#!/usr/bin/env python
# Copyright 2014-2019,2021 The PySCF Developers. All Rights Reserved.
#
# Licensed under the Apache License, Version 2.0 (the "License");
# you may not use this file except in compliance with the License.
# You may obtain a copy of the License at
#
# http://www.apache.org/licenses/LICENSE-2.0
#
# Unless required by applicable law or agreed to in writing, software
# distributed under the License is distributed on an "AS IS" BASIS,
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
# See the License for the specific language governing permissions and
# limitations under the License.
#
# Author: Qiming Sun <osirpt.sun@gmail.com>
#
'''
Density fitting
Divide the 3-center Coulomb integrals to two parts. Compute the local
part in real space, long range part in reciprocal space.
Note when diffuse functions are used in fitting basis, it is easy to cause
linear dependence (non-positive definite) issue under PBC.
Ref:
J. Chem. Phys. 147, 164119 (2017)
'''
import os
import ctypes
import warnings
import tempfile
import contextlib
import itertools
import numpy
import h5py
import scipy.linalg
from pyscf import lib
from pyscf import gto
from pyscf.lib import logger
from pyscf.df import addons
from pyscf.df.outcore import _guess_shell_ranges
from pyscf.pbc.gto.cell import _estimate_rcut
from pyscf.pbc import tools
from pyscf.pbc.df import incore
from pyscf.pbc.df import outcore
from pyscf.pbc.df import ft_ao
from pyscf.pbc.df import aft
from pyscf.pbc.df import df_jk
from pyscf.pbc.df import df_ao2mo
from pyscf.pbc.df.aft import estimate_eta, _check_kpts
from pyscf.pbc.df.df_jk import zdotCN
from pyscf.pbc.lib.kpts_helper import (is_zero, gamma_point, member, unique,
KPT_DIFF_TOL)
from pyscf.pbc.df.gdf_builder import libpbc, _CCGDFBuilder, _CCNucBuilder
from pyscf.pbc.df.rsdf_builder import _RSGDFBuilder, _RSNucBuilder
from pyscf import __config__
LINEAR_DEP_THR = getattr(__config__, 'pbc_df_df_DF_lindep', 1e-9)
LONGRANGE_AFT_TURNOVER_THRESHOLD = 2.5
[docs]
def make_modrho_basis(cell, auxbasis=None, drop_eta=None):
r'''Generate a cell object using the density fitting auxbasis as
the basis set. The normalization coeffcients of the auxiliary cell are
different to the regular (square-norm) convention. To simplify the
compensated charge algorithm, they are normalized against
\int (r^l e^{-ar^2} r^2 dr
'''
auxcell = incore.make_auxcell(cell, auxbasis)
# Note libcint library will multiply the norm of the integration over spheric
# part sqrt(4pi) to the basis.
half_sph_norm = numpy.sqrt(.25/numpy.pi)
steep_shls = []
ndrop = 0
rcut = []
_env = auxcell._env.copy()
for ib in range(len(auxcell._bas)):
l = auxcell.bas_angular(ib)
np = auxcell.bas_nprim(ib)
nc = auxcell.bas_nctr(ib)
es = auxcell.bas_exp(ib)
ptr = auxcell._bas[ib,gto.PTR_COEFF]
cs = auxcell._env[ptr:ptr+np*nc].reshape(nc,np).T
if drop_eta is not None and numpy.any(es < drop_eta):
cs = cs[es>=drop_eta]
es = es[es>=drop_eta]
np, ndrop = len(es), ndrop+np-len(es)
if np > 0:
pe = auxcell._bas[ib,gto.PTR_EXP]
auxcell._bas[ib,gto.NPRIM_OF] = np
_env[pe:pe+np] = es
# int1 is the multipole value. l*2+2 is due to the radial part integral
# \int (r^l e^{-ar^2} * Y_{lm}) (r^l Y_{lm}) r^2 dr d\Omega
int1 = gto.gaussian_int(l*2+2, es)
s = numpy.einsum('pi,p->i', cs, int1)
