 = kpt.f_n[n1] / deg
for n2 in range(n1, nbands):
psit2_G = psit_nG[n2]
f2 = kpt.f_n[n2] / deg
# Double count factor:
dc = (1 + (n1 != n2)) * deg
nt_G, rhot_g = self.calculate_pair_density(
n1, n2, psit_nG, P_ani)
vt_g[:] = 0.0
# XXXXX This will go wrong because we are solving the
# Poisson equation on the distribution of gd, not finegd
# Or maybe it's fixed now
self.poissonsolver.solve(vt_g,
-rhot_g,
charge=-float(n1 == n2),
eps=1e-12,
zero_initial_phi=True)
vt_g *= hybrid
if self.gd is self.finegd:
vt_G = vt_g
else:
self.restrictor.apply(vt_g, vt_G)
# Integrate the potential on fine and coarse grids
int_fine = self.finegd.integrate(vt_g * rhot_g)
int_coarse = self.gd.integrate(vt_G * nt_G)
if self.gd.comm.rank == 0: # only add to energy on master CPU
exx += 0.5 * dc * f1 * f2 * int_fine
ekin -= dc * f1 * f2 * int_coarse
if Htpsit_nG is not None:
Htpsit_nG[n1] += f2 * vt_G * psit2_G
if n1 == n2:
kpt.vt_nG[n1] = f1 * vt_G
else:
Htpsit_nG[n2] += f1 * vt_G * psit1_G
# Update the vxx_uni and vxx_unii vectors of the nuclei,
# used to determine the atomic hamiltonian, and the
# residuals
v_aL = self.ghat.dict()
self.ghat.integrate(vt_g, v_aL)
for a, v_L in v_aL.items():
v_ii = unpack(np.dot(setups[a].Delta_pL, v_L))
v_ni = kpt.vxx_ani[a]
v_nii = kpt.vxx_anii[a]
P_ni = P_ani[a]
v_ni[n1] += f2 * np.dot(v_ii, P_ni[n2])
if n1 != n2:
v_ni[n2] += f1 * np.dot(v_ii, P_ni[n1])
else:
# XXX Check this:
v_nii[n1] = f1 * v_ii
# Apply the atomic corrections to the energy and the Hamiltonian matrix
for a, P_ni in P_ani.items():
setup = setups[a]
if Htpsit_nG is not None:
# Add non-trivial corrections the Hamiltonian matrix
h_nn = symmetrize(
np.inner(P_ni[:nbands], kpt.vxx_ani[a][:nbands]))
ekin -= np.dot(kpt.f_n[:nbands], h_nn.diagonal())
dH_p = dH_asp[a][kpt.s]
# Get atomic density and Hamiltonian matrices
D_p = self.density.D_asp[a][kpt.s]
D_ii = unpack2(D_p)
ni = len(D_ii)
# Add atomic corrections to the valence-valence exchange energy
# --
# > D C D
# -- ii iiii 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]
p12 = packed_index(i1, i2, ni)
if Htpsit_nG is not None:
dH_p[p12] -= 2 * hybrid / deg * A / ((i1 != i2) + 1)
ekin += 2 * hybrid / deg * D_ii[i1, i2] * A
exx -= hybrid / deg * D_ii[i1, i2] * A
# Add valence-core exchange energy
# --
# > X D
# -- ii ii
if setup.X_p is not None:
exx -= hybrid * np.dot(D_p, setup.X_p)
if Htpsit_nG is not None:
dH_p -= hybrid * setup.X_p
ekin += hybrid * np.dot(D_p, setup.X_p)
# Add core-core exchange energy
if kpt.s == 0:
exx += hybrid * setup.ExxC
self.exx_s[kpt.s] = self.gd.comm.sum(exx)
self.ekin_s[kpt.s] = self.gd.comm.sum(ekin)
def correct_hamiltonian_matrix(self, kpt, H_nn):
if not hasattr(kpt, 'vxx_ani'):
return
if self.gd.comm.rank > 0:
H_nn[:] = 0.0
nocc = self.nocc_s[kpt.s]
nbands = len(kpt.vt_nG)
for a, P_ni in kpt.P_ani.items():
H_nn[:nbands, :nbands] += symmetrize(
np.inner(P_ni[:nbands], kpt.vxx_ani[a]))
self.gd.comm.sum(H_nn)
H_nn[:nocc, nocc:] = 0.0
H_nn[nocc:, :nocc] = 0.0
def calculate_pair_density(self, n1, n2, psit_nG, P_ani):
Q_aL = {}
for a, P_ni in P_ani.items():
P1_i = P_ni[n1]
P2_i = P_ni[n2]
D_ii = np.outer(P1_i, P2_i.conj()).real
D_p = pack(D_ii)
Q_aL[a] = np.dot(D_p, self.setups[a].Delta_pL)
nt_G = psit_nG[n1] * psit_nG[n2]
if self.finegd is self.gd:
nt_g = nt_G
else:
nt_g = self.finegd.empty()
self.interpolator.apply(nt_G, nt_g)
rhot_g = nt_g.copy()
self.ghat.add(rhot_g, Q_aL)
return nt_G, rhot_g
def add_correction(self,
kpt,
psit_xG,
Htpsit_xG,
P_axi,
c_axi,
n_x,
calculate_change=False):
if kpt.f_n is None:
return
nocc = self.nocc_s[kpt.s]
if calculate_change:
for x, n in enumerate(n_x):
if n < nocc:
Htpsit_xG[x] += kpt.vt_nG[n] * psit_xG[x]
for a, P_xi in P_axi.items():
c_axi[a][x] += np.dot(kpt.vxx_anii[a][n], P_xi[x])
else:
for a, c_xi in c_axi.items():
c_xi[:nocc] += kpt.vxx_ani[a][:nocc]
def rotate(self, kpt, U_nn):
if kpt.f_n is None:
return
nocc = self.nocc_s[kpt.s]
if len(kpt.vt_nG) == nocc:
U_nn = U_nn[:nocc, :nocc]
gemm(1.0, kpt.vt_nG.copy(), U_nn, 0.0, kpt.vt_nG)
for v_ni in kpt.vxx_ani.values():
gemm(1.0, v_ni.copy(), U_nn, 0.0, v_ni)
for v_nii in kpt.vxx_anii.values():
gemm(1.0, v_nii.copy(), U_nn, 0.0, v_nii)
class DensityFourierTransform(Observer):
def __init__(self, timestep, frequencies, width=None, interval=1):
"""
Parameters
----------
timestep: float
Time step in attoseconds (10^-18 s), e.g., 4.0 or 8.0
frequencies: NumPy array or list of floats
Frequencies in eV for Fourier transforms
width: float or None
Width of Gaussian envelope in eV, otherwise no envelope
interval: int
Number of timesteps between calls (used when attaching)
"""
Observer.__init__(self, interval)
self.timestep = interval * timestep * attosec_to_autime # autime
self.omega_w = np.asarray(frequencies) * eV_to_aufrequency # autime^(-1)
if width is None:
self.sigma = None
else:
self.sigma = width * eV_to_aufrequency # autime^(-1)
self.nw = len(self.omega_w)
self.dtype = complex # np.complex128 really, but hey...
self.Fnt_wsG = None
self.Fnt_wsg = None
self.Ant_sG = None
self.Ant_sg = None
def initialize(self, paw, allocate=True):
self.allocated = False
assert hasattr(paw, 'time') and hasattr(paw, 'niter'), 'Use TDDFT!'
self.time = paw.time
self.niter = paw.niter
self.world = paw.wfs.world
self.gd = paw.density.gd
self.finegd = paw.density.finegd
self.nspins = paw.density.nspins
self.stencil = paw.input_parameters.stencils[1] # i.e. tar['InterpolationStencil']
self.interpolator = paw.density.interpolator
self.cinterpolator = Transformer(self.gd, self.finegd, self.stencil, \
dtype=self.dtype, allocate=False)
self.phase_cd = np.ones((3, 2), dtype=complex)
self.Ant_sG = paw.density.nt_sG.copy() # TODO in allocate instead?
# Attach to PAW-type object
paw.attach(self, self.interval, density=paw.density)
if allocate:
self.allocate()
def allocate(self):
if not self.allocated:
self.Fnt_wsG = self.gd.zeros((self.nw, self.nspins), \
dtype=self.dtype)
self.Fnt_wsg = None
#self.Ant_sG = ...
self.Ant_sg = None
self.gamma_w = np.ones(self.nw, dtype=complex) * self.timestep
self.cinterpolator.allocate()
self.allocated = True
if debug:
assert is_contiguous(self.Fnt_wsG, self.dtype)
def interpolate_fourier_transform(self):
if self.Fnt_wsg is None:
self.Fnt_wsg = self.finegd.empty((self.nw, self.nspins), \
dtype=self.dtype)
if self.dtype == float:
intapply = self.interpolator.apply
else:
intapply = lambda Fnt_G, Fnt_g: self.cinterpolator.apply(Fnt_G, \
Fnt_g, self.phase_cd)
for w in range(self.nw):
for s in range(self.nspins):
intapply(self.Fnt_wsG[w,s], self.Fnt_wsg[w,s])
def interpolate_average(self):
if self.Ant_sg is None:
self.Ant_sg = self.finegd.empty(self.nspins, dtype=float)
for s in range(self.nspins):
self.interpolator.apply(self.Ant_sG[s], self.Ant_sg[s])
def update(self, density):
# Update time
# t[N] = t[N-1] + dt[N-1] #TODO better time-convention?
self.time += self.timestep
# Complex exponential with/without finite-width envelope
f_w = np.exp(1.0j*self.omega_w*self.time)
if self.sigma is not None:
f_w *= np.exp(-self.time**2*self.sigma**2/2.0)
# Update Fourier transformed density components
# Fnt_wG[N] = Fnt_wG[N-1] + 1/sqrt(pi) * (nt_G[N]-avg_nt_G[N-1]) \
# * (f[N]*t[N] - gamma[N-1]) * dt[N]/(t[N]+dt[N])
for w in range(self.nw):
self.Fnt_wsG[w] += 1/np.pi**0.5 * (density.nt_sG - self.Ant_sG) \
* (f_w[w]*self.time - self.gamma_w[w]) * self.timestep \
/ (self.time + self.timestep)
# Update the cumulative phase factors
# gamma[N] = gamma[N-1] + f[N]*dt[N]
self.gamma_w += f_w * self.timestep
# If dt[N] = dt for all N and sigma = 0, then this simplifies to:
# gamma[N] = Sum_{n=0}^N exp(i*omega*n*dt) * dt
# = (1 - exp(i*omega*(N+1)*dt)) / (1 - exp(i*omega*dt)) * dt
# Update average density
# Ant_G[N] = (t[N]*Ant_G[N-1] + nt_G[N]*dt[N])/(t[N]+dt[N])
self.Ant_sG = (self.time*self.Ant_sG + density.nt_sG*self.timestep) \
/ (self.time + self.timestep)
def get_fourier_transform(self, frequency=0, spin=0, gridrefinement=1):
if gridrefinement == 1:
return self.Fnt_wsG[frequency, spin]
elif gridrefinement == 2:
if self.Fnt_wsg is None:
self.interpolate_fourier_transform()
return self.Fnt_wsg[frequency, spin]
else:
raise NotImplementedError('Arbitrary refinement not implemented')
def get_average(self, spin=0, gridrefinement=1):
if gridrefinement == 1:
return self.Ant_sG[spin]
elif gridrefinement == 2:
if self.Ant_sg is None:
self.interpolate_average()
return self.Ant_sg[spin]
else:
raise NotImplementedError('Arbitrary refinement not implemented')
def read(self, filename, idiotproof=True):
if idiotproof and not filename.endswith('.ftd'):
raise IOError('Filename must end with `.ftd`.')
