def get_irrep_nelec(mol, mo_coeff, mo_occ, s=None):
'''Alpha/beta electron numbers for each irreducible representation.
Args:
mol : an instance of :class:`Mole`
To provide irrep_id, and spin-adapted basis
mo_occ : a list of 1D ndarray
Regular occupancy, without grouping for irreps
mo_coeff : a list of 2D ndarray
Regular orbital coefficients, without grouping for irreps
Returns:
irrep_nelec : dict
The number of alpha/beta electrons for each irrep {'ir_name':(int,int), ...}.
Examples:
>>> mol = gto.M(atom='O 0 0 0; H 0 0 1; H 0 1 0', basis='ccpvdz', symmetry=True, charge=1, spin=1, verbose=0)
>>> mf = scf.UHF(mol)
>>> mf.scf()
-75.623975516256721
>>> scf.uhf_symm.get_irrep_nelec(mol, mf.mo_coeff, mf.mo_occ)
{'A1': (3, 3), 'A2': (0, 0), 'B1': (1, 1), 'B2': (1, 0)}
'''
orbsyma = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb,
mo_coeff[0], s)
orbsymb = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb,
mo_coeff[1], s)
orbsyma = numpy.array(orbsyma)
orbsymb = numpy.array(orbsymb)
irrep_nelec = dict([(mol.irrep_name[k], (int(sum(mo_occ[0][orbsyma==ir])),
int(sum(mo_occ[1][orbsymb==ir]))))
for k, ir in enumerate(mol.irrep_id)])
return irrep_nelec
def get_grad(self, mo_coeff, mo_occ, fock=None):
mol = self.mol
if not mol.symmetry:
return uhf.UHF.get_grad(self, mo_coeff, mo_occ, fock)
if fock is None:
dm1 = self.make_rdm1(mo_coeff, mo_occ)
fock = self.get_hcore(mol) + self.get_veff(self.mol, dm1)
ovlp_ao = self.get_ovlp()
orbsyma = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff[0], ovlp_ao, False)
orbsymb = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff[1], ovlp_ao, False)
orbsyma = numpy.asarray(orbsyma)
orbsymb = numpy.asarray(orbsymb)
occidxa = mo_occ[0] > 0
occidxb = mo_occ[1] > 0
viridxa = ~occidxa
viridxb = ~occidxb
ga = reduce(numpy.dot, (mo_coeff[0][:,viridxa].T.conj(), fock[0],
mo_coeff[0][:,occidxa]))
ga[orbsyma[viridxa].reshape(-1,1)!=orbsyma[occidxa]] = 0
gb = reduce(numpy.dot, (mo_coeff[1][:,viridxb].T.conj(), fock[1],
mo_coeff[1][:,occidxb]))
gb[orbsymb[viridxb].reshape(-1,1)!=orbsymb[occidxb]] = 0
return numpy.hstack((ga.ravel(), gb.ravel()))
def gen_g_hop(self, mo_coeff, mo_occ, fock_ao=None, h1e=None):
mol = self._scf.mol
if mol.symmetry:
ovlp_ao = self._scf.get_ovlp()
self._orbsym =(symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, mo_coeff[0], s=ovlp_ao),
symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, mo_coeff[1], s=ovlp_ao))
return gen_g_hop_uhf(self, mo_coeff, mo_occ, fock_ao, h1e)
def kernel(self, mo_coeff=None, ci0=None, macro=None, micro=None, callback=None, _kern=None):
if mo_coeff is None:
mo_coeff = self.mo_coeff
else:
self.mo_coeff = mo_coeff
if macro is None:
macro = self.max_cycle_macro
if micro is None:
micro = self.max_cycle_micro
if callback is None:
callback = self.callback
if _kern is None:
_kern = mc1step.kernel
if self.verbose > logger.QUIET:
pyscf.gto.mole.check_sanity(self, self._keys, self.stdout)
self.mol.check_sanity(self)
self.dump_flags()
# irrep_name = self.mol.irrep_name
irrep_name = self.mol.irrep_id
try:
self.orbsym = symm.label_orb_symm(self.mol, irrep_name, self.mol.symm_orb, mo_coeff, s=self._scf.get_ovlp())
except ValueError:
logger.warn(self, "mc1step_symm symmetrizes input orbitals")
s = self._scf.get_ovlp()
mo_coeff = symm.symmetrize_orb(self.mol, mo_coeff, s=s)
diag = numpy.einsum("ki,ki->i", mo_coeff, numpy.dot(s, mo_coeff))
mo_coeff = numpy.einsum("ki,i->ki", mo_coeff, 1 / numpy.sqrt(diag))
self.orbsym = symm.label_orb_symm(self.mol, irrep_name, self.mol.symm_orb, mo_coeff, s=s)
if not hasattr(self.fcisolver, "orbsym") or not self.fcisolver.orbsym:
ncore = self.ncore
nocc = self.ncore + self.ncas
self.fcisolver.orbsym = self.orbsym[ncore:nocc]
logger.debug(self, "Active space irreps %s", str(self.fcisolver.orbsym))
self.converged, self.e_tot, e_cas, self.ci, self.mo_coeff = _kern(
self,
mo_coeff,
tol=self.conv_tol,
conv_tol_grad=self.conv_tol_grad,
macro=macro,
micro=micro,
ci0=ci0,
callback=callback,
verbose=self.verbose,
)
logger.note(self, "CASSCF energy = %.15g", self.e_tot)
return self.e_tot, e_cas, self.ci, self.mo_coeff
def test_kernel_symm(self):
mol = gto.Mole()
mol.verbose = 0
mol.output = None
mol.atom = [
['O', ( 0., 0. , 0. )],
['H', ( 0., -0.757, 0.587)],
['H', ( 0., 0.757 , 0.587)],]
mol.basis = 'sto-3g'
mol.symmetry = 1
mol.build()
m = scf.RHF(mol).run()
norb = m.mo_coeff.shape[1]
nelec = mol.nelectron - 2
h1e = reduce(numpy.dot, (m.mo_coeff.T, scf.hf.get_hcore(mol), m.mo_coeff))
eri = ao2mo.incore.full(m._eri, m.mo_coeff)