# The auxiliary basis normalization factor is not a must for density expansion.
# half_sph_norm here to normalize the monopole (charge). This convention can
# simplify the formulism of \int \bar{\rho}, see function auxbar.
cs = numpy.einsum('pi,i->pi', cs, half_sph_norm/s)
_env[ptr:ptr+np*nc] = cs.T.ravel()
steep_shls.append(ib)
r = _estimate_rcut(es, l, abs(cs).max(axis=1), cell.precision)
rcut.append(r.max())
auxcell._env = _env
auxcell.rcut = max(rcut)
auxcell._bas = numpy.asarray(auxcell._bas[steep_shls], order='C')
logger.info(cell, 'Drop %d primitive fitting functions', ndrop)
logger.info(cell, 'make aux basis, num shells = %d, num cGTOs = %d',
auxcell.nbas, auxcell.nao_nr())
logger.info(cell, 'auxcell.rcut %s', auxcell.rcut)
return auxcell
make_auxcell = make_modrho_basis
[docs]
class GDF(lib.StreamObject, aft.AFTDFMixin):
'''Gaussian density fitting
'''
blockdim = getattr(__config__, 'pbc_df_df_DF_blockdim', 240)
_dataname = 'j3c'
# Call _CCGDFBuilder if applicable. _CCGDFBuilder is slower than
# _RSGDFBuilder but numerically more close to previous versions
_prefer_ccdf = False
# If True, force using denisty matrix-based K-build
force_dm_kbuild = False
_keys = set((
'blockdim', 'force_dm_kbuild', 'cell', 'kpts', 'kpts_band', 'eta',
'mesh', 'exp_to_discard', 'exxdiv', 'auxcell', 'linear_dep_threshold',
))
def __init__(self, cell, kpts=numpy.zeros((1,3))):
self.cell = cell
self.stdout = cell.stdout
self.verbose = cell.verbose
self.max_memory = cell.max_memory
self.kpts = kpts # default is gamma point
self.kpts_band = None
self._auxbasis = None
self.eta = None
self.mesh = None
# exp_to_discard to remove diffused fitting functions. The diffused
# fitting functions may cause linear dependency in DF metric. Removing
# the fitting functions whose exponents are smaller than exp_to_discard
# can improve the linear dependency issue. However, this parameter
# affects the quality of the auxiliary basis. The default value of
# this parameter was set to 0.2 in v1.5.1 or older and was changed to
# 0 since v1.5.2.
self.exp_to_discard = cell.exp_to_discard
# The following attributes are not input options.
self.exxdiv = None # to mimic KRHF/KUHF object in function get_coulG
self.auxcell = None
self.linear_dep_threshold = LINEAR_DEP_THR
self._j_only = False
# If _cderi_to_save is specified, the 3C-integral tensor will be saved in this file.
self._cderi_to_save = tempfile.NamedTemporaryFile(dir=lib.param.TMPDIR)
# If _cderi is specified, the 3C-integral tensor will be read from this file
self._cderi = None
self._rsh_df = {} # Range separated Coulomb DF objects
@property
def auxbasis(self):
return self._auxbasis
@auxbasis.setter
def auxbasis(self, x):
if self._auxbasis != x:
self._auxbasis = x
self.auxcell = None
self._cderi = None
[docs]
def reset(self, cell=None):
if cell is not None:
self.cell = cell
self.auxcell = None
self._cderi = None
self._rsh_df = {}
return self
@property
def gs(self):
return [n//2 for n in self.mesh]
@gs.setter
def gs(self, x):
warnings.warn('Attribute .gs is deprecated. It is replaced by attribute .mesh.\n'
'mesh = the number of PWs (=2*gs+1) for each direction.')