tar = Reader(filename)
# Test data type
dtype = {'Float':float, 'Complex':complex}[tar['DataType']]
if dtype != self.dtype:
raise IOError('Data is an incompatible type.')
# Test time
time = tar['Time']
if idiotproof and abs(time-self.time) >= 1e-9:
raise IOError('Timestamp is incompatible with calculator.')
# Test timestep (non-critical)
timestep = tar['TimeStep']
if abs(timestep - self.timestep) > 1e-12:
print 'Warning: Time-step has been altered. (%lf -> %lf)' \
% (self.timestep, timestep)
self.timestep = timestep
# Test dimensions
nw = tar.dimension('nw')
nspins = tar.dimension('nspins')
ng = (tar.dimension('ngptsx'), tar.dimension('ngptsy'), \
tar.dimension('ngptsz'),)
if (nw != self.nw or nspins != self.nspins or
(ng != self.gd.get_size_of_global_array()).any()):
raise IOError('Data has incompatible shapes.')
# Test width (non-critical)
sigma = tar['Width']
if ((sigma is None)!=(self.sigma is None) or # float <-> None
(sigma is not None and self.sigma is not None and \
abs(sigma - self.sigma) > 1e-12)): # float -> float
print 'Warning: Width has been altered. (%s -> %s)' \
% (self.sigma, sigma)
self.sigma = sigma
# Read frequencies
self.omega_w[:] = tar.get('Frequency')
# Read cumulative phase factors
self.gamma_w[:] = tar.get('PhaseFactor')
# Read average densities on master and distribute
for s in range(self.nspins):
all_Ant_G = tar.get('Average', s)
self.gd.distribute(all_Ant_G, self.Ant_sG[s])
# Read fourier transforms on master and distribute
for w in range(self.nw):
for s in range(self.nspins):
all_Fnt_G = tar.get('FourierTransform', w, s)
self.gd.distribute(all_Fnt_G, self.Fnt_wsG[w,s])
# Close for good measure
tar.close()
def write(self, filename, idiotproof=True):
if idiotproof and not filename.endswith('.ftd'):
raise IOError('Filename must end with `.ftd`.')
master = self.world.rank == 0
# Open writer on master and set parameters/dimensions
if master:
tar = Writer(filename)
tar['DataType'] = {float:'Float', complex:'Complex'}[self.dtype]
tar['Time'] = self.time
tar['TimeStep'] = self.timestep #non-essential
tar['Width'] = self.sigma
tar.dimension('nw', self.nw)
tar.dimension('nspins', self.nspins)
# Create dimensions for varioius netCDF variables:
ng = self.gd.get_size_of_global_array()
tar.dimension('ngptsx', ng[0])
tar.dimension('ngptsy', ng[1])
tar.dimension('ngptsz', ng[2])
# Write frequencies
tar.add('Frequency', ('nw',), self.omega_w, dtype=float)
# Write cumulative phase factors
tar.add('PhaseFactor', ('nw',), self.gamma_w, dtype=self.dtype)
# Collect average densities on master and write
if master:
tar.add('Average', ('nspins', 'ngptsx', 'ngptsy',
'ngptsz', ), dtype=float)
for s in range(self.nspins):
big_Ant_G = self.gd.collect(self.Ant_sG[s])
if master:
tar.fill(big_Ant_G)
# Collect fourier transforms on master and write
if master:
tar.add('FourierTransform', ('nw', 'nspins', 'ngptsx', 'ngptsy', \
'ngptsz', ), dtype=self.dtype)
for w in range(self.nw):
for s in range(self.nspins):
big_Fnt_G = self.gd.collect(self.Fnt_wsG[w,s])
if master:
tar.fill(big_Fnt_G)
# Close to flush changes
if master:
tar.close()
# Make sure slaves don't return before master is done
self.world.barrier()
def dump(self, filename):
if debug:
assert is_contiguous(self.Fnt_wsG, self.dtype)
assert is_contiguous(self.Ant_sG, float)
all_Fnt_wsG = self.gd.collect(self.Fnt_wsG)
all_Ant_sG = self.gd.collect(self.Ant_sG)
if self.world.rank == 0:
all_Fnt_wsG.dump(filename)
all_Ant_sG.dump(filename+'_avg') # crude but easy
self.omega_w.dump(filename+'_omega') # crude but easy
self.gamma_w.dump(filename+'_gamma') # crude but easy
def load(self, filename):
if self.world.rank == 0:
all_Fnt_wsG = np.load(filename)
all_Ant_sG = np.load(filename+'_avg') # crude but easy
else:
all_Fnt_wsG = None
all_Ant_sG = None
if debug:
assert all_Fnt_wsG is None or is_contiguous(all_Fnt_wsG, self.dtype)
assert all_Ant_sG is None or is_contiguous(all_Ant_sG, float)
if not self.allocated:
self.allocate()
self.gd.distribute(all_Fnt_wsG, self.Fnt_wsG)
self.gd.distribute(all_Ant_sG, self.Ant_sG)
self.omega_w = np.load(filename+'_omega') # crude but easy
self.gamma_w = np.load(filename+'_gamma') # crude but easy
class RealSpaceDensity(Density):
def __init__(self, gd, finegd, nspins, charge, collinear=True,
stencil=3):
Density.__init__(self, gd, finegd, nspins, charge, collinear)
self.stencil = stencil
def initialize(self, setups, timer, magmom_av, hund):
Density.initialize(self, setups, timer, magmom_av, hund)
# Interpolation function for the density:
self.interpolator = Transformer(self.gd, self.finegd, self.stencil)
spline_aj = []
for setup in setups:
if setup.nct is None:
spline_aj.append([])
else:
spline_aj.append([setup.nct])
self.nct = LFC(self.gd, spline_aj,
integral=[setup.Nct for setup in setups],
forces=True, cut=True)
self.ghat = LFC(self.finegd, [setup.ghat_l for setup in setups],
integral=sqrt(4 * pi), forces=True)
def set_positions(self, spos_ac, rank_a=None):
Density.set_positions(self, spos_ac, rank_a)
self.nct_G = self.gd.zeros()
self.nct.add(self.nct_G, 1.0 / self.nspins)
def interpolate_pseudo_density(self, comp_charge=None):
"""Interpolate pseudo density to fine grid."""
if comp_charge is None:
comp_charge = self.calculate_multipole_moments()
self.nt_sg = self.interpolate(self.nt_sG, self.nt_sg)
# With periodic boundary conditions, the interpolation will
# conserve the number of electrons.
if not self.gd.pbc_c.all():
# With zero-boundary conditions in one or more directions,
# this is not the case.
pseudo_charge = -(self.charge + comp_charge)
if abs(pseudo_charge) > 1.0e-14:
x = (pseudo_charge /
self.finegd.integrate(self.nt_sg[:self.nspins]).sum())
self.nt_sg *= x
def interpolate(self, in_xR, out_xR=None):
"""Interpolate array(s)."""
# ndim will be 3 in finite-difference mode and 1 when working
# with the AtomPAW class (spherical atoms and 1d grids)
ndim = self.gd.ndim
if out_xR is None:
out_xR = self.finegd.empty(in_xR.shape[:-ndim])
a_xR = in_xR.reshape((-1,) + in_xR.shape[-ndim:])
b_xR = out_xR.reshape((-1,) + out_xR.shape[-ndim:])
for in_R, out_R in zip(a_xR, b_xR):
self.interpolator.apply(in_R, out_R)
return out_xR
def calculate_pseudo_charge(self):
self.nt_g = self.nt_sg[:self.nspins].sum(axis=0)
self.rhot_g = self.nt_g.copy()
self.ghat.add(self.rhot_g, self.Q_aL)
if debug:
charge = self.finegd.integrate(self.rhot_g) + self.charge
if abs(charge) > self.charge_eps:
raise RuntimeError('Charge not conserved: excess=%.9f' %
charge)
def get_pseudo_core_kinetic_energy_density_lfc(self):
return LFC(self.gd,
[[setup.tauct] for setup in self.setups],
forces=True, cut=True)
def calculate_dipole_moment(self):
return self.finegd.calculate_dipole_moment(self.rhot_g)
class SICSpin:
def __init__(self,
kpt,
xc,
density,
hamiltonian,
wfs,
poissonsolver,
ghat,
finegd,
dtype=float,
coulomb_factor=0.5,
xc_factor=0.5,
uominres=1E-1,
uomaxres=1E-10,
uorelres=1E-4,
uonscres=1E-10,
rattle=-0.1,
stabpot=0.0,
maxuoiter=10,
logging=2):
"""Single spin SIC object.