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, m.mo_coeff)
myci = selected_ci_symm.SCI().set(orbsym=orbsym, select_cutoff=.5e-3)
e1, c1 = myci.kernel(h1e, eri, norb, nelec)
myci = direct_spin1_symm.FCISolver().set(orbsym=orbsym)
e2, c2 = myci.kernel(h1e, eri, norb, nelec)
self.assertAlmostEqual(e1, e2, 6)
c2_cut = selected_ci.from_fci(c2, c1._strs, norb, nelec)
self.assertAlmostEqual(abs(numpy.dot(c1.ravel(), c2_cut.ravel())), 1, 6)
myci = selected_ci_symm.SCI().set(orbsym=orbsym, select_cutoff=1e-5)
e1, c1 = myci.kernel(h1e, eri, norb, nelec, ci0=c2_cut, wfnsym=0)
self.assertAlmostEqual(e1, e2, 9)
c2_cut = selected_ci.from_fci(c2, c1._strs, norb, nelec)
self.assertAlmostEqual(abs(numpy.dot(c1.ravel(), c2_cut.ravel())), 1, 9)
def get_occ(self, mo_energy, mo_coeff=None):
''' We cannot assume default mo_energy value, because the orbital
energies are sorted after doing SCF. But in this function, we need
the orbital energies are grouped by symmetry irreps
'''
mol = self.mol
nirrep = len(mol.symm_orb)
if mo_coeff is not None:
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
else:
orbsym = [numpy.repeat(ir, mol.symm_orb[i].shape[1])
for i, ir in enumerate(mol.irrep_id)]
orbsym = numpy.hstack(orbsym)
mo_occ = numpy.zeros_like(mo_energy)
mo_e_left = []
idx_e_left = []
nelec_fix = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = numpy.where(orbsym == ir)[0]
if irname in self.irrep_nelec:
n = self.irrep_nelec[irname]
e_idx = numpy.argsort(mo_energy[ir_idx])
mo_occ[ir_idx[e_idx[:n//2]]] = 2
nelec_fix += n
else:
idx_e_left.append(ir_idx)
nelec_float = mol.nelectron - nelec_fix
assert(nelec_float >= 0)
if nelec_float > 0:
idx_e_left = numpy.hstack(idx_e_left)
mo_e_left = mo_energy[idx_e_left]
mo_e_sort = numpy.argsort(mo_e_left)
occ_idx = idx_e_left[mo_e_sort[:(nelec_float//2)]]
mo_occ[occ_idx] = 2
viridx = (mo_occ==0)
if self.verbose < logger.INFO or viridx.sum() == 0:
return mo_occ
ehomo = max(mo_energy[mo_occ>0 ])
elumo = min(mo_energy[mo_occ==0])
noccs = []
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = (orbsym == ir)
noccs.append(int(mo_occ[ir_idx].sum()))
if ehomo in mo_energy[ir_idx]:
irhomo = irname
if elumo in mo_energy[ir_idx]:
irlumo = irname
logger.info(self, 'H**O (%s) = %.15g LUMO (%s) = %.15g',
irhomo, ehomo, irlumo, elumo)
if self.verbose >= logger.DEBUG:
logger.debug(self, 'irrep_nelec = %s', noccs)
_dump_mo_energy(mol, mo_energy, mo_occ, ehomo, elumo, orbsym)
return mo_occ
def get_irrep_nelec(mol, mo_coeff, mo_occ, s=None):
'''Electron numbers for each irreducible representation.
Args:
mol : an instance of :class:`Mole`
To provide irrep_id, and spin-adapted basis
mo_coeff : 2D ndarray
Regular orbital coefficients, without grouping for irreps
mo_occ : 1D ndarray
Regular occupancy, without grouping for irreps
Returns:
irrep_nelec : dict
The number of electrons for each irrep {'ir_name':int,...}.
Examples:
>>> mol = gto.M(atom='O 0 0 0; H 0 0 1; H 0 1 0', basis='ccpvdz', symmetry=True, verbose=0)
>>> mf = scf.RHF(mol)
>>> mf.scf()
-76.016789472074251
>>> scf.hf_symm.get_irrep_nelec(mol, mf.mo_coeff, mf.mo_occ)
{'A1': 6, 'A2': 0, 'B1': 2, 'B2': 2}
'''
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_coeff, s)
orbsym = numpy.array(orbsym)
irrep_nelec = dict([(mol.irrep_name[k], int(sum(mo_occ[orbsym==ir])))
for k, ir in enumerate(mol.irrep_id)])
return irrep_nelec
def get_grad(self, mo_coeff, mo_occ, fock=None):
mol = self.mol
if not self.mol.symmetry:
return rohf.ROHF.get_grad(self, mo_coeff, mo_occ, fock)
if fock is None:
dm1 = self.make_rdm1(mo_coeff, mo_occ)
fock = self.get_hcore(mol) + self.get_veff(self.mol, dm1)
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
sym_allow = orbsym.reshape(-1,1) == orbsym
occidxa = mo_occ > 0
occidxb = mo_occ == 2
viridxa = ~occidxa
viridxb = ~occidxb
focka = reduce(numpy.dot, (mo_coeff.T, fock[0], mo_coeff))
fockb = reduce(numpy.dot, (mo_coeff.T, fock[1], mo_coeff))
uniq_var_a = viridxa.reshape(-1,1) & occidxa
uniq_var_b = viridxb.reshape(-1,1) & occidxb
g = numpy.zeros_like(focka)
g[uniq_var_a] = focka[uniq_var_a]
g[uniq_var_b] += fockb[uniq_var_b]
g[~sym_allow] = 0
return g[uniq_var_a | uniq_var_b].ravel()
def from_chkfile(filename, chkfile, tol=TOL, float_format=DEFAULT_FLOAT_FORMAT):
'''Read SCF results from PySCF chkfile and transform 1-electron,
2-electron integrals using the SCF orbitals. The transformed integrals is
written to FCIDUMP'''
from pyscf import scf, symm
with open(filename, 'w') as fout:
mol, scf_rec = scf.chkfile.load_scf(chkfile)
mo_coeff = numpy.array(scf_rec['mo_coeff'])