self.mesh = [2*n+1 for n in x]
[docs]
def dump_flags(self, verbose=None):
log = logger.new_logger(self, verbose)
log.info('\n')
log.info('******** %s ********', self.__class__)
if self.auxcell is None:
log.info('auxbasis = %s', self.auxbasis)
else:
log.info('auxbasis = %s', self.auxcell.basis)
if self.eta is not None:
log.info('eta = %s', self.eta)
if self.mesh is not None:
log.info('mesh = %s (%d PWs)', self.mesh, numpy.prod(self.mesh))
log.info('exp_to_discard = %s', self.exp_to_discard)
if isinstance(self._cderi, str):
log.info('_cderi = %s where DF integrals are loaded (readonly).',
self._cderi)
elif isinstance(self._cderi_to_save, str):
log.info('_cderi_to_save = %s', self._cderi_to_save)
else:
log.info('_cderi_to_save = %s', self._cderi_to_save.name)
log.info('len(kpts) = %d', len(self.kpts))
log.debug1(' kpts = %s', self.kpts)
if self.kpts_band is not None:
log.info('len(kpts_band) = %d', len(self.kpts_band))
log.debug1(' kpts_band = %s', self.kpts_band)
return self
[docs]
def build(self, j_only=None, with_j3c=True, kpts_band=None):
if j_only is not None:
self._j_only = j_only
if self.kpts_band is not None:
self.kpts_band = numpy.reshape(self.kpts_band, (-1,3))
if kpts_band is not None:
kpts_band = numpy.reshape(kpts_band, (-1,3))
if self.kpts_band is None:
self.kpts_band = kpts_band
else:
self.kpts_band = unique(numpy.vstack((self.kpts_band,kpts_band)))[0]
self.check_sanity()
self.dump_flags()
self.auxcell = make_modrho_basis(self.cell, self.auxbasis,
self.exp_to_discard)
if with_j3c and self._cderi_to_save is not None:
if isinstance(self._cderi_to_save, str):
cderi = self._cderi_to_save
else:
cderi = self._cderi_to_save.name
if isinstance(self._cderi, str):
if self._cderi == cderi and os.path.isfile(cderi):
logger.warn(self, 'File %s (specified by ._cderi) is '
'overwritten by GDF initialization.', cderi)
else:
logger.warn(self, 'Value of ._cderi is ignored. '
'DF integrals will be saved in file %s .', cderi)
self._cderi = cderi
t1 = (logger.process_clock(), logger.perf_counter())
self._make_j3c(self.cell, self.auxcell, None, cderi)
t1 = logger.timer_debug1(self, 'j3c', *t1)
return self
def _make_j3c(self, cell=None, auxcell=None, kptij_lst=None, cderi_file=None):
if cell is None: cell = self.cell
if auxcell is None: auxcell = self.auxcell
if cderi_file is None: cderi_file = self._cderi_to_save
# Remove duplicated k-points. Duplicated kpts may lead to a buffer
# located in incore.wrap_int3c larger than necessary. Integral code
# only fills necessary part of the buffer, leaving some space in the
# buffer unfilled.
if self.kpts_band is None:
kpts_union = self.kpts
else:
kpts_union = unique(numpy.vstack([self.kpts, self.kpts_band]))[0]
if self._prefer_ccdf or cell.omega > 0:
# For long-range integrals _CCGDFBuilder is the only option
dfbuilder = _CCGDFBuilder(cell, auxcell, kpts_union)
dfbuilder.eta = self.eta
else:
dfbuilder = _RSGDFBuilder(cell, auxcell, kpts_union)
dfbuilder.mesh = self.mesh
dfbuilder.linear_dep_threshold = self.linear_dep_threshold
j_only = self._j_only or len(kpts_union) == 1
dfbuilder.make_j3c(cderi_file, j_only=j_only, dataname=self._dataname,
kptij_lst=kptij_lst)
[docs]
def cderi_array(self, label=None):
'''
Returns CDERIArray object which provides numpy APIs to access cderi tensor.