coulomb_factor:
Scaling factor for Hartree-functional
xc_factor:
Scaling factor for xc-functional
uominres:
Minimum residual before unitary optimization starts
uomaxres:
Target accuracy for unitary optimization
(absolute variance)
uorelres:
Target accuracy for unitary optimization
(rel. to basis residual)
maxuoiter:
Maximum number of unitary optimization steps
rattle:
perturbation to the initial states
"""
self.wfs = wfs
self.kpt = kpt
self.xc = xc
self.poissonsolver = poissonsolver
self.ghat = ghat
self.pt = wfs.pt
self.gd = wfs.gd
self.finegd = finegd
if self.finegd is self.gd:
self.interpolator = None
self.restrictor = None
else:
self.interpolator = Transformer(self.gd, self.finegd, 3)
self.restrictor = Transformer(self.finegd, self.gd, 3)
self.nspins = wfs.nspins
self.spin = kpt.s
self.timer = wfs.timer
self.setups = wfs.setups
self.dtype = dtype
self.coulomb_factor = coulomb_factor
self.xc_factor = xc_factor
self.nocc = None # number of occupied states
self.W_mn = None # unit. transf. to energy optimal states
self.initial_W_mn = None # initial unitary transformation
self.vt_mG = None # orbital dependent potentials
self.exc_m = None # PZ-SIC contributions (from E_xc)
self.ecoulomb_m = None # PZ-SIC contributions (from E_H)
self.rattle = rattle # perturb the initial unitary transformation
self.stabpot = stabpot # stabilizing constant potential to avoid
# occupation of unoccupied states
self.uominres = uominres
self.uomaxres = uomaxres
self.uorelres = uorelres
self.uonscres = uonscres
self.maxuoiter = maxuoiter
self.maxlsiter = 1 # maximum number of line-search steps
self.maxcgiter = 2 # maximum number of CG-iterations
self.lsinterp = True # interpolate for minimum during line search
self.basiserror = 1E+20
self.logging = logging
def initialize_orbitals(self, rattle=-0.1, localize=True):
if self.initial_W_mn is not None:
self.nocc = self.initial_W_mn.shape[0]
else:
self.nocc, x = divmod(int(self.kpt.f_n.sum()), 3 - self.nspins)
assert x == 0
if self.nocc == 0:
return
Z_mmv = np.empty((self.nocc, self.nocc, 3), complex)
for v in range(3):
G_v = np.zeros(3)
G_v[v] = 1
Z_mmv[:, :,
v] = self.gd.wannier_matrix(self.kpt.psit_nG,
self.kpt.psit_nG, G_v, self.nocc)
self.finegd.comm.sum(Z_mmv)
if self.initial_W_mn is not None:
self.W_mn = self.initial_W_mn
elif localize:
W_nm = np.identity(self.nocc)
localization = 0.0
for iter in range(30):
loc = _gpaw.localize(Z_mmv, W_nm)
if loc - localization < 1e-6:
break
localization = loc
self.W_mn = W_nm.T.copy()
else:
self.W_mn = np.identity(self.nocc)
if (rattle != 0.0 and self.W_mn is not None
and self.initial_W_mn is None):
U_mm = random_unitary_matrix(rattle, self.nocc)
self.W_mn = np.dot(U_mm, self.W_mn)
if self.W_mn is not None:
self.finegd.comm.broadcast(self.W_mn, 0)
spos_mc = -np.angle(Z_mmv.diagonal()).T / (2 * pi)
self.initial_pos_mv = np.dot(spos_mc % 1.0, self.gd.cell_cv)
def localize_orbitals(self):
assert self.gd.orthogonal
# calculate wannier matrixelements
Z_mmv = np.empty((self.nocc, self.nocc, 3), complex)
for v in range(3):
G_v = np.zeros(3)
G_v[v] = 1
Z_mmv[:, :,
v] = self.gd.wannier_matrix(self.kpt.psit_nG,
self.kpt.psit_nG, G_v, self.nocc)
self.finegd.comm.sum(Z_mmv)
# setup the initial configuration (identity)
W_nm = np.identity(self.nocc)
# localize the orbitals
localization = 0.0
for iter in range(30):
loc = _gpaw.localize(Z_mmv, W_nm)
if loc - localization < 1e-6:
break
localization = loc
# apply localizing transformation
self.W_mn = W_nm.T.copy()
def rattle_orbitals(self, rattle=-0.1):
# check for the trivial cases
if rattle == 0.0:
return
if self.W_mn is None:
return
# setup a "random" unitary matrix
nocc = self.W_mn.shape[0]
U_mm = random_unitary_matrix(rattle, nocc)
# apply unitary transformation
self.W_mn = np.dot(U_mm, self.W_mn)
def get_centers(self):
assert self.gd.orthogonal
# calculate energy optimal states (if necessary)
if self.phit_mG is None:
self.update_optimal_states()
# calculate wannier matrixelements
Z_mmv = np.empty((self.nocc, self.nocc, 3), complex)
for v in range(3):
G_v = np.zeros(3)
G_v[v] = 1
Z_mmv[:, :, v] = self.gd.wannier_matrix(self.phit_mG, self.phit_mG,
G_v, self.nocc)
self.finegd.comm.sum(Z_mmv)
# calculate positions of localized orbitals
spos_mc = -np.angle(Z_mmv.diagonal()).T / (2 * pi)
return np.dot(spos_mc % 1.0, self.gd.cell_cv) * Bohr
def calculate_sic_matrixelements(self):
# overlap of pseudo wavefunctions
Htphit_mG = self.vt_mG * self.phit_mG
V_mm = np.zeros((self.nocc, self.nocc), dtype=self.dtype)
gemm(self.gd.dv, self.phit_mG, Htphit_mG, 0.0, V_mm, 't')
# PAW
for a, P_mi in self.P_ami.items():
for m, dH_p in enumerate(self.dH_amp[a]):
dH_ii = unpack(dH_p)
V_mm[m, :] += np.dot(P_mi[m], np.dot(dH_ii, P_mi.T))
# accumulate over grid-domains
self.finegd.comm.sum(V_mm)
self.V_mm = V_mm
# Symmetrization of V and kappa-matrix:
K_mm = 0.5 * (V_mm - V_mm.T.conj())
V_mm = 0.5 * (V_mm + V_mm.T.conj())
# evaluate the kinetic correction
self.ekin = -np.trace(V_mm) * (3 - self.nspins)
return V_mm, K_mm, np.vdot(K_mm, K_mm).real
def update_optimal_states(self):
# pseudo wavefunctions
self.phit_mG = self.gd.zeros(self.nocc)
if self.nocc > 0:
gemm(1.0, self.kpt.psit_nG[:self.nocc], self.W_mn, 0.0,
self.phit_mG)
# PAW
self.P_ami = {}
for a, P_ni in self.kpt.P_ani.items():
self.P_ami[a] = np.dot(self.W_mn, P_ni[:self.nocc])
def calculate_density(self, m):
# pseudo density
nt_G = self.phit_mG[m]**2
if self.finegd is self.gd:
nt_g = nt_G
else:
nt_g = self.finegd.empty()
self.interpolator.apply(nt_G, nt_g)
# normalize single-particle density
nt_g *= self.gd.integrate(nt_G) / self.finegd.integrate(nt_g)
# PAW corrections
Q_aL = {}
D_ap = {}
for a, P_mi in self.P_ami.items():
P_i = P_mi[m]
D_ii = np.outer(P_i, P_i.conj()).real
D_ap[a] = D_p = pack(D_ii)
Q_aL[a] = np.dot(D_p, self.setups[a].Delta_pL)
return nt_g, Q_aL, D_ap
def update_potentials(self, save=False, restore=False):
if restore:
self.exc_m = self.exc_save_m
self.ecoulomb_m = self.eco_save_m
self.esic = self.esic_save
self.vt_mG = self.vt_save_mG.copy()
self.dH_amp = self.dH_save_amp.copy()
return
self.timer.start('ODD-potentials')
nt_sg = self.finegd.empty(2)
nt_sg[1] = 0.0
vt_sg = self.finegd.empty(2)
# PAW
W_aL = self.ghat.dict()
zero_initial_phi = False
# initialize some bigger fields
if self.vt_mG is None or self.nocc != self.phit_mG.shape[0]:
self.vt_mG = self.gd.empty(self.nocc)
self.exc_m = np.zeros(self.nocc)
self.ecoulomb_m = np.zeros(self.nocc)
self.vHt_mg = self.finegd.zeros(self.nocc)
zero_initial_phi = True
#
# PAW
self.dH_amp = {}
for a, P_mi in self.P_ami.items():
ni = P_mi.shape[1]
self.dH_amp[a] = np.empty((self.nocc, ni * (ni + 1) // 2))
#
self.Q_maL = {}
# loop all occupied orbitals
for m, phit_G in enumerate(self.phit_mG):
#
# setup the single-particle density and PAW density-matrix
nt_sg[0], Q_aL, D_ap = self.calculate_density(m)
vt_sg[:] = 0.0
#
# xc-SIC
self.timer.start('XC')
if self.xc_factor != 0.0:
exc = self.xc.calculate(self.finegd, nt_sg, vt_sg)
exc /= self.finegd.comm.size
vt_sg[0] *= -self.xc_factor
#
# PAW
for a, D_p in D_ap.items():
setup = self.setups[a]
dH_p = self.dH_amp[a][m]
dH_sp = np.zeros((2, len(dH_p)))
#
D_sp = np.array([D_p, np.zeros_like(D_p)])
exc += self.xc.calculate_paw_correction(
setup, D_sp, dH_sp, addcoredensity=False)
dH_p[:] = -dH_sp[0] * self.xc_factor
self.exc_m[m] = -self.xc_factor * exc
self.timer.stop('XC')
#
# Hartree-SIC
self.timer.start('Hartree')
if self.coulomb_factor != 0.0:
#
# add compensation charges to pseudo density
self.ghat.add(nt_sg[0], Q_aL)
#
# solve the coulomb problem
self.poissonsolver.solve(self.vHt_mg[m],
nt_sg[0],
zero_initial_phi=zero_initial_phi)
ecoulomb = 0.5 * self.finegd.integrate(
nt_sg[0] * self.vHt_mg[m])
ecoulomb /= self.finegd.comm.size
vt_sg[0] -= self.coulomb_factor * self.vHt_mg[m]
#
# PAW
self.ghat.integrate(self.vHt_mg[m], W_aL)
for a, D_p in D_ap.items():
setup = self.setups[a]
dH_p = self.dH_amp[a][m]
M_p = np.dot(setup.M_pp, D_p)
ecoulomb += np.dot(D_p, M_p)
#
dH_p -= self.coulomb_factor * (
2.0 * M_p + np.dot(setup.Delta_pL, W_aL[a]))
#
self.ecoulomb_m[m] = -self.coulomb_factor * ecoulomb
self.timer.stop('Hartree')
# restrict to course grid
if self.finegd is self.gd:
self.vt_mG[m] = vt_sg[0]
else:
self.timer.start('Restrictor')
self.restrictor.apply(vt_sg[0], self.vt_mG[m])
self.timer.stop('Restrictor')
self.Q_maL[m] = Q_aL
self.timer.stop('ODD-potentials')
# accumulate total xc-SIC and coulomb-SIC
self.finegd.comm.sum(self.exc_m)
self.finegd.comm.sum(self.ecoulomb_m)
# total sic (including spin-degeneracy)
self.esic = self.exc_m.sum()
self.esic += self.ecoulomb_m.sum()
self.esic *= (3 - self.nspins)
if save:
self.exc_save_m = self.exc_m
self.eco_save_m = self.ecoulomb_m
self.esic_save = self.esic
self.vt_save_mG = self.vt_mG.copy()
self.dH_save_amp = self.dH_amp.copy()
def apply_orbital_dependent_hamiltonian(self, psit_nG):
"""...