nmo = mo_coeff.shape[1]
if mol.symmetry:
orbsym = symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, mo_coeff, check=False)
write_head(fout, nmo, mol.nelectron, mol.spin, orbsym)
else:
write_head(fout, nmo, mol.nelectron, mol.spin)
eri = ao2mo.full(mol, mo_coeff, verbose=0)
write_eri(fout, ao2mo.restore(8, eri, nmo), nmo, tol, float_format)
t = mol.intor_symmetric('int1e_kin')
v = mol.intor_symmetric('int1e_nuc')
h = reduce(numpy.dot, (mo_coeff.T, t+v, mo_coeff))
write_hcore(fout, h, nmo, tol, float_format)
output_format = ' ' + float_format + ' 0 0 0 0\n'
fout.write(output_format % mol.energy_nuc())
def orbital_coeff(mol, fout, mo_coeff, spin='Alpha', symm=None, ene=None,
occ=None, ignore_h=False):
from pyscf.symm import label_orb_symm
if ignore_h:
mol, mo_coeff = remove_high_l(mol, mo_coeff)
aoidx = order_ao_index(mol)
nmo = mo_coeff.shape[1]
if symm is None:
symm = ['A']*nmo
if mol.symmetry:
try:
symm = label_orb_symm(mol, mol.irrep_name, mol.symm_orb,
mo_coeff, tol=1e-5)
except ValueError as e:
logger.warn(mol, str(e))
if ene is None:
ene = numpy.arange(nmo)
assert(spin == 'Alpha' or spin == 'Beta')
if occ is None:
occ = numpy.zeros(nmo)
neleca, nelecb = mol.nelec
if spin == 'Alpha':
occ[:neleca] = 1
else:
occ[:nelecb] = 1
fout.write('[MO]\n')
for imo in range(nmo):
fout.write(' Sym= %s\n' % symm[imo])
fout.write(' Ene= %15.10g\n' % ene[imo])
fout.write(' Spin= %s\n' % spin)
fout.write(' Occup= %10.5f\n' % occ[imo])
for i,j in enumerate(aoidx):
fout.write(' %3d %18.14g\n' % (i+1, mo_coeff[j,imo]))
def gen_g_hop(self, mo_coeff, mo_occ, fock_ao=None, h1e=None):
mol = self._scf.mol
if mol.symmetry:
# label the symmetry every time calling gen_g_hop because kernel function may
# change mo_coeff ordering after calling self.eig
self._orbsym = symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, mo_coeff, s=self._scf.get_ovlp())
return gen_g_hop_rohf(self, mo_coeff, mo_occ, fock_ao, h1e)
def test_symmetrize_space(self):
from pyscf import gto, symm, scf
mol = gto.M(atom = 'C 0 0 0; H 1 1 1; H -1 -1 1; H 1 -1 -1; H -1 1 -1',
basis = 'sto3g', verbose=0)
mf = scf.RHF(mol).run()
mol.build(0, 0, symmetry='D2')
mo = symm.symmetrize_space(mol, mf.mo_coeff)
irreps = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mo)
self.assertEqual(irreps, ['A','A','A','B1','B1','B2','B2','B3','B3'])
def analyze(self, verbose=logger.DEBUG):
from pyscf.tools import dump_mat
mo_energy = self.mo_energy
mo_occ = self.mo_occ
mo_coeff = self.mo_coeff
log = logger.Logger(self.stdout, verbose)
mol = self.mol
nirrep = len(mol.irrep_id)
ovlp_ao = self.get_ovlp()
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_coeff,
s=ovlp_ao)
orbsym = numpy.array(orbsym)
wfnsym = 0
ndoccs = []
nsoccs = []
for k,ir in enumerate(mol.irrep_id):
ndoccs.append(sum(orbsym[mo_occ==2] == ir))
nsoccs.append(sum(orbsym[mo_occ==1] == ir))
if nsoccs[k] % 2:
wfnsym ^= ir
if mol.groupname in ('Dooh', 'Coov'):
log.info('TODO: total symmetry for %s', mol.groupname)
else:
log.info('total symmetry = %s',
symm.irrep_id2name(mol.groupname, wfnsym))
log.info('occupancy for each irrep: ' + (' %4s'*nirrep),
*mol.irrep_name)
log.info('double occ ' + (' %4d'*nirrep), *ndoccs)
log.info('single occ ' + (' %4d'*nirrep), *nsoccs)
log.info('**** MO energy ****')
irname_full = {}
for k,ir in enumerate(mol.irrep_id):
irname_full[ir] = mol.irrep_name[k]
irorbcnt = {}
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.info('MO #%d (%s #%d), energy= %.15g occ= %g',
k+1, irname_full[j], irorbcnt[j], mo_energy[k], mo_occ[k])
if verbose >= logger.DEBUG:
label = mol.spheric_labels(True)
molabel = []
irorbcnt = {}
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
molabel.append('#%-d(%s #%d)' % (k+1, irname_full[j], irorbcnt[j]))
log.debug(' ** MO coefficients **')
dump_mat.dump_rec(mol.stdout, mo_coeff, label, molabel, start=1)
dm = self.make_rdm1(mo_coeff, mo_occ)
return self.mulliken_meta(mol, dm, s=ovlp_ao, verbose=verbose)
def __init__(self):
self.__dict__.update(cis.__dict__)
self.h1e = reduce(numpy.dot, (mo.T, scf.hf.get_hcore(mol), mo))
self.eri = ao2mo.outcore.full_iofree(mol, mo)
self.eci = None
self.ci = None
if mol.symmetry:
self.orbsym = symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, mo)
self._keys = set(self.__dict__.keys())
def analyze(mf, verbose=logger.DEBUG, **kwargs):
'''Analyze the given SCF object: print orbital energies, occupancies;
print orbital coefficients; Occupancy for each irreps; Mulliken population analysis
'''
from pyscf.lo import orth