'''
if label is None:
label = self._dataname
if self._cderi is None:
self.build()
return CDERIArray(self._cderi, label)
[docs]
def has_kpts(self, kpts):
if kpts is None:
return True
else:
kpts = numpy.asarray(kpts).reshape(-1,3)
if self.kpts_band is None:
return all((len(member(kpt, self.kpts))>0) for kpt in kpts)
else:
return all((len(member(kpt, self.kpts))>0 or
len(member(kpt, self.kpts_band))>0) for kpt in kpts)
[docs]
def sr_loop(self, kpti_kptj=numpy.zeros((2,3)), max_memory=2000,
compact=True, blksize=None, aux_slice=None):
'''Short range part'''
if self._cderi is None:
self.build()
cell = self.cell
kpti, kptj = kpti_kptj
unpack = is_zero(kpti-kptj) and not compact
is_real = is_zero(kpti_kptj)
nao = cell.nao_nr()
if blksize is None:
if is_real:
blksize = max_memory*1e6/8/(nao**2*2)
else:
blksize = max_memory*1e6/16/(nao**2*2)
blksize /= 2 # For prefetch
blksize = max(16, min(int(blksize), self.blockdim))
logger.debug3(self, 'max_memory %d MB, blksize %d', max_memory, blksize)
def load(aux_slice):
b0, b1 = aux_slice
naux = b1 - b0
if is_real:
LpqR = numpy.asarray(j3c[b0:b1].real)
if compact and LpqR.shape[1] == nao**2:
LpqR = lib.pack_tril(LpqR.reshape(naux,nao,nao))
elif unpack and LpqR.shape[1] != nao**2:
LpqR = lib.unpack_tril(LpqR).reshape(naux,nao**2)
LpqI = numpy.zeros_like(LpqR)
else:
Lpq = numpy.asarray(j3c[b0:b1])
LpqR = numpy.asarray(Lpq.real, order='C')
LpqI = numpy.asarray(Lpq.imag, order='C')
Lpq = None
if compact and LpqR.shape[1] == nao**2:
LpqR = lib.pack_tril(LpqR.reshape(naux,nao,nao))
LpqI = lib.pack_tril(LpqI.reshape(naux,nao,nao))
elif unpack and LpqR.shape[1] != nao**2:
LpqR = lib.unpack_tril(LpqR).reshape(naux,nao**2)
LpqI = lib.unpack_tril(LpqI, lib.ANTIHERMI).reshape(naux,nao**2)
return LpqR, LpqI
with _load3c(self._cderi, self._dataname, kpti_kptj) as j3c:
if aux_slice is None:
slices = lib.prange(0, j3c.shape[0], blksize)
else:
slices = lib.prange(*aux_slice, blksize)
for LpqR, LpqI in lib.map_with_prefetch(load, slices):
yield LpqR, LpqI, 1
LpqR = LpqI = None
if cell.dimension == 2 and cell.low_dim_ft_type != 'inf_vacuum':
# Truncated Coulomb operator is not postive definite. Load the
# CDERI tensor of negative part.
with _load3c(self._cderi, self._dataname+'-', kpti_kptj,
ignore_key_error=True) as j3c:
if aux_slice is None:
slices = lib.prange(0, j3c.shape[0], blksize)
else:
slices = lib.prange(*aux_slice, blksize)
for LpqR, LpqI in lib.map_with_prefetch(load, slices):
yield LpqR, LpqI, -1
LpqR = LpqI = None
[docs]
def get_pp(self, kpts=None):
'''Get the periodic pseudotential nuc-el AO matrix, with G=0 removed.
'''
cell = self.cell
kpts, is_single_kpt = _check_kpts(self, kpts)
if self._prefer_ccdf or cell.omega > 0:
# For long-range integrals _CCGDFBuilder is the only option
dfbuilder = _CCNucBuilder(cell, kpts).build()
else:
dfbuilder = _RSNucBuilder(cell, kpts).build()
vpp = dfbuilder.get_pp()
if is_single_kpt:
vpp = vpp[0]
return vpp
[docs]
def get_nuc(self, kpts=None):
'''Get the periodic nuc-el AO matrix, with G=0 removed.
'''
cell = self.cell
kpts, is_single_kpt = _check_kpts(self, kpts)
if self._prefer_ccdf or cell.omega > 0:
# For long-range integrals _CCGDFBuilder is the only option
dfbuilder = _CCNucBuilder(cell, kpts).build()
else:
dfbuilder = _RSNucBuilder(cell, kpts).build()
nuc = dfbuilder.get_nuc()
if is_single_kpt:
nuc = nuc[0]