Setup::
|V phi_m> and <l|Vphi_m>,
for occupied states m and unoccupied states l."""
# nocc = self.nocc
# nvirt = psit_nG.shape[0] - nocc
self.Htphit_mG = self.vt_mG * self.phit_mG
def correct_hamiltonian_matrix(self, H_nn):
""" Add contributions of the non-local part of the
interaction potential to the Hamiltonian matrix.
on entry:
H_nn[n,m] = <n|H_{KS}|m>
on exit:
H_nn[n,m] = <n|H_{KS} + V_{u}|m>
where V_u is the unified Hamiltonian
V_u = ...
"""
nocc = self.nocc
nvirt = H_nn.shape[0] - nocc
W_mn = self.W_mn
# R_mk = self.R_mk
if self.gd.comm.rank == 0:
V_mm = 0.5 * (self.V_mm + self.V_mm.T)
H_nn[:nocc, :nocc] += np.dot(W_mn.T, np.dot(V_mm, W_mn))
if self.stabpot != 0.0:
H_nn[nocc:, nocc:] += np.eye(nvirt) * self.stabpot
if nvirt != 0:
H_nn[:nocc, nocc:] = 0.0 # R_nk
H_nn[nocc:, :nocc] = 0.0 # R_nk.T
# R_nk = np.dot(W_mn.T, R_mk) # CHECK THIS
# H_nn[:nocc, nocc:] += R_nk
# H_nn[nocc:, :nocc] += R_nk.T
def calculate_residual(self, psit_nG, Htpsit_nG, P_ani, c_ani):
""" Calculate the action of the unified Hamiltonian on an
arbitrary state:
H_u|Psi> =
"""
nocc = self.nocc
nvirt = psit_nG.shape[0] - nocc
# constraint for unoccupied states
R_mk = np.zeros((nocc, nvirt), dtype=self.dtype)
if nvirt > 0:
gemm(self.gd.dv, psit_nG[nocc:], self.Htphit_mG, 0.0, R_mk, 't')
# PAW
for a, P_mi in self.P_ami.items():
P_ni = P_ani[a]
for m, dH_p in enumerate(self.dH_amp[a]):
dH_ii = unpack(dH_p)
R_mk[m] += np.dot(P_mi[m], np.dot(dH_ii, P_ni[nocc:].T))
self.finegd.comm.sum(R_mk)
# self.R_mk = R_mk
# R_mk = self.R_mk
W_mn = self.W_mn
Htphit_mG = self.Htphit_mG
phit_mG = self.phit_mG
K_mm = 0.5 * (self.V_mm - self.V_mm.T)
Q_mn = np.dot(K_mm, W_mn)
# Action of unified Hamiltonian on occupied states:
if nocc > 0:
gemm(1.0, Htphit_mG, W_mn.T.copy(), 1.0, Htpsit_nG[:nocc])
gemm(1.0, phit_mG, Q_mn.T.copy(), 1.0, Htpsit_nG[:nocc])
if nvirt > 0:
gemm(1.0, phit_mG, R_mk.T.copy(), 1.0, Htpsit_nG[nocc:])
if self.stabpot != 0.0:
Htpsit_nG[nocc:] += self.stabpot * psit_nG[nocc:]
# PAW
for a, P_mi in self.P_ami.items():
#
c_ni = c_ani[a]
ct_mi = P_mi.copy()
#
dO_ii = self.setups[a].dO_ii
c_ni[:nocc] += np.dot(Q_mn.T, np.dot(P_mi, dO_ii))
c_ni[nocc:] += np.dot(R_mk.T, np.dot(P_mi, dO_ii))
#
for m, dH_p in enumerate(self.dH_amp[a]):
dH_ii = unpack(dH_p)
ct_mi[m] = np.dot(P_mi[m], dH_ii)
c_ni[:nocc] += np.dot(W_mn.T, ct_mi)
c_ni[nocc:] += self.stabpot * np.dot(P_ani[a][nocc:], dO_ii)
def calculate_residual_change(self, psit_xG, Htpsit_xG, P_axi, c_axi, n_x):
"""
"""
assert len(n_x) == 1
Htphit_mG = self.Htphit_mG
phit_mG = self.phit_mG
w_mx = np.zeros((self.nocc, 1), dtype=self.dtype)
v_mx = np.zeros((self.nocc, 1), dtype=self.dtype)
gemm(self.gd.dv, psit_xG, phit_mG, 0.0, w_mx, 't')
gemm(self.gd.dv, psit_xG, Htphit_mG, 0.0, v_mx, 't')
# PAW
for a, P_mi in self.P_ami.items():
P_xi = P_axi[a]
dO_ii = self.setups[a].dO_ii
#
w_mx += np.dot(P_mi, np.dot(dO_ii, P_xi.T))
for m, dH_p in enumerate(self.dH_amp[a]):
dH_ii = unpack(dH_p)
v_mx[m] += np.dot(P_mi[m], np.dot(dH_ii, P_xi.T))
# sum over grid-domains
self.finegd.comm.sum(w_mx)
self.finegd.comm.sum(v_mx)
V_mm = 0.5 * (self.V_mm + self.V_mm.T)
q_mx = v_mx - np.dot(V_mm, w_mx)
if self.stabpot != 0.0:
q_mx -= self.stabpot * w_mx
gemm(1.0, Htphit_mG, w_mx.T.copy(), 1.0, Htpsit_xG)
gemm(1.0, phit_mG, q_mx.T.copy(), 1.0, Htpsit_xG)
# PAW
for a, P_mi in self.P_ami.items():
c_xi = c_axi[a]
ct_mi = P_mi.copy()
dO_ii = self.setups[a].dO_ii
c_xi += np.dot(q_mx.T, np.dot(P_mi, dO_ii))
for m, dH_p in enumerate(self.dH_amp[a]):
dH_ii = unpack(dH_p)
ct_mi[m] = np.dot(P_mi[m], dH_ii)
c_xi += np.dot(w_mx.T, ct_mi)
if self.stabpot != 0.0:
Htphit_mG += self.stabpot * psit_xG
for a, P_xi in P_axi.items():
dO_ii = self.setups[a].dO_ii
c_axi[a] += self.stabpot * np.dot(P_xi, dO_ii)
def rotate(self, U_nn):
""" Unitary transformations amongst the canonic states
require to apply a counter-acting transformation to
the energy optimal states. This subroutine takes
care of it.
Reorthogonalization is required whenever unoccupied
states are mixed in.
"""
# skip if no transformation to optimal states is set-up
if self.W_mn is None:
return
# compensate the transformation amongst the occupied states
self.W_mn = np.dot(self.W_mn, U_nn[:self.nocc, :self.nocc])
# reorthogonalize if unoccupied states may have been mixed in
if self.nocc != U_nn.shape[0]:
self.W_mn = ortho(self.W_mn)
# self.R_mk = np.dot(self.R_mk, U_nn[self.nocc:, self.nocc:].T)
def add_forces(self, F_av):
# Calculate changes in projections
deg = 3 - self.nspins
F_amiv = self.pt.dict(self.nocc, derivative=True)
self.pt.derivative(self.phit_mG, F_amiv)
for m in range(self.nocc):
# Force from compensation charges:
dF_aLv = self.ghat.dict(derivative=True)
self.ghat.derivative(self.vHt_mg[m], dF_aLv)
for a, dF_Lv in dF_aLv.items():
F_av[a] -= deg * self.coulomb_factor * \
np.dot(self.Q_maL[m][a], dF_Lv)
# Force from projectors
for a, F_miv in F_amiv.items():
F_vi = F_miv[m].T.conj()
dH_ii = unpack(self.dH_amp[a][m])
P_i = self.P_ami[a][m]
F_v = np.dot(np.dot(F_vi, dH_ii), P_i)
F_av[a] += deg * 2 * F_v.real
def calculate(self):
""" Evaluate the non-unitary invariant part of the
energy functional and returns
esic: float
self-interaction energy
ekin: float
correction to the kinetic energy
"""
# initialize transformation from canonic to energy
# optimal states (if necessary)
if self.W_mn is None:
self.initialize_orbitals(rattle=self.rattle)
# optimize the non-unitary invariant part of the
# functional
self.unitary_optimization()
return self.esic, self.ekin
def unitary_optimization(self):
""" Optimization of the non-unitary invariant part of the
energy functional.