from pyscf.tools import dump_mat
mol = mf.mol
if not mol.symmetry:
return hf.analyze(mf, verbose, **kwargs)
mo_energy = mf.mo_energy
mo_occ = mf.mo_occ
mo_coeff = mf.mo_coeff
log = logger.Logger(mf.stdout, verbose)
nirrep = len(mol.irrep_id)
ovlp_ao = mf.get_ovlp()
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_coeff,
s=ovlp_ao, check=False)
orbsym = numpy.array(orbsym)
wfnsym = 0
noccs = [sum(orbsym[mo_occ>0]==ir) for ir in mol.irrep_id]
log.note('total symmetry = %s', symm.irrep_id2name(mol.groupname, wfnsym))
log.note('occupancy for each irrep: ' + (' %4s'*nirrep), *mol.irrep_name)
log.note('double occ ' + (' %4d'*nirrep), *noccs)
log.note('**** MO energy ****')
irname_full = {}
for k,ir in enumerate(mol.irrep_id):
irname_full[ir] = mol.irrep_name[k]
irorbcnt = {}
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note('MO #%d (%s #%d), energy= %.15g occ= %g',
k+1, irname_full[j], irorbcnt[j], mo_energy[k], mo_occ[k])
if verbose >= logger.DEBUG:
label = mol.spheric_labels(True)
molabel = []
irorbcnt = {}
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
molabel.append('#%-d(%s #%d)' % (k+1, irname_full[j], irorbcnt[j]))
log.debug(' ** MO coefficients (expansion on meta-Lowdin AOs) **')
orth_coeff = orth.orth_ao(mol, 'meta_lowdin', s=ovlp_ao)
c = reduce(numpy.dot, (orth_coeff.T, ovlp_ao, mo_coeff))
dump_mat.dump_rec(mf.stdout, c, label, molabel, start=1, **kwargs)
dm = mf.make_rdm1(mo_coeff, mo_occ)
return mf.mulliken_meta(mol, dm, s=ovlp_ao, verbose=log)
def label_symmetry_(mc, mo_coeff):
#irrep_name = mc.mol.irrep_name
irrep_name = mc.mol.irrep_id
s = mc._scf.get_ovlp()
try:
mc.orbsym = symm.label_orb_symm(mc.mol, irrep_name,
mc.mol.symm_orb, mo_coeff, s=s)
except ValueError:
logger.warn(mc, 'mc1step_symm symmetrizes input orbitals')
ncore = mc.ncore
nocc = mc.ncore + mc.ncas
mo_cor = symm.symmetrize_space(mc.mol, mo_coeff[:, :ncore], s=s)
mo_act = symm.symmetrize_space(mc.mol, mo_coeff[:,ncore:nocc], s=s)
mo_vir = symm.symmetrize_space(mc.mol, mo_coeff[:,nocc: ], s=s)
mo_coeff = numpy.hstack((mo_cor,mo_act,mo_vir))
mc.orbsym = symm.label_orb_symm(mc.mol, irrep_name,
mc.mol.symm_orb, mo_coeff, s=s)
if not hasattr(mc.fcisolver, 'orbsym') or not mc.fcisolver.orbsym:
ncore = mc.ncore
nocc = mc.ncore + mc.ncas
mc.fcisolver.orbsym = mc.orbsym[ncore:nocc]
logger.debug(mc, 'Active space irreps %s', str(mc.fcisolver.orbsym))
def get_grad(self, mo_coeff, mo_occ, fock=None):
mol = self.mol
if fock is None:
dm1 = self.make_rdm1(mo_coeff, mo_occ)
fock = self.get_hcore(mol) + self.get_veff(self.mol, dm1)
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
occidx = mo_occ > 0
viridx = ~occidx
g = reduce(numpy.dot, (mo_coeff[:,viridx].T.conj(), fock,
mo_coeff[:,occidx])) * 2
sym_allow = orbsym[viridx].reshape(-1,1) == orbsym[occidx]
g[~sym_allow] = 0
return g.ravel()
def write_integrals(xci, orb):
mol = xci.mol
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, orb)
h1e = reduce(numpy.dot, (orb.T, xci.get_hcore(), orb))
norb = orb.shape[1]
if xci._eri is not None:
h2e = ao2mo.restore(1, ao2mo.full(xci._eri, orb), norb)
else:
h2e = ao2mo.restore(1, ao2mo.full(mol, orb), norb)
with h5py.File(xci.integralfile, 'w') as f:
f['h1e'] = h1e
f['h2e'] = h2e
f['norb' ] = numpy.array(norb, dtype=numpy.int32)
f['group' ] = mol.groupname
f['orbsym'] = numpy.asarray(orbsym, dtype=numpy.int32)
f['ecore' ] = mol.energy_nuc()
def get_orbsym(mol, mo_coeff, s=None, check=False):
if mo_coeff is None:
orbsym = numpy.hstack([[ir] * mol.symm_orb[i].shape[1]
for i, ir in enumerate(mol.irrep_id)])
elif getattr(mo_coeff, 'orbsym', None) is not None:
orbsym = mo_coeff.orbsym
else:
nao = mo_coeff.shape[0] // 2
if isinstance(s, numpy.ndarray):
assert(s.size == nao**2 or numpy.allclose(s[:nao,:nao], s[nao:,nao:]))
s = s[:nao,:nao]
mo_a = mo_coeff[:nao].copy()
mo_b = mo_coeff[nao:]
zero_alpha_idx = numpy.linalg.norm(mo_a, axis=0) < 1e-7
mo_a[:,zero_alpha_idx] = mo_b[:,zero_alpha_idx]
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb,
mo_a, s, check)
return numpy.asarray(orbsym)
def generate_hamiltonian():
### PYSCF INPUT
r0 = 1.50
molecule = '''
Cr
Cr 1 {}
'''.format(r0)
charge = 0
spin = 0
basis_set = 'def2-svp'
### TPSCI BASIS INPUT
orb_basis = 'scf'
cas = True
cas_nstart = 12
cas_nstop = 42
loc_start = 1
loc_stop = 6
cas_nel = 24
def ordering_diatomics_cr(mol,C):
# {{{
##DZ basis diatomics reordering with frozen 1s
orb_type = ['s','pz','dz','px','dxz','py','dyz','dx2-y2','dxy']
ref = np.zeros(C.shape[1])
## Find dimension of each space
dim_orb = []
for orb in orb_type:
print("Orb type",orb)
idx = 0
for label in mol.ao_labels():
if orb in label:
#print(label)
idx += 1
##frozen 1s orbitals
if orb == 's':
idx -= 6
elif orb == 'px':
idx -=2
elif orb == 'py':
idx -=2
elif orb == 'pz':
idx -=2
dim_orb.append(idx)
print(idx)
new_idx = []
## Find orbitals corresponding to each orb space
for i,orb in enumerate(orb_type):
print("Orbital type:",orb)
from pyscf import mo_mapping
s_pop = mo_mapping.mo_comps(orb, mol, C)
print(s_pop)
ref += s_pop
cas_list = s_pop.argsort()[-dim_orb[i]:]
print('cas_list', np.array(cas_list))
new_idx.extend(cas_list)
#print(orb,' population for active space orbitals', s_pop[cas_list])
ao_labels = mol.ao_labels()
#idx = mol.search_ao_label(['N.*s'])
#for i in idx:
# print(i, ao_labels[i])
print(ref)
print(new_idx)
for label in mol.ao_labels():
print(label)
return new_idx
# }}}
# basis is SVP read comments by alex thom paper DOI:10.1021/acs.jctc.9b01023
from pyscf import gto
basis_set={'Cr': gto.parse('''
BASIS "ao basis" PRINT
#BASIS SET: (14s,8p,5d) -> [5s,2p,2d]
Cr S
51528.086349 0.14405823106E-02
7737.2103487 0.11036202287E-01
1760.3748470 0.54676651806E-01
496.87706544 0.18965038103
161.46520598 0.38295412850
55.466352268 0.29090050668
Cr S
107.54732999 -0.10932281100
12.408671897 0.64472599471
5.0423628826 0.46262712560
Cr S
8.5461640165 -0.22711013286
1.3900441221 0.73301527591
0.56066602876 0.44225565433
Cr S
0.71483705972E-01 1.0000000000
Cr S
0.28250687604E-01 1.0000000000
Cr P
640.48536096 0.96126715203E-02
150.69711194 0.70889834655E-01
47.503755296 0.27065258990
16.934120165 0.52437343414
6.2409680590 0.34107994714
Cr P
3.0885463206 0.33973986903
1.1791047769 0.57272062927
0.43369774432 0.24582728206
Cr D
27.559479426 0.30612488044E-01
7.4687020327 0.15593270944
2.4345903574 0.36984421276
0.78244754808 0.47071118077
Cr D
0.21995774311 0.33941649889
END''')}
### TPSCI CLUSTER INPUT
init_fspace = ((1, 1),(3, 3),(3, 3),(3, 3), (1, 1), (1, 1))
blocks = [range(0,4),range(4,10),range(10,16),range(16,22),range(22,26),range(26,30)]
# Integrals from pyscf
#Integrals from pyscf
pmol = PyscfHelper()
pmol.init(molecule,charge,spin,basis_set,orb_basis,
cas_nstart=cas_nstart,cas_nstop=cas_nstop,cas_nel=cas_nel,cas=True,
loc_nstart=loc_start,loc_nstop = loc_stop)
h = pmol.h
g = pmol.g
ecore = pmol.ecore
print("Ecore:%16.8f"%ecore)
C = pmol.C
K = pmol.K
mol = pmol.mol
mo_energy = pmol.mf.mo_energy
dm_aa = pmol.dm_aa
dm_bb = pmol.dm_bb
do_fci = 0
do_hci = 0
do_tci = 1
if do_fci:
efci, fci_dim = run_fci_pyscf(h,g,nelec,ecore=ecore)
if do_hci:
ehci, hci_dim = run_hci_pyscf(h,g,nelec,ecore=ecore,select_cutoff=5e-4,ci_cutoff=5e-4)
#cluster using hcore
idx = ordering_diatomics_cr(mol,C)
h,g = reorder_integrals(idx,h,g)
C = C[:,idx]
mo_energy = mo_energy[idx]
dm_aa = dm_aa[:,idx]
dm_aa = dm_aa[idx,:]
dm_bb = dm_bb[:,idx]
dm_bb = dm_bb[idx,:]
print(dm_aa)
from pyscf import molden
molden.from_mo(pmol.mol, 'h8.molden', C)
print(h)
mol = pmol.mol
if mol.symmetry == True:
from pyscf import symm
mo = symm.symmetrize_orb(mol, C)
osym = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mo)
#symm.addons.symmetrize_space(mol, mo, s=None, check=True, tol=1e-07)
for i in range(len(osym)):
print("%4d %8s %16.8f"%(i+1,osym[i],mo_energy[i]))
clusters = []
for ci,c in enumerate(blocks):
clusters.append(Cluster(ci,c))
print(" Clusters:")
[print(ci) for ci in clusters]
clustered_ham = ClusteredOperator(clusters, core_energy=ecore)
print(" Add 1-body terms")
clustered_ham.add_local_terms()
clustered_ham.add_1b_terms(h)
print(" Add 2-body terms")
clustered_ham.add_2b_terms(g)
# intial state
ci_vector = ClusteredState(clusters)
ci_vector.init(init_fspace)
ci_vector.print()
# do cmf
do_cmf = 1
if do_cmf:
# Get CMF reference
e_cmf, cmf_conv, rdm_a, rdm_b = cmf(clustered_ham, ci_vector, h, g, max_iter=10, dm_guess=(dm_aa, dm_bb), diis=True)
print(" Final CMF Total Energy %12.8f" %(e_cmf + ecore))
# build cluster basis and operator matrices using CMF optimized density matrices
for ci_idx, ci in enumerate(clusters):
print(ci)
fspaces_i = init_fspace[ci_idx]
delta_e = 2
fspaces_i = ci.possible_fockspaces( delta_elec=(fspaces_i[0], fspaces_i[1], delta_e) )
print()
print(" Form basis by diagonalizing local Hamiltonian for cluster: ",ci_idx)
ci.form_fockspace_eigbasis(h, g, fspaces_i, max_roots=100, rdm1_a=rdm_a, rdm1_b=rdm_b)
print(" Build mats for cluster ",ci.idx)
ci.build_op_matrices()
ci.build_local_terms(h,g)
hamiltonian_file = open('hamiltonian_file', 'wb')
pickle.dump(clustered_ham, hamiltonian_file)
print(" Done.")