return nuc
# Note: Special exxdiv by default should not be used for an arbitrary
# input density matrix. When the df object was used with the molecular
# post-HF code, get_jk was often called with an incomplete DM (e.g. the
# core DM in CASCI). An SCF level exxdiv treatment is inadequate for
# post-HF methods.
[docs]
def get_jk(self, dm, hermi=1, kpts=None, kpts_band=None,
with_j=True, with_k=True, omega=None, exxdiv=None):
if omega is not None: # J/K for RSH functionals
cell = self.cell
# * AFT is computationally more efficient than GDF if the Coulomb
# attenuation tends to the long-range role (i.e. small omega).
# * Note: changing to AFT integrator may cause small difference to
# the GDF integrator. If a very strict GDF result is desired,
# we can disable this trick by setting
# LONGRANGE_AFT_TURNOVER_THRESHOLD to 0.
# * The sparse mesh is not appropriate for low dimensional systems
# with infinity vacuum since the ERI may require large mesh to
# sample density in vacuum.
if (omega < LONGRANGE_AFT_TURNOVER_THRESHOLD and
cell.dimension >= 2 and cell.low_dim_ft_type != 'inf_vacuum'):
mydf = aft.AFTDF(cell, self.kpts)
ke_cutoff = aft.estimate_ke_cutoff_for_omega(cell, omega)
mydf.mesh = cell.cutoff_to_mesh(ke_cutoff)
else:
mydf = self
with mydf.range_coulomb(omega) as rsh_df:
return rsh_df.get_jk(dm, hermi, kpts, kpts_band, with_j, with_k,
omega=None, exxdiv=exxdiv)
kpts, is_single_kpt = _check_kpts(self, kpts)
if is_single_kpt:
return df_jk.get_jk(self, dm, hermi, kpts[0], kpts_band, with_j,
with_k, exxdiv)
vj = vk = None
if with_k:
vk = df_jk.get_k_kpts(self, dm, hermi, kpts, kpts_band, exxdiv)
if with_j:
vj = df_jk.get_j_kpts(self, dm, hermi, kpts, kpts_band)
return vj, vk
get_eri = get_ao_eri = df_ao2mo.get_eri
ao2mo = get_mo_eri = df_ao2mo.general
ao2mo_7d = df_ao2mo.ao2mo_7d
[docs]
def update_mp(self):
mf = self.copy()
mf.with_df = self
return mf
[docs]
def update_cc(self):
raise NotImplementedError
[docs]
def update(self):
raise NotImplementedError
[docs]
def prange(self, start, stop, step):
'''This is a hook for MPI parallelization. DO NOT use it out of the
scope of AFTDF/GDF/MDF.
'''
return lib.prange(start, stop, step)
################################################################################
# With this function to mimic the molecular DF.loop function, the pbc gamma
# point DF object can be used in the molecular code
[docs]
def loop(self, blksize=None):
cell = self.cell
if cell.dimension == 2 and cell.low_dim_ft_type != 'inf_vacuum':
raise RuntimeError('ERIs of PBC-2D systems are not positive '
'definite. Current API only supports positive '
'definite ERIs.')
if blksize is None:
blksize = self.blockdim
for LpqR, LpqI, sign in self.sr_loop(compact=True, blksize=blksize):
# LpqI should be 0 for gamma point DF
# assert (numpy.linalg.norm(LpqI) < 1e-12)
yield LpqR
[docs]
def get_naoaux(self):
'''The dimension of auxiliary basis at gamma point'''