"""
optstep = 0.0
Gold = 0.0
cgiter = 0
#
epsstep = 0.005 # 0.005
dltstep = 0.1 # 0.1
prec = 1E-7
# get the initial ODD potentials/energy/matrixelements
self.update_optimal_states()
self.update_potentials(save=True)
ESI = self.esic
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
if norm < self.uonscres and self.maxuoiter > 0:
return
if self.nocc <= 1:
return
# optimize the unitary transformation
#
# allocate arrays for the search direction,
# i.e., the (conjugate) gradient
D_old_mm = np.zeros_like(self.W_mn)
for iter in range(abs(self.maxuoiter)):
# copy the initial unitary transformation and orbital
# dependent energies
W_old_mn = self.W_mn.copy()
# setup the steepest-descent/conjugate gradient
# D_nn: search direction
# K_nn: inverse gradient
# G0 : <K,D> (projected length of D along K)
if Gold != 0.0:
# conjugate gradient
G0 = np.sum(K_mm * K_mm.conj()).real
beta = G0 / Gold
Gold = G0
D_mm = K_mm + beta * D_old_mm
G0 = np.sum(K_mm * D_mm.conj()).real
else:
# steepest-descent
G0 = np.sum(K_mm * K_mm.conj()).real
Gold = G0
D_mm = K_mm
updated = False
minimum = False
failed = True
noise = False
E0 = ESI
# try to estimate optimal step-length from change in length
# of the gradient (force-only)
if (epsstep != 0.0 and norm > self.uomaxres):
step = epsstep
while (True):
U_mm = matrix_exponential(D_mm, step)
self.W_mn = np.dot(U_mm, W_old_mn)
self.update_optimal_states()
self.update_potentials()
E1 = self.esic
K0_mm = K_mm.copy()
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
# projected length of the gradient at the new position
G1 = np.sum(((K_mm - K0_mm) / step) * D_mm.conj()).real
#
if (abs(E1 - E0) < prec and E1 >= E0):
#
eps_works = True
Eeps = E1
noise = True
elif (E1 < E0):
#
# trial step reduced energy
eps_works = True
Eeps = E1
else:
#
# epsilon step did not work
eps_works = False
optstep = 0.0
break
# compute the optimal step size
# optstep = step*G0/(G0-G1)
# print -G0/G1
optstep = -G0 / G1
if (eps_works):
break
# print eps_works, optstep, G0/((G0-G1)/step)
# decide on the method for stepping
if (optstep > 0.0):
# convex region -> force only estimate for minimum
U_mm = matrix_exponential(D_mm, optstep)
self.W_mn = np.dot(U_mm, W_old_mn)
self.update_optimal_states()
self.update_potentials()
E1 = self.esic
if (abs(E1 - E0) < prec and E1 >= E0):
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
ESI = E1
optstep = optstep
lsiter = 0
maxlsiter = -1
updated = True
minimum = True
failed = False
lsmethod = 'CV-N'
noise = True
elif (E1 < E0):
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
ESI = E1
optstep = optstep
lsiter = 0
maxlsiter = -1
updated = True
minimum = True
failed = False
lsmethod = 'CV-S'
else:
# self.K_unn[q] = K_nn
ESI = E0
step = optstep
optstep = 0.0
lsiter = 0
maxlsiter = self.maxlsiter
updated = False
minimum = False
failed = True
lsmethod = 'CV-F-CC'
else:
# self.K_unn[q] = K_nn
ESI = E0
step = optstep
optstep = 0.0
lsiter = 0
maxlsiter = self.maxlsiter
updated = False
minimum = False
failed = True
lsmethod = 'CC'
else:
maxlsiter = 0
lsiter = -1
optstep = epsstep
updated = False
minimum = True
failed = False
lsmethod = 'CC-EPS'
if (optstep == 0.0):
#
# we are in the concave region or force-only estimate failed,
# just follow the (conjugate) gradient
step = dltstep * abs(step)
U_mm = matrix_exponential(D_mm, step)
self.W_mn = np.dot(U_mm, W_old_mn)
self.update_optimal_states()
self.update_potentials()
E1 = self.esic
#
#
if (abs(E1 - E0) < prec and E1 >= E0):
ESI = E1
optstep = 0.0
updated = False
minimum = True
failed = True
lsmethod = lsmethod + '-DLT-N'
noise = True
maxlsiter = -1
elif (E1 < E0):
ESI = E1
optstep = step
updated = True
minimum = False
failed = False
lsmethod = lsmethod + '-DLT'
maxlsiter = self.maxlsiter
elif (eps_works):
ESI = Eeps
E1 = Eeps
step = epsstep
updated = False
minimum = False
failed = False
lsmethod = lsmethod + '-EPS'
maxlsiter = self.maxlsiter
else:
optstep = 0.0
updated = False
minimum = False
failed = True
lsmethod = lsmethod + '-EPS-F'
maxlsiter = -1
#
G = (E1 - E0) / step
step0 = 0.0
step1 = step
step2 = 2 * step
#
for lsiter in range(maxlsiter):
#
# energy at the new position
U_mm = matrix_exponential(D_mm, step2)
self.W_mn = np.dot(U_mm, W_old_mn)
self.update_optimal_states()
self.update_potentials()
E2 = self.esic
G = (E2 - E1) / (step2 - step1)
#
#
if (G > 0.0):
if self.lsinterp:
a = (E0 / ((step2 - step0) * (step1 - step0)) +
E2 / ((step2 - step1) * (step2 - step0)) -
E1 / ((step2 - step1) * (step1 - step0)))
b = (E2 - E0) / (step2 - step0) - a * (step2 +
step0)
if (a < step**2):
optstep = 0.5 * (step0 + step2)
else:
optstep = -0.5 * b / a
updated = False
minimum = True
break
else:
optstep = step1
updated = False
minimum = True
break
elif (G < 0.0):
optstep = step2
step0 = step1
step1 = step2
step2 = step2 + step
E0 = E1
E1 = E2
ESI = E2
updated = True
minimum = False
if (cgiter != 0):
lsmethod = lsmethod + ' CG'
if (cgiter >= self.maxcgiter or not minimum):
Gold = 0.0
cgiter = 0
else:
cgiter = cgiter + 1
D_old_mm[:, :] = D_mm[:, :]
# update the energy and matrixelements of V and Kappa
# and accumulate total residual of unitary optimization
if (not updated):
if optstep > 0.0:
U_mm = matrix_exponential(D_mm, optstep)
self.W_mn = np.dot(U_mm, W_old_mn)
self.update_optimal_states()
self.update_potentials()
ESI = self.esic
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
else:
self.W_mn = W_old_mn
self.update_optimal_states()
self.update_potentials(restore=True)
ESI = self.esic
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
if (lsiter == maxlsiter - 1):
V_mm, K_mm, norm = self.calculate_sic_matrixelements()
E0 = ESI
# orthonormalize the energy optimal orbitals
self.W_mn = ortho(self.W_mn)
K = max(norm, 1.0e-16)
if self.finegd.comm.rank == 0:
if self.logging == 1:
print(" UO-%d: %2d %5.1f %20.5f " %
(self.spin, iter, np.log10(K), ESI * Hartree))
elif self.logging == 2:
print(" UO-%d: %2d %5.1f %20.5f " %
(self.spin, iter, np.log10(K), ESI * Hartree) +
lsmethod)
if ((K < self.uomaxres
or K < self.wfs.eigensolver.error * self.uorelres) or noise
or failed) and not self.maxuoiter < 0:
break
class DensityFourierTransform(Observer):
def __init__(self, timestep, frequencies, width=None, interval=1):
"""
Parameters
timestep: float
Time step in attoseconds (10^-18 s), e.g., 4.0 or 8.0
frequencies: NumPy array or list of floats
Frequencies in eV for Fourier transforms
width: float or None
Width of Gaussian envelope in eV, otherwise no envelope
interval: int
Number of timesteps between calls (used when attaching)
"""
Observer.__init__(self, interval)
self.timestep = interval * timestep * attosec_to_autime # autime
self.omega_w = np.asarray(
frequencies) * eV_to_aufrequency # autime^(-1)
if width is None:
self.sigma = None
else:
self.sigma = width * eV_to_aufrequency # autime^(-1)
self.nw = len(self.omega_w)
self.dtype = complex # np.complex128 really, but hey...
self.Fnt_wsG = None
self.Fnt_wsg = None
self.Ant_sG = None
self.Ant_sg = None
def initialize(self, paw, allocate=True):
self.allocated = False
assert hasattr(paw, 'time') and hasattr(paw, 'niter'), 'Use TDDFT!'
self.time = paw.time
self.niter = paw.niter
self.world = paw.wfs.world
self.gd = paw.density.gd
self.finegd = paw.density.finegd
self.nspins = paw.density.nspins
self.stencil = paw.input_parameters.stencils[
1] # i.e. tar['InterpolationStencil']
self.interpolator = paw.density.interpolator
self.cinterpolator = Transformer(self.gd, self.finegd, self.stencil, \
dtype=self.dtype)
self.phase_cd = np.ones((3, 2), dtype=complex)
self.Ant_sG = paw.density.nt_sG.copy() # TODO in allocate instead?
# Attach to PAW-type object
paw.attach(self, self.interval, density=paw.density)
if allocate:
self.allocate()
def allocate(self):
if not self.allocated:
self.Fnt_wsG = self.gd.zeros((self.nw, self.nspins), \
dtype=self.dtype)
self.Fnt_wsg = None
#self.Ant_sG = ...