def get_occ(self, mo_energy=None, mo_coeff=None, orbsym=None):
if mo_energy is None: mo_energy = self.mo_energy
mol = self.mol
if not self.mol.symmetry:
return rohf.ROHF.get_occ(self, mo_energy, mo_coeff)
if mo_coeff is None or self._focka_ao is None:
mo_ea = mo_eb = mo_energy
else:
mo_ea = numpy.einsum('ik,ik->k', mo_coeff,
self._focka_ao.dot(mo_coeff))
mo_eb = numpy.einsum('ik,ik->k', mo_coeff,
self._fockb_ao.dot(mo_coeff))
nmo = mo_ea.size
mo_occ = numpy.zeros(nmo)
if orbsym is None:
if mo_coeff is not None:
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
else:
orbsym = [
numpy.repeat(ir, mol.symm_orb[i].shape[1])
for i, ir in enumerate(mol.irrep_id)
]
orbsym = numpy.hstack(orbsym)
else:
orbsym = numpy.asarray(orbsym)
assert (mo_energy.size == orbsym.size)
float_idx = []
neleca_fix = 0
nelecb_fix = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = numpy.where(orbsym == ir)[0]
if irname in self.irrep_nelec:
if isinstance(self.irrep_nelec[irname], (int, numpy.integer)):
nelecb = self.irrep_nelec[irname] // 2
neleca = self.irrep_nelec[irname] - nelecb
else:
neleca, nelecb = self.irrep_nelec[irname]
mo_occ[ir_idx] = rohf._fill_rohf_occ(mo_energy[ir_idx],
mo_ea[ir_idx],
mo_eb[ir_idx], nelecb,
neleca - nelecb)
neleca_fix += neleca
nelecb_fix += nelecb
else:
float_idx.append(ir_idx)
nelec_float = mol.nelectron - neleca_fix - nelecb_fix
assert (nelec_float >= 0)
if len(float_idx) > 0:
float_idx = numpy.hstack(float_idx)
nopen = mol.spin - (neleca_fix - nelecb_fix)
ncore = (nelec_float - nopen) // 2
mo_occ[float_idx] = rohf._fill_rohf_occ(mo_energy[float_idx],
mo_ea[float_idx],
mo_eb[float_idx], ncore,
nopen)
ncore = self.nelec[1]
nocc = self.nelec[0]
nopen = nocc - ncore
vir_idx = (mo_occ == 0)
if self.verbose >= logger.INFO and nocc < nmo and ncore > 0:
ehomo = max(mo_energy[mo_occ > 0])
elumo = min(mo_energy[mo_occ == 0])
ndoccs = []
nsoccs = []
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = (orbsym == ir)
ndoccs.append(numpy.count_nonzero(mo_occ[ir_idx] == 2))
nsoccs.append(numpy.count_nonzero(mo_occ[ir_idx] == 1))
if ehomo in mo_energy[ir_idx]:
irhomo = irname
if elumo in mo_energy[ir_idx]:
irlumo = irname
# to help self.eigh compute orbital energy
self._irrep_doccs = ndoccs
self._irrep_soccs = nsoccs
logger.info(self, 'H**O (%s) = %.15g LUMO (%s) = %.15g', irhomo,
ehomo, irlumo, elumo)
logger.debug(self, 'double occ irrep_nelec = %s', ndoccs)
logger.debug(self, 'single occ irrep_nelec = %s', nsoccs)
#_dump_mo_energy(mol, mo_energy, mo_occ, ehomo, elumo, orbsym,
# verbose=self.verbose)
if nopen > 0:
core_idx = mo_occ == 2
open_idx = mo_occ == 1
vir_idx = mo_occ == 0
logger.debug(
self,
' Roothaan | alpha | beta'
)
logger.debug(self,
' Highest 2-occ = %18.15g | %18.15g | %18.15g',
max(mo_energy[core_idx]), max(mo_ea[core_idx]),
max(mo_eb[core_idx]))
logger.debug(self,
' Lowest 0-occ = %18.15g | %18.15g | %18.15g',
min(mo_energy[vir_idx]), min(mo_ea[vir_idx]),
min(mo_eb[vir_idx]))
for i in numpy.where(open_idx)[0]:
logger.debug(
self, ' 1-occ = %18.15g | %18.15g | %18.15g',
mo_energy[i], mo_ea[i], mo_eb[i])
numpy.set_printoptions(threshold=nmo)
logger.debug(self, ' Roothaan mo_energy =\n%s', mo_energy)
logger.debug1(self, ' alpha mo_energy =\n%s', mo_ea)
logger.debug1(self, ' beta mo_energy =\n%s', mo_eb)
numpy.set_printoptions(threshold=1000)
return mo_occ
def writeNevpt2Integrals(mc, dm1, dm2, dm1eff, aaavsplit, frozen):
eris = _ERIS(mc, mc.mo_coeff)
nocc = mc.ncore + mc.ncas
ncore = mc.ncore
nact = mc.ncas
norbs = eris['ppaa'].shape[0]
nvirt = norbs - ncore - nact
eris_sp = {}
#eris_sp['cvcv']= numpy.zeros(shape=(1,1)) #numpy.zeros(shape=(mc.ncore, norbs-mc.ncore-mc.ncas, mc.ncore, norbs-mc.ncas-mc.ncore))
eris_sp['h1eff'] = 1. * eris['h1eff'] #numpy.zeros(shape=(norbs, norbs))