# determine naoaux with self._cderi, because DF object may be used as CD
# object when self._cderi is provided.
if self._cderi is None:
self.build()
cell = self.cell
if isinstance(self._cderi, numpy.ndarray):
# self._cderi is likely offered by user. Ensure
# cderi.shape = (nkpts,naux,nao_pair)
nao = cell.nao
if self._cderi.shape[-1] == nao:
assert self._cderi.ndim == 4
naux = self._cderi.shape[1]
elif self._cderi.shape[-1] in (nao**2, nao*(nao+1)//2):
assert self._cderi.ndim == 3
naux = self._cderi.shape[1]
else:
raise RuntimeError('cderi shape')
return naux
# self._cderi['j3c/k_id/seg_id']
with h5py.File(self._cderi, 'r') as feri:
key = next(iter(feri[self._dataname].keys()))
dat = feri[f'{self._dataname}/{key}']
if isinstance(dat, h5py.Group):
naux = dat['0'].shape[0]
else:
naux = dat.shape[0]
if (cell.dimension == 2 and cell.low_dim_ft_type != 'inf_vacuum' and
f'{self._dataname}-' in feri):
key = next(iter(feri[f'{self._dataname}-'].keys()))
dat = feri[f'{self._dataname}-/{key}']
if isinstance(dat, h5py.Group):
naux += dat['0'].shape[0]
else:
naux += dat.shape[0]
return naux
DF = GDF
[docs]
class CDERIArray:
'''
Provide numpy APIs to access cderi tensor. This object can be viewed as an
5-dimension array [kpt-i, kpt-j, aux-index, ao-i, ao-j]
'''
def __init__(self, data_group, label='j3c'):
self._data_is_h5obj = isinstance(data_group, h5py.Group)
if not self._data_is_h5obj:
data_group = h5py.File(data_group, 'r')
self.data_group = data_group
if 'kpts' not in data_group:
# TODO: Deprecate the v1 data format
self._data_version = 'v1'
self._cderi = data_group.file.filename
self._label = label
self._kptij_lst = data_group['j3c-kptij'][()]
kpts = unique(self._kptij_lst[:,0])[0]
self.nkpts = nkpts = len(kpts)
if len(self._kptij_lst) not in (nkpts, nkpts**2, nkpts*(nkpts+1)//2):
raise RuntimeError(f'Dimension error for CDERI {self._cderi}')
return
self._data_version = 'v2'
aosym = data_group['aosym'][()]
if isinstance(aosym, bytes):
aosym = aosym.decode()
self.aosym = aosym
self.j3c = data_group[label]
self.kpts = data_group['kpts'][:]
self.nkpts = self.kpts.shape[0]
self.naux = 0
nao_pair = 0
for dat in self.j3c.values():
nao_pair = sum(x.shape[1] for x in dat.values())
self.naux = dat['0'].shape[0]
break
if self.aosym == 's1':
nao = int(nao_pair ** .5)
assert nao ** 2 == nao_pair
self.nao = nao
elif self.aosym == 's2':
self.nao = int((nao_pair * 2)**.5)
else:
raise NotImplementedError
def __del__(self):
if not self._data_is_h5obj:
self.data_group.close()
def __enter__(self):
return self
def __exit__(self, type, value, traceback):
if not self._data_is_h5obj:
self.data_group.close()
def __getitem__(self, slices):
if isinstance(slices, tuple):
ns = len(slices)
if ns < 2:
# patch (:) to slices
slices = slices + (range(self.nkpts),) * (2 - ns)
k_slices = slices[:2]
a_slices = slices[2:]
if isinstance(k_slices[0], int) and isinstance(k_slices[1], int):
return self._load_one(k_slices[0], k_slices[1], ())
else:
k_slices = slices
a_slices = ()
out = numpy.empty((self.nkpts, self.nkpts), dtype=object)
out[k_slices] = True
for ki, kj in numpy.argwhere(out):
out[ki,kj] = self._load_one(ki, kj, a_slices)
return out[k_slices]
def _load_one(self, ki, kj, slices):
if self._data_version == 'v1':
with _load3c(self._cderi, self._label) as fload:
if len(self._kptij_lst) == self.nkpts:
# kptij_lst was generated with option j_only, leading to
# only the diagonal terms
kikj = ki
kpti, kptj = self._kptij_lst[kikj]
elif len(self._kptij_lst) == self.nkpts**2:
kikj = ki * self.nkpts + kj
kpti, kptj = self._kptij_lst[kikj]
elif ki >= kj:
kikj = ki*(ki+1)//2 + kj
kpti, kptj = self._kptij_lst[kikj]
else:
kikj = kj*(kj+1)//2 + ki
kptj, kpti = self._kptij_lst[kikj]
out = fload(kpti, kptj)
return out[slices]
kikj = ki * self.nkpts + kj
kjki = kj * self.nkpts + ki
if self.aosym == 's1' or kikj == kjki:
dat = self.j3c[str(kikj)]