self.Ant_sg = None
self.gamma_w = np.ones(self.nw, dtype=complex) * self.timestep
self.allocated = True
if debug:
assert is_contiguous(self.Fnt_wsG, self.dtype)
def interpolate_fourier_transform(self):
if self.Fnt_wsg is None:
self.Fnt_wsg = self.finegd.empty((self.nw, self.nspins), \
dtype=self.dtype)
if self.dtype == float:
intapply = self.interpolator.apply
else:
intapply = lambda Fnt_G, Fnt_g: self.cinterpolator.apply(Fnt_G, \
Fnt_g, self.phase_cd)
for w in range(self.nw):
for s in range(self.nspins):
intapply(self.Fnt_wsG[w, s], self.Fnt_wsg[w, s])
def interpolate_average(self):
if self.Ant_sg is None:
self.Ant_sg = self.finegd.empty(self.nspins, dtype=float)
for s in range(self.nspins):
self.interpolator.apply(self.Ant_sG[s], self.Ant_sg[s])
def update(self, density):
# Update time
# t[N] = t[N-1] + dt[N-1] #TODO better time-convention?
self.time += self.timestep
# Complex exponential with/without finite-width envelope
f_w = np.exp(1.0j * self.omega_w * self.time)
if self.sigma is not None:
f_w *= np.exp(-self.time**2 * self.sigma**2 / 2.0)
# Update Fourier transformed density components
# Fnt_wG[N] = Fnt_wG[N-1] + 1/sqrt(pi) * (nt_G[N]-avg_nt_G[N-1]) \
# * (f[N]*t[N] - gamma[N-1]) * dt[N]/(t[N]+dt[N])
for w in range(self.nw):
self.Fnt_wsG[w] += 1/np.pi**0.5 * (density.nt_sG - self.Ant_sG) \
* (f_w[w]*self.time - self.gamma_w[w]) * self.timestep \
/ (self.time + self.timestep)
# Update the cumulative phase factors
# gamma[N] = gamma[N-1] + f[N]*dt[N]
self.gamma_w += f_w * self.timestep
# If dt[N] = dt for all N and sigma = 0, then this simplifies to:
# gamma[N] = Sum_{n=0}^N exp(i*omega*n*dt) * dt
# = (1 - exp(i*omega*(N+1)*dt)) / (1 - exp(i*omega*dt)) * dt
# Update average density
# Ant_G[N] = (t[N]*Ant_G[N-1] + nt_G[N]*dt[N])/(t[N]+dt[N])
self.Ant_sG = (self.time*self.Ant_sG + density.nt_sG*self.timestep) \
/ (self.time + self.timestep)
def get_fourier_transform(self, frequency=0, spin=0, gridrefinement=1):
if gridrefinement == 1:
return self.Fnt_wsG[frequency, spin]
elif gridrefinement == 2:
if self.Fnt_wsg is None:
self.interpolate_fourier_transform()
return self.Fnt_wsg[frequency, spin]
else:
raise NotImplementedError('Arbitrary refinement not implemented')
def get_average(self, spin=0, gridrefinement=1):
if gridrefinement == 1:
return self.Ant_sG[spin]
elif gridrefinement == 2:
if self.Ant_sg is None:
self.interpolate_average()
return self.Ant_sg[spin]
else:
raise NotImplementedError('Arbitrary refinement not implemented')
def read(self, filename, idiotproof=True):
if idiotproof and not filename.endswith('.ftd'):
raise IOError('Filename must end with `.ftd`.')
tar = Reader(filename)
# Test data type
dtype = {'Float': float, 'Complex': complex}[tar['DataType']]
if dtype != self.dtype:
raise IOError('Data is an incompatible type.')
# Test time
time = tar['Time']
if idiotproof and abs(time - self.time) >= 1e-9:
raise IOError('Timestamp is incompatible with calculator.')
# Test timestep (non-critical)
timestep = tar['TimeStep']
if abs(timestep - self.timestep) > 1e-12:
print('Warning: Time-step has been altered. (%lf -> %lf)' \
% (self.timestep, timestep))
self.timestep = timestep
# Test dimensions
nw = tar.dimension('nw')
nspins = tar.dimension('nspins')
ng = (tar.dimension('ngptsx'), tar.dimension('ngptsy'), \
tar.dimension('ngptsz'),)
if (nw != self.nw or nspins != self.nspins
or (ng != self.gd.get_size_of_global_array()).any()):
raise IOError('Data has incompatible shapes.')
# Test width (non-critical)
sigma = tar['Width']
if ((sigma is None)!=(self.sigma is None) or # float <-> None
(sigma is not None and self.sigma is not None and \
abs(sigma - self.sigma) > 1e-12)): # float -> float
print('Warning: Width has been altered. (%s -> %s)' \
% (self.sigma, sigma))
self.sigma = sigma
# Read frequencies
self.omega_w[:] = tar.get('Frequency')
# Read cumulative phase factors
self.gamma_w[:] = tar.get('PhaseFactor')
# Read average densities on master and distribute
for s in range(self.nspins):
all_Ant_G = tar.get('Average', s)
self.gd.distribute(all_Ant_G, self.Ant_sG[s])
# Read fourier transforms on master and distribute
for w in range(self.nw):
for s in range(self.nspins):
all_Fnt_G = tar.get('FourierTransform', w, s)
self.gd.distribute(all_Fnt_G, self.Fnt_wsG[w, s])
# Close for good measure
tar.close()
def write(self, filename, idiotproof=True):
if idiotproof and not filename.endswith('.ftd'):
raise IOError('Filename must end with `.ftd`.')
master = self.world.rank == 0
# Open writer on master and set parameters/dimensions
if master:
tar = Writer(filename)
tar['DataType'] = {float: 'Float', complex: 'Complex'}[self.dtype]
tar['Time'] = self.time
tar['TimeStep'] = self.timestep #non-essential
tar['Width'] = self.sigma
tar.dimension('nw', self.nw)
tar.dimension('nspins', self.nspins)
# Create dimensions for varioius netCDF variables:
ng = self.gd.get_size_of_global_array()
tar.dimension('ngptsx', ng[0])
tar.dimension('ngptsy', ng[1])
tar.dimension('ngptsz', ng[2])
# Write frequencies
tar.add('Frequency', ('nw', ), self.omega_w, dtype=float)
# Write cumulative phase factors
tar.add('PhaseFactor', ('nw', ), self.gamma_w, dtype=self.dtype)
# Collect average densities on master and write
if master:
tar.add('Average', (
'nspins',
'ngptsx',
'ngptsy',
'ngptsz',
),
dtype=float)
for s in range(self.nspins):
big_Ant_G = self.gd.collect(self.Ant_sG[s])
if master:
tar.fill(big_Ant_G)
# Collect fourier transforms on master and write
if master:
tar.add('FourierTransform', ('nw', 'nspins', 'ngptsx', 'ngptsy', \
'ngptsz', ), dtype=self.dtype)
for w in range(self.nw):
for s in range(self.nspins):
big_Fnt_G = self.gd.collect(self.Fnt_wsG[w, s])
if master:
tar.fill(big_Fnt_G)
# Close to flush changes
if master:
tar.close()
# Make sure slaves don't return before master is done
self.world.barrier()
def dump(self, filename):
if debug:
assert is_contiguous(self.Fnt_wsG, self.dtype)
assert is_contiguous(self.Ant_sG, float)
all_Fnt_wsG = self.gd.collect(self.Fnt_wsG)
all_Ant_sG = self.gd.collect(self.Ant_sG)
if self.world.rank == 0:
all_Fnt_wsG.dump(filename)
all_Ant_sG.dump(filename + '_avg') # crude but easy
self.omega_w.dump(filename + '_omega') # crude but easy
self.gamma_w.dump(filename + '_gamma') # crude but easy
def load(self, filename):
if self.world.rank == 0:
all_Fnt_wsG = np.load(filename)
all_Ant_sG = np.load(filename + '_avg') # crude but easy
else:
all_Fnt_wsG = None
all_Ant_sG = None
if debug:
assert all_Fnt_wsG is None or is_contiguous(
all_Fnt_wsG, self.dtype)
assert all_Ant_sG is None or is_contiguous(all_Ant_sG, float)
if not self.allocated:
self.allocate()
self.gd.distribute(all_Fnt_wsG, self.Fnt_wsG)
self.gd.distribute(all_Ant_sG, self.Ant_sG)
self.omega_w = np.load(filename + '_omega') # crude but easy
self.gamma_w = np.load(filename + '_gamma') # crude but easy
def get_all_electron_density(self,
atoms=None,
gridrefinement=2,
spos_ac=None,
skip_core=False):
"""Return real all-electron density array.
Usage: Either get_all_electron_density(atoms) or
get_all_electron_density(spos_ac=spos_ac)
skip_core=True theoretically returns the
all-electron valence density (use with
care; will not in general integrate
to valence)
"""
if spos_ac is None:
spos_ac = atoms.get_scaled_positions() % 1.0
# Refinement of coarse grid, for representation of the AE-density
# XXXXXXXXXXXX think about distribution depending on gridrefinement!
if gridrefinement == 1:
gd = self.redistributor.aux_gd
n_sg = self.nt_sG.copy()
# This will get the density with the same distribution
# as finegd:
n_sg = self.redistributor.distribute(n_sg)
elif gridrefinement == 2:
gd = self.finegd
if self.nt_sg is None:
self.interpolate_pseudo_density()
n_sg = self.nt_sg.copy()
elif gridrefinement == 4:
# Extra fine grid
gd = self.finegd.refine()
# Interpolation function for the density:
interpolator = Transformer(self.finegd, gd, 3) # XXX grids!
# Transfer the pseudo-density to the fine grid:
n_sg = gd.empty(self.nspins)
if self.nt_sg is None:
self.interpolate_pseudo_density()
for s in range(self.nspins):
interpolator.apply(self.nt_sg[s], n_sg[s])
else:
raise NotImplementedError
# Add corrections to pseudo-density to get the AE-density
splines = {}
phi_aj = []
phit_aj = []
nc_a = []
nct_a = []
for a, id in enumerate(self.setups.id_a):
if id in splines:
phi_j, phit_j, nc, nct = splines[id]
else:
# Load splines:
phi_j, phit_j, nc, nct = self.setups[a].get_partial_waves()[:4]
splines[id] = (phi_j, phit_j, nc, nct)
phi_aj.append(phi_j)
phit_aj.append(phit_j)
nc_a.append([nc])
nct_a.append([nct])
# Create localized functions from splines
phi = BasisFunctions(gd, phi_aj)
phit = BasisFunctions(gd, phit_aj)
nc = LFC(gd, nc_a)
nct = LFC(gd, nct_a)
phi.set_positions(spos_ac)
phit.set_positions(spos_ac)
nc.set_positions(spos_ac)
nct.set_positions(spos_ac)
I_sa = np.zeros((self.nspins, len(spos_ac)))
a_W = np.empty(len(phi.M_W), np.intc)
W = 0
for a in phi.atom_indices:
nw = len(phi.sphere_a[a].M_w)
a_W[W:W + nw] = a
W += nw
x_W = phi.create_displacement_arrays()[0]
D_asp = self.D_asp # XXX really?