int1 = reduce(numpy.dot, (mc.mo_coeff.T, mc.get_hcore(), mc.mo_coeff))
#eris_sp['h1eff'] = makeheff(int1, eris['papa'], eris['ppaa'], dm1, ncore, nvirt)
eris_sp['h1eff'][:mc.ncore, :mc.ncore] += numpy.einsum(
'abcd,cd', eris['ppaa'][:mc.ncore, :mc.ncore, :, :], dm1eff)
eris_sp['h1eff'][:mc.ncore, :mc.ncore] -= numpy.einsum(
'abcd,bd', eris['papa'][:mc.ncore, :, :mc.ncore, :], dm1eff) * 0.5
eris_sp['h1eff'][mc.ncas + mc.ncore:, mc.ncas + mc.ncore:] += numpy.einsum(
'abcd,cd', eris['ppaa'][mc.ncas + mc.ncore:,
mc.ncas + mc.ncore:, :, :], dm1eff)
eris_sp['h1eff'][mc.ncas + mc.ncore:, mc.ncas + mc.ncore:] -= numpy.einsum(
'abcd,bd', eris['papa'][mc.ncas + mc.ncore:, :,
mc.ncas + mc.ncore:, :], dm1eff) * 0.5
offdiagonal = 0.0
#zero out off diagonal core
for k in range(mc.ncore):
for l in range(mc.ncore):
if (k != l):
offdiagonal = max(abs(offdiagonal), abs(eris_sp['h1eff'][k,
l]))
#zero out off diagonal virtuals
for k in range(mc.ncore + mc.ncas, norbs):
for l in range(mc.ncore + mc.ncas, norbs):
if (k != l):
offdiagonal = max(abs(offdiagonal), abs(eris_sp['h1eff'][k,
l]))
if (abs(offdiagonal) > 1e-6):
print "WARNING ***** Have to use natorual orbitals from casscf ****"
print "offdiagonal elements ", offdiagonal
eriscvcv = eris['cvcv']
if (not isinstance(eris['cvcv'], type(eris_sp['h1eff']))):
#eriscvcv = h5py.File(eris['cvcv'].name,'r')["eri_mo"]
eriscvcv = lib.chkfile.load(
eris['cvcv'].name,
"eri_mo") #h5py.File(eris['cvcv'].name,'r')["eri_mo"]
eris_sp['cvcv'] = eriscvcv.reshape(mc.ncore, norbs - mc.ncore - mc.ncas,
mc.ncore, norbs - mc.ncore - mc.ncas)
import os
os.system("mkdir int")
numpy.save(
"int/W:caac",
numpy.asfortranarray(eris['papa'][frozen:mc.ncore, :,
frozen:mc.ncore, :].transpose(
0, 3, 1, 2)))
numpy.save(
"int/W:aeca",
numpy.asfortranarray(eris['papa'][frozen:mc.ncore, :,
mc.ncore + mc.ncas:, :].transpose(
1, 2, 0, 3)))
numpy.save(
"int/W:ccaa",
numpy.asfortranarray(eris['papa'][frozen:mc.ncore, :,
frozen:mc.ncore, :].transpose(
0, 2, 1, 3)))
numpy.save(
"int/W:eeaa",
numpy.asfortranarray(eris['papa'][mc.ncore + mc.ncas:, :,
mc.ncore + mc.ncas:, :].transpose(
0, 2, 1, 3)))
numpy.save(
"int/W:caca",
numpy.asfortranarray(eris['ppaa'][frozen:mc.ncore,
frozen:mc.ncore, :, :].transpose(
0, 2, 1, 3)))
numpy.save(
"int/W:eaca",
numpy.asfortranarray(eris['ppaa'][mc.ncore + mc.ncas:,
frozen:mc.ncore, :, :].transpose(
0, 2, 1, 3)))
numpy.save(
"int/W:eecc",
numpy.asfortranarray(eris_sp['cvcv'][frozen:, :,
frozen:, :].transpose(1, 3, 0,
2)))
numpy.save(
"int/W:ccae",
numpy.asfortranarray(eris['pacv'][frozen:mc.ncore, :,
frozen:, :].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:aaaa",
numpy.asfortranarray(eris['ppaa'][mc.ncore:mc.ncore + mc.ncas,
mc.ncore:mc.ncore +
mc.ncas, :, :].transpose(0, 2, 1,
3)))
numpy.save(
"int/W:eeca",
numpy.asfortranarray(eris['pacv'][mc.ncore + mc.ncas:, :,
frozen:, :].transpose(3, 0, 2, 1)))
numpy.save("int/int1eff",
numpy.asfortranarray(eris_sp['h1eff'][frozen:, frozen:]))
numpy.save("int/E1.npy", numpy.asfortranarray(dm1))
numpy.save("int/E2.npy", numpy.asfortranarray(dm2))
#numpy.save("int/E3",dm3)
#numpy.save("int/E3B.npy", dm3.transpose(0,3,1,4,2,5))
#numpy.save("int/E3C.npy", dm3.transpose(5,0,2,4,1,3))
nc = mc.ncore + mc.ncas
energyE0 = 1.0 * numpy.einsum('ij,ij', eris_sp['h1eff'][ncore:nc,
ncore:nc], dm1)
energyE0 += 0.5 * numpy.einsum(
'ijkl,ijkl', eris['ppaa'][mc.ncore:mc.ncore + mc.ncas,
mc.ncore:mc.ncore + mc.ncas, :, :].transpose(
0, 2, 1, 3), dm2)
mo = mc.mo_coeff
dmcore = numpy.dot(mo[:, :ncore], mo[:, :ncore].T) * 2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj - vk * 0.5, mo))
energyE0 += numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
energyE0 += mc.mol.energy_nuc()
print "Energy = ", energyE0
from pyscf import symm
mol = mc.mol
orbsymout = []
orbsym = []