nsegs = len(dat)
out = numpy.hstack([dat[str(i)][slices] for i in range(nsegs)])
elif self.aosym == 's2':
dat_ij = self.j3c[str(kikj)]
dat_ji = self.j3c[str(kjki)]
tril = numpy.hstack([dat_ij[str(i)][slices] for i in range(len(dat_ij))])
triu = numpy.hstack([dat_ji[str(i)][slices] for i in range(len(dat_ji))])
assert tril.dtype == numpy.complex128
naux = self.naux
nao = self.nao
out = numpy.empty((naux, nao*nao), dtype=tril.dtype)
libpbc.PBCunpack_tril_triu(out.ctypes.data_as(ctypes.c_void_p),
tril.ctypes.data_as(ctypes.c_void_p),
triu.ctypes.data_as(ctypes.c_void_p),
ctypes.c_int(naux), ctypes.c_int(nao))
return out
[docs]
def load(self, kpti, kptj):
if self._data_version == 'v1':
with _load3c(self._cderi, self._label) as fload:
return numpy.asarray(fload(kpti, kptj))
ki = member(kpti, self.kpts)
kj = member(kptj, self.kpts)
if len(ki) == 0 or len(kj) == 0:
raise RuntimeError(f'CDERI for kpts ({kpti}, {kptj}) not found')
return self._load_one(ki[0], kj[0], ())
def __array__(self):
'''Create a numpy array'''
return self[:]
class _load3c:
#'''Read cderi from old version pyscf (<= 2.0)'''
'''cderi file may be stored in different formats (version 1 generated from
pyscf-2.0 or older, version 2 from pyscf-2.1 or newer). This function
can read both data formats.
'''
def __init__(self, cderi, label, kpti_kptj=None, kptij_label='j3c-kptij',
ignore_key_error=False):
self.cderi = cderi
self.label = label
self.kptij_label = kptij_label
self.kpti_kptj = kpti_kptj
self.ignore_key_error = ignore_key_error
self.feri = None
self._kptij_lst = None
self._aosym = None
def __enter__(self):
self.feri = h5py.File(self.cderi, 'r')
if self.label not in self.feri:
# Return a size-0 array to skip the loop in sr_loop
if self.ignore_key_error:
return numpy.zeros(0)
else:
raise KeyError('Key "%s" not found' % self.label)
if self.kpti_kptj is None:
return self.getitem
else:
return self.getitem(*self.kpti_kptj)
def __exit__(self, type, value, traceback):
self.feri.close()
@property
def kptij_lst(self):
if self._kptij_lst is None:
if self.data_version == 'v2':
self._kptij_lst = self.feri['kpts'][()]
else:
self._kptij_lst = self.feri[self.kptij_label][()]
return self._kptij_lst
@property
def aosym(self):
if self._aosym is None:
self._aosym = self.feri['aosym'][()]
if isinstance(self._aosym, bytes):
self._aosym = self._aosym.decode()
return self._aosym
@property
def data_version(self):
'''Guess the data format version'''
if 'kpts' in self.feri:
return 'v2'
else:
return 'v1'
def getitem(self, kpti, kptj):
assert self.feri is not None
if self.data_version == 'v2':
kpts = self.kptij_lst
nkpts = len(kpts)
if (isinstance(kpti, (int, numpy.integer)) and
isinstance(kptj, (int, numpy.integer))):
ki = kpti
kj = kptj
else:
ki = member(kpti, kpts)
kj = member(kptj, kpts)
if len(ki) == 0 or len(kj) == 0:
raise RuntimeError(f'CDERI {self.label} for kpts ({kpti}, {kptj}) is '
'not initialized.')
ki = ki[0]
kj = kj[0]
key = f'{self.label}/{ki * nkpts + kj}'
if key not in self.feri:
if self.ignore_key_error:
return numpy.zeros(0)
else:
raise KeyError(f'Key {key} not found')
return _KPair3CLoader(self.feri[self.label], ki, kj, nkpts, self.aosym)
else: # data format version 1
return _getitem(self.feri, self.label, (kpti, kptj), self.kptij_lst,
self.ignore_key_error)
def _getitem(h5group, label, kpti_kptj, kptij_lst, ignore_key_error=False,
aosym=None):
kpti_kptj = numpy.asarray(kpti_kptj)
k_id = member(kpti_kptj, kptij_lst)
if len(k_id) > 0:
key = label + '/' + str(k_id[0])
if key not in h5group:
if ignore_key_error:
return numpy.zeros(0)
else:
raise KeyError('Key "%s" not found' % key)
hermi = False
else:
# swap ki,kj due to the hermiticity
kptji = kpti_kptj[[1,0]]
k_id = member(kptji, kptij_lst)
if len(k_id) == 0:
raise RuntimeError('%s for kpts %s is not initialized.\n'
'You need to update the attribute .kpts then call '
'.build() to initialize %s.'