rho_MM = np.zeros((phi.Mmax, phi.Mmax))
for s, I_a in enumerate(I_sa):
M1 = 0
for a, setup in enumerate(self.setups):
ni = setup.ni
D_sp = D_asp.get(a)
if D_sp is None:
D_sp = np.empty((self.nspins, ni * (ni + 1) // 2))
else:
I_a[a] = (
(setup.Nct) / self.nspins -
sqrt(4 * pi) * np.dot(D_sp[s], setup.Delta_pL[:, 0]))
if not skip_core:
I_a[a] -= setup.Nc / self.nspins
if gd.comm.size > 1:
gd.comm.broadcast(D_sp, D_asp.partition.rank_a[a])
M2 = M1 + ni
rho_MM[M1:M2, M1:M2] = unpack2(D_sp[s])
M1 = M2
assert np.all(n_sg[s].shape == phi.gd.n_c)
phi.lfc.ae_valence_density_correction(rho_MM, n_sg[s], a_W, I_a,
x_W)
phit.lfc.ae_valence_density_correction(-rho_MM, n_sg[s], a_W, I_a,
x_W)
a_W = np.empty(len(nc.M_W), np.intc)
W = 0
for a in nc.atom_indices:
nw = len(nc.sphere_a[a].M_w)
a_W[W:W + nw] = a
W += nw
scale = 1.0 / self.nspins
for s, I_a in enumerate(I_sa):
if not skip_core:
nc.lfc.ae_core_density_correction(scale, n_sg[s], a_W, I_a)
nct.lfc.ae_core_density_correction(-scale, n_sg[s], a_W, I_a)
gd.comm.sum(I_a)
N_c = gd.N_c
g_ac = np.around(N_c * spos_ac).astype(int) % N_c - gd.beg_c
if not skip_core:
for I, g_c in zip(I_a, g_ac):
if (g_c >= 0).all() and (g_c < gd.n_c).all():
n_sg[s][tuple(g_c)] -= I / gd.dv
return n_sg, gd
class PhononPerturbation(Perturbation):
"""Implementation of a phonon perturbation.
This class implements the change in the effective potential due to a
displacement of an atom ``a`` in direction ``v`` with wave-vector ``q``.
The action of the perturbing potential on a state vector is implemented in
the ``apply`` member function.
"""
def __init__(self, calc, kd, poisson_solver, dtype=float, **kwargs):
"""Store useful objects, e.g. lfc's for the various atomic functions.
Depending on whether the system is periodic or finite, Poisson's equation
is solved with FFT or multigrid techniques, respectively.
Parameters
----------
calc: Calculator
Ground-state calculation.
kd: KPointDescriptor
Descriptor for the q-vectors of the dynamical matrix.
"""
self.kd = kd
self.dtype = dtype
self.poisson = poisson_solver
# Gamma wrt q-vector
if self.kd.gamma:
self.phase_cd = None
else:
assert self.kd.mynks == len(self.kd.ibzk_qc)
self.phase_qcd = []
sdisp_cd = calc.wfs.gd.sdisp_cd
for q in range(self.kd.mynks):
phase_cd = np.exp(2j * np.pi * \
sdisp_cd * self.kd.ibzk_qc[q, :, np.newaxis])
self.phase_qcd.append(phase_cd)
# Store grid-descriptors
self.gd = calc.density.gd
self.finegd = calc.density.finegd
# Steal setups for the lfc's
setups = calc.wfs.setups
# Store projector coefficients
self.dH_asp = calc.hamiltonian.dH_asp.copy()
# Localized functions:
# core corections
self.nct = LFC(self.gd, [[setup.nct] for setup in setups],
integral=[setup.Nct for setup in setups], dtype=self.dtype)
# compensation charges
#XXX what is the consequence of numerical errors in the integral ??
self.ghat = LFC(self.finegd, [setup.ghat_l for setup in setups],
dtype=self.dtype)
## self.ghat = LFC(self.finegd, [setup.ghat_l for setup in setups],
## integral=sqrt(4 * pi), dtype=self.dtype)
# vbar potential
self.vbar = LFC(self.finegd, [[setup.vbar] for setup in setups],
dtype=self.dtype)
# Expansion coefficients for the compensation charges
self.Q_aL = calc.density.Q_aL.copy()
# Grid transformer -- convert array from fine to coarse grid
self.restrictor = Transformer(self.finegd, self.gd, nn=3,
dtype=self.dtype, allocate=False)
# Atom, cartesian coordinate and q-vector of the perturbation
self.a = None
self.v = None
# Local q-vector index of the perturbation
if self.kd.gamma:
self.q = -1
else:
self.q = None
def initialize(self, spos_ac):
"""Prepare the various attributes for a calculation."""
# Set positions on LFC's
self.nct.set_positions(spos_ac)
self.ghat.set_positions(spos_ac)
self.vbar.set_positions(spos_ac)
if not self.kd.gamma:
# Set q-vectors and update
self.ghat.set_k_points(self.kd.ibzk_qc)
self.ghat._update(spos_ac)
# Set q-vectors and update
self.vbar.set_k_points(self.kd.ibzk_qc)
self.vbar._update(spos_ac)
# Phase factor exp(iq.r) needed to obtian the periodic part of lfcs
coor_vg = self.finegd.get_grid_point_coordinates()
cell_cv = self.finegd.cell_cv
# Convert to scaled coordinates
scoor_cg = np.dot(la.inv(cell_cv), coor_vg.swapaxes(0, -2))
scoor_cg = scoor_cg.swapaxes(1,-2)
# Phase factor
phase_qg = np.exp(2j * pi *
np.dot(self.kd.ibzk_qc, scoor_cg.swapaxes(0,-2)))
self.phase_qg = phase_qg.swapaxes(1, -2)
#XXX To be removed from this class !!
# Setup the Poisson solver -- to be used on the fine grid
self.poisson.set_grid_descriptor(self.finegd)
self.poisson.initialize()
# Grid transformer
self.restrictor.allocate()
def set_q(self, q):
"""Set the index of the q-vector of the perturbation."""
assert not self.kd.gamma, "Gamma-point calculation"
self.q = q
# Update phases and Poisson solver
self.phase_cd = self.phase_qcd[q]
self.poisson.set_q(self.kd.ibzk_qc[q])
# Invalidate calculated quantities
# - local part of perturbing potential
self.v1_G = None
def set_av(self, a, v):
"""Set atom and cartesian component of the perturbation.
Parameters
----------
a: int
Index of the atom.
v: int
Cartesian component (0, 1 or 2) of the atomic displacement.
"""
assert self.q is not None
self.a = a
self.v = v
# Update derivative of local potential
self.calculate_local_potential()
def get_phase_cd(self):
"""Overwrite base class member function."""
return self.phase_cd
def has_q(self):
"""Overwrite base class member function."""
return (not self.kd.gamma)
def get_q(self):
"""Return q-vector."""
assert not self.kd.gamma, "Gamma-point calculation."
return self.kd.ibzk_qc[self.q]
def solve_poisson(self, phi_g, rho_g):
"""Solve Poisson's equation for a Bloch-type charge distribution.
More to come here ...
Parameters
----------
phi_g: GridDescriptor
Grid for the solution of Poissons's equation.
rho_g: GridDescriptor
Grid with the charge distribution.
"""
#assert phi_g.shape == rho_g.shape == self.phase_qg.shape[-3:], \
# ("Arrays have incompatible shapes.")
assert self.q is not None, ("q-vector not set")
# Gamma point calculation wrt the q-vector -> rho_g periodic
if self.kd.gamma:
#XXX NOTICE: solve_neutral
self.poisson.solve_neutral(phi_g, rho_g)
else:
# Divide out the phase factor to get the periodic part
rhot_g = rho_g/self.phase_qg[self.q]
# Solve Poisson's equation for the periodic part of the potential
#XXX NOTICE: solve_neutral
self.poisson.solve_neutral(phi_g, rhot_g)
# Return to Bloch form
phi_g *= self.phase_qg[self.q]
def calculate_local_potential(self):
"""Derivate of the local potential wrt an atomic displacements.
The local part of the PAW potential has contributions from the
compensation charges (``ghat``) and a spherical symmetric atomic
potential (``vbar``).
"""
assert self.a is not None
assert self.v is not None
assert self.q is not None
a = self.a
v = self.v
# Expansion coefficients for the ghat functions
Q_aL = self.ghat.dict(zero=True)
# Remember sign convention for add_derivative method
# And be sure not to change the dtype of the arrays by assigning values
# to array elements.
Q_aL[a][:] = -1 * self.Q_aL[a]
# Grid for derivative of compensation charges
ghat1_g = self.finegd.zeros(dtype=self.dtype)
self.ghat.add_derivative(a, v, ghat1_g, c_axi=Q_aL, q=self.q)
# Solve Poisson's eq. for the potential from the periodic part of the
# compensation charge derivative
v1_g = self.finegd.zeros(dtype=self.dtype)
self.solve_poisson(v1_g, ghat1_g)
# Store potential from the compensation charge
self.vghat1_g = v1_g.copy()
# Add derivative of vbar - sign convention in add_derivative method
c_ai = self.vbar.dict(zero=True)
c_ai[a][0] = -1.
self.vbar.add_derivative(a, v, v1_g, c_axi=c_ai, q=self.q)
# Store potential for the evaluation of the energy derivative
self.v1_g = v1_g.copy()
# Transfer to coarse grid
v1_G = self.gd.zeros(dtype=self.dtype)
self.restrictor.apply(v1_g, v1_G, phases=self.phase_cd)
self.v1_G = v1_G
def apply(self, psi_nG, y_nG, wfs, k, kplusq):
"""Apply perturbation to unperturbed wave-functions.
Parameters
----------
psi_nG: ndarray
Set of grid vectors to which the perturbation is applied.
y_nG: ndarray
Output vectors.
wfs: WaveFunctions
Instance of class ``WaveFunctions``.
k: int
Index of the k-point for the vectors.
kplusq: int
Index of the k+q vector.
"""
assert self.a is not None
assert self.v is not None
assert self.q is not None
assert psi_nG.ndim in (3, 4)
assert tuple(self.gd.n_c) == psi_nG.shape[-3:]
if psi_nG.ndim == 3:
y_nG += self.v1_G * psi_nG
else:
y_nG += self.v1_G[np.newaxis, :] * psi_nG
self.apply_nonlocal_potential(psi_nG, y_nG, wfs, k, kplusq)
def apply_nonlocal_potential(self, psi_nG, y_nG, wfs, k, kplusq):
"""Derivate of the non-local PAW potential wrt an atomic displacement.