% (label, kpti_kptj, label))
key = label + '/' + str(k_id[0])
if key not in h5group:
if ignore_key_error:
return numpy.zeros(0)
else:
raise KeyError('Key "%s" not found' % key)
hermi = True
dat = _load_and_unpack(h5group[key],hermi)
return dat
class _load_and_unpack:
'''
This class returns an array-like object to an hdf5 file that can
be sliced, to allow for lazy loading
hermi : boolean
Take the conjugate transpose of the slice
See PR 1086 and Issue 1076
'''
def __init__(self, dat, hermi):
self.dat = dat
self.hermi = hermi
def __getitem__(self, s):
dat = self.dat
if isinstance(dat, h5py.Group):
v = numpy.hstack([dat[str(i)][s] for i in range(len(dat))])
else: # For mpi4pyscf, pyscf-1.5.1 or older
v = numpy.asarray(dat[s])
if self.hermi:
nao = int(numpy.sqrt(v.shape[-1]))
v1 = lib.transpose(v.reshape(-1,nao,nao), axes=(0,2,1)).conj()
return v1.reshape(v.shape)
else:
return v
def __array__(self):
'''Create a numpy array'''
return self[()]
@property
def shape(self):
dat = self.dat
if isinstance(dat, h5py.Group):
all_shape = [dat[str(i)].shape for i in range(len(dat))]
shape = all_shape[0][:-1] + (sum(x[-1] for x in all_shape),)
return shape
else: # For mpi4pyscf, pyscf-1.5.1 or older
return dat.shape
class _KPair3CLoader:
def __init__(self, dat, ki, kj, nkpts, aosym):
self.dat = dat
self.kikj = ki * nkpts + kj
self.kjki = kj * nkpts + ki
self.nkpts = nkpts
self.nsegs = len(dat[str(self.kikj)])
self.aosym = aosym
def __getitem__(self, s):
if self.aosym == 's1' or self.kikj == self.kjki:
dat = self.dat[str(self.kikj)]
out = numpy.hstack([dat[str(i)][s] for i in range(self.nsegs)])
elif self.aosym == 's2':
dat_ij = self.dat[str(self.kikj)]
dat_ji = self.dat[str(self.kjki)]
tril = numpy.hstack([dat_ij[str(i)][s] for i in range(self.nsegs)])
triu = numpy.hstack([dat_ji[str(i)][s] for i in range(self.nsegs)])
assert tril.dtype == numpy.complex128
naux, nao_pair = tril.shape
nao = int((nao_pair * 2)**.5)
out = numpy.empty((naux, nao*nao), dtype=tril.dtype)
libpbc.PBCunpack_tril_triu(out.ctypes.data_as(ctypes.c_void_p),
tril.ctypes.data_as(ctypes.c_void_p),
triu.ctypes.data_as(ctypes.c_void_p),
ctypes.c_int(naux), ctypes.c_int(nao))
else:
raise ValueError(f'Unknown aosym {self.aosym}')
return out
def __array__(self):
'''Create a numpy array'''
return self[()]
@property
def shape(self):
dat = self.dat[str(self.kikj)]
shapes = [dat[str(i)].shape for i in range(self.nsegs)]
naux = shapes[0][0]
nao_pair = sum([shape[1] for shape in shapes])
if self.aosym == 's1' or self.kikj == self.kjki:
return (naux, nao_pair)
else:
nao = int((nao_pair * 2)**.5)
return (naux, nao*nao)
def _gaussian_int(cell):
r'''Regular gaussian integral \int g(r) dr^3'''
return ft_ao.ft_ao(cell, numpy.zeros((1,3)))[0].real