Parameters
----------
k: int
Index of the k-point being operated on.
kplusq: int
Index of the k+q vector.
"""
assert self.a is not None
assert self.v is not None
assert psi_nG.ndim in (3, 4)
assert tuple(self.gd.n_c) == psi_nG.shape[-3:]
if psi_nG.ndim == 3:
n = 1
else:
n = psi_nG.shape[0]
a = self.a
v = self.v
P_ani = wfs.kpt_u[k].P_ani
dP_aniv = wfs.kpt_u[k].dP_aniv
pt = wfs.pt
# < p_a^i | Psi_nk >
P_ni = P_ani[a]
# < dp_av^i | Psi_nk > - remember the sign convention of the derivative
dP_ni = -1 * dP_aniv[a][...,v]
# Expansion coefficients for the projectors on atom a
dH_ii = unpack(self.dH_asp[a][0])
# The derivative of the non-local PAW potential has two contributions
# 1) Sum over projectors
c_ni = np.dot(dP_ni, dH_ii)
c_ani = pt.dict(shape=n, zero=True)
c_ani[a] = c_ni
# k+q !!
pt.add(y_nG, c_ani, q=kplusq)
# 2) Sum over derivatives of the projectors
dc_ni = np.dot(P_ni, dH_ii)
dc_ani = pt.dict(shape=n, zero=True)
# Take care of sign of derivative in the coefficients
dc_ani[a] = -1 * dc_ni
# k+q !!
pt.add_derivative(a, v, y_nG, dc_ani, q=kplusq)
class RealSpaceDensity(Density):
def __init__(self,
gd,
finegd,
nspins,
charge,
redistributor,
stencil=3,
background_charge=None):
Density.__init__(self,
gd,
finegd,
nspins,
charge,
redistributor,
background_charge=background_charge)
self.stencil = stencil
def initialize(self, setups, timer, magmom_a, hund):
Density.initialize(self, setups, timer, magmom_a, hund)
# Interpolation function for the density:
self.interpolator = Transformer(self.redistributor.aux_gd, self.finegd,
self.stencil)
spline_aj = []
for setup in setups:
if setup.nct is None:
spline_aj.append([])
else:
spline_aj.append([setup.nct])
self.nct = LFC(self.gd,
spline_aj,
integral=[setup.Nct for setup in setups],
forces=True,
cut=True)
self.ghat = LFC(self.finegd, [setup.ghat_l for setup in setups],
integral=sqrt(4 * pi),
forces=True)
def set_positions(self, spos_ac, rank_a=None):
Density.set_positions(self, spos_ac, rank_a)
self.nct_G = self.gd.zeros()
self.nct.add(self.nct_G, 1.0 / self.nspins)
def interpolate_pseudo_density(self, comp_charge=None):
"""Interpolate pseudo density to fine grid."""
if comp_charge is None:
comp_charge = self.calculate_multipole_moments()
self.nt_sg = self.distribute_and_interpolate(self.nt_sG, self.nt_sg)
# With periodic boundary conditions, the interpolation will
# conserve the number of electrons.
if not self.gd.pbc_c.all():
# With zero-boundary conditions in one or more directions,
# this is not the case.
pseudo_charge = (self.background_charge.charge - self.charge -
comp_charge)
if abs(pseudo_charge) > 1.0e-14:
x = (pseudo_charge / self.finegd.integrate(self.nt_sg).sum())
self.nt_sg *= x
def interpolate(self, in_xR, out_xR=None):
"""Interpolate array(s)."""
# ndim will be 3 in finite-difference mode and 1 when working
# with the AtomPAW class (spherical atoms and 1d grids)
ndim = self.gd.ndim
if out_xR is None:
out_xR = self.finegd.empty(in_xR.shape[:-ndim])
a_xR = in_xR.reshape((-1, ) + in_xR.shape[-ndim:])
b_xR = out_xR.reshape((-1, ) + out_xR.shape[-ndim:])
for in_R, out_R in zip(a_xR, b_xR):
self.interpolator.apply(in_R, out_R)
return out_xR
def distribute_and_interpolate(self, in_xR, out_xR=None):
in_xR = self.redistributor.distribute(in_xR)
return self.interpolate(in_xR, out_xR)
def calculate_pseudo_charge(self):
self.nt_g = self.nt_sg.sum(axis=0)
self.rhot_g = self.nt_g.copy()
self.ghat.add(self.rhot_g, self.Q_aL)
self.background_charge.add_charge_to(self.rhot_g)
if debug:
charge = self.finegd.integrate(self.rhot_g) + self.charge
if abs(charge) > self.charge_eps:
raise RuntimeError('Charge not conserved: excess=%.9f' %
charge)
def get_pseudo_core_kinetic_energy_density_lfc(self):
return LFC(self.gd, [[setup.tauct] for setup in self.setups],
forces=True,
cut=True)
def calculate_dipole_moment(self):
return self.finegd.calculate_dipole_moment(self.rhot_g)
class RealSpaceHamiltonian(Hamiltonian):
def __init__(self,
gd,
finegd,
nspins,
setups,
timer,
xc,
world,
vext=None,
psolver=None,
stencil=3,
redistributor=None):
Hamiltonian.__init__(self,
gd,
finegd,
nspins,
setups,
timer,
xc,
world,
vext=vext,
redistributor=redistributor)
# Solver for the Poisson equation:
if psolver is None:
psolver = {}
if isinstance(psolver, dict):
psolver = create_poisson_solver(**psolver)
self.poisson = psolver
self.poisson.set_grid_descriptor(self.finegd)
# Restrictor function for the potential:
self.restrictor = Transformer(self.finegd, self.redistributor.aux_gd,
stencil)
self.restrict = self.restrictor.apply
self.vbar = LFC(self.finegd, [[setup.vbar] for setup in setups],
forces=True)
self.vbar_g = None
def restrict_and_collect(self, a_xg, b_xg=None, phases=None):
if self.redistributor.enabled:
tmp_xg = self.restrictor.apply(a_xg, output=None, phases=phases)
b_xg = self.redistributor.collect(tmp_xg, b_xg)
else:
b_xg = self.restrictor.apply(a_xg, output=b_xg, phases=phases)
return b_xg
def __str__(self):
s = Hamiltonian.__str__(self)
degree = self.restrictor.nn * 2 - 1
name = ['linear', 'cubic', 'quintic', 'heptic'][degree // 2]
s += (' Interpolation: tri-%s ' % name +
'(%d. degree polynomial)\n' % degree)
s += ' Poisson solver: %s' % self.poisson.get_description()
return s
def set_positions(self, spos_ac, rank_a):
Hamiltonian.set_positions(self, spos_ac, rank_a)
if self.vbar_g is None:
self.vbar_g = self.finegd.empty()
self.vbar_g[:] = 0.0
self.vbar.add(self.vbar_g)
def update_pseudo_potential(self, dens):
self.timer.start('vbar')
e_zero = self.finegd.integrate(self.vbar_g,
dens.nt_g,
global_integral=False)
vt_g = self.vt_sg[0]
vt_g[:] = self.vbar_g
self.timer.stop('vbar')
e_external = 0.0
if self.vext is not None:
vext_g = self.vext.get_potential(self.finegd)
vt_g += vext_g
e_external = self.finegd.integrate(vext_g,
dens.rhot_g,
global_integral=False)
if self.nspins == 2:
self.vt_sg[1] = vt_g
self.timer.start('XC 3D grid')
e_xc = self.xc.calculate(self.finegd, dens.nt_sg, self.vt_sg)
e_xc /= self.finegd.comm.size
self.timer.stop('XC 3D grid')
self.timer.start('Poisson')
# npoisson is the number of iterations:
self.npoisson = self.poisson.solve(self.vHt_g,
dens.rhot_g,
charge=-dens.charge)
self.timer.stop('Poisson')
self.timer.start('Hartree integrate/restrict')
e_coulomb = 0.5 * self.finegd.integrate(
self.vHt_g, dens.rhot_g, global_integral=False)
for vt_g in self.vt_sg:
vt_g += self.vHt_g
self.timer.stop('Hartree integrate/restrict')
return np.array([e_coulomb, e_zero, e_external, e_xc])
def calculate_kinetic_energy(self, density):
# XXX new timer item for kinetic energy?
self.timer.start('Hartree integrate/restrict')
self.restrict_and_collect(self.vt_sg, self.vt_sG)
e_kinetic = 0.0
s = 0
for vt_G, nt_G in zip(self.vt_sG, density.nt_sG):
if self.ref_vt_sG is not None:
vt_G += self.ref_vt_sG[s]
if s < self.nspins:
e_kinetic -= self.gd.integrate(vt_G,
nt_G - density.nct_G,
global_integral=False)
else:
e_kinetic -= self.gd.integrate(vt_G,
nt_G,
global_integral=False)
s += 1
self.timer.stop('Hartree integrate/restrict')
return e_kinetic
def calculate_atomic_hamiltonians(self, dens):
def getshape(a):
return sum(2 * l + 1 for l, _ in enumerate(self.setups[a].ghat_l)),
W_aL = ArrayDict(self.atomdist.aux_partition, getshape, float)
if self.vext:
vext_g = self.vext.get_potential(self.finegd)
dens.ghat.integrate(self.vHt_g + vext_g, W_aL)
else:
dens.ghat.integrate(self.vHt_g, W_aL)
return self.atomdist.to_work(self.atomdist.from_aux(W_aL))
def calculate_forces2(self, dens, ghat_aLv, nct_av, vbar_av):
if self.nspins == 2:
vt_G = self.vt_sG.mean(0)
else:
vt_G = self.vt_sG[0]
self.vbar.derivative(dens.nt_g, vbar_av)
if self.vext:
vext_g = self.vext.get_potential(self.finegd)
dens.ghat.derivative(self.vHt_g + vext_g, ghat_aLv)
else:
dens.ghat.derivative(self.vHt_g, ghat_aLv)
dens.nct.derivative(vt_G, nct_av)
def get_electrostatic_potential(self, dens):
self.update(dens)
v_g = self.finegd.collect(self.vHt_g, broadcast=True)
v_g = self.finegd.zero_pad(v_g)
if hasattr(self.poisson, 'correction'):
assert self.poisson.c == 2
v_g[:, :, 0] = self.poisson.correction
return v_g