if (mol.symmetry):
orbsym = symm.label_orb_symm(mc.mol,
mc.mol.irrep_id,
mc.mol.symm_orb,
mc.mo_coeff,
s=mc._scf.get_ovlp())
if mol.symmetry and orbsym:
if mol.groupname.lower() == 'dooh':
orbsymout = [dmrg_sym.IRREP_MAP['D2h'][i % 10] for i in orbsym]
elif mol.groupname.lower() == 'coov':
orbsymout = [dmrg_sym.IRREP_MAP['C2v'][i % 10] for i in orbsym]
else:
orbsymout = [dmrg_sym.IRREP_MAP[mol.groupname][i] for i in orbsym]
else:
orbsymout = []
ncore = mc.ncore
mo = mc.mo_coeff
dmcore = numpy.dot(mo[:, :ncore], mo[:, :ncore].T) * 2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj - vk * 0.5, mo))
energy_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
print energy_core
virtOrbs = range(ncore + mc.ncas, eris_sp['h1eff'].shape[0])
chunks = len(virtOrbs) / aaavsplit
virtRange = [
virtOrbs[i:i + chunks] for i in xrange(0, len(virtOrbs), chunks)
]
for K in range(aaavsplit):
currentOrbs = range(ncore, mc.ncas + ncore) + virtRange[K]
fout = open('FCIDUMP_aaav%d' % (K), 'w')
#tools.fcidump.write_head(fout, eris_sp['h1eff'].shape[0]-ncore, mol.nelectron-2*ncore, orbsym= orbsymout[ncore:])
tools.fcidump.write_head(
fout,
mc.ncas + len(virtRange[K]),
mol.nelectron - 2 * ncore,
orbsym=(orbsymout[ncore:ncore + mc.ncas] +
orbsymout[virtRange[K][0]:virtRange[K][-1] + 1]))
ij = ncore * (ncore + 1) / 2
for i in range(len(currentOrbs)):
for j in range(ncore, mc.ncas + ncore):
for k in range(mc.ncas):
for l in range(k + 1):
I = currentOrbs[i]
if abs(eris['ppaa'][I, j, k, l]) > 1.e-8:
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (eris['ppaa'][I,j,k,l], i+1, j+1-ncore, k+1, l+1))
h1eff = numpy.zeros(shape=(mc.ncas + len(virtRange[K]),
mc.ncas + len(virtRange[K])))
h1eff[:mc.ncas, :mc.ncas] = eris_sp['h1eff'][ncore:ncore + mc.ncas,
ncore:ncore + mc.ncas]
h1eff[mc.ncas:,
mc.ncas:] = eris_sp['h1eff'][virtRange[K][0]:virtRange[K][-1] +
1,
virtRange[K][0]:virtRange[K][-1] +
1]
h1eff[:mc.ncas,
mc.ncas:] = eris_sp['h1eff'][ncore:ncore + mc.ncas,
virtRange[K][0]:virtRange[K][-1] +
1]
h1eff[mc.ncas:, :mc.ncas] = eris_sp['h1eff'][
virtRange[K][0]:virtRange[K][-1] + 1, ncore:ncore + mc.ncas]
tools.fcidump.write_hcore(fout,
h1eff,
mc.ncas + len(virtRange[K]),
tol=1e-8)
#tools.fcidump.write_hcore(fout, eris_sp['h1eff'][virtRange[K][0]:virtRange[K][-1]+1, virtRange[K][0]:virtRange[K][-1]+1], len(virtRange[K]), tol=1e-8)
fout.write(' %17.9e 0 0 0 0\n' %
(mol.energy_nuc() + energy_core - energyE0))
fout.close()
nc = ncore + mc.ncas
fout = open('FCIDUMP_aaac', 'w')
tools.fcidump.write_head(fout,
nc - frozen,
mol.nelectron - 2 * frozen,
orbsym=orbsymout[frozen:nc])
for i in range(frozen, nc):
for j in range(ncore, nc):
for k in range(ncore, nc):
for l in range(ncore, k + 1):
if abs(eris['ppaa'][i, j, k - ncore, l - ncore]) > 1.e-8:
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (eris['ppaa'][i,j,k-ncore,l-ncore], i+1-frozen, j+1-frozen, k+1-frozen, l+1-frozen))
dmrge = energyE0 - mol.energy_nuc() - energy_core
ecore_aaac = 0.0
for i in range(frozen, ncore):
ecore_aaac += 2.0 * eris_sp['h1eff'][i, i]
tools.fcidump.write_hcore(fout,
eris_sp['h1eff'][frozen:nc, frozen:nc],
nc - frozen,
tol=1e-8)
fout.write(' %17.9e 0 0 0 0\n' % (-dmrge - ecore_aaac))
fout.close()
return norbs, energyE0
def hchain(n_sites, r=1.8, pg_reorder=True, **kwargs):
"""
1D Hydrogen chain model. r in bohr.
"""
if 'scratch' in kwargs:
import os
if not os.path.isdir(kwargs['scratch']):
os.mkdir(kwargs['scratch'])
os.environ['TMPDIR'] = kwargs['scratch']
from pyscf import gto, scf, symm, ao2mo
BOHR = 0.52917721092 # Angstroms
r = r * BOHR
mol = gto.M(atom=[['H', (i * r, 0, 0)] for i in range(n_sites)],
basis='sto6g',
verbose=0,
symmetry='d2h')
pg = mol.symmetry.lower()
# Reorder
if pg == 'd2h':
fcidump_sym = [
"Ag", "B3u", "B2u", "B1g", "B1u", "B2g", "B3g", "Au"
]
optimal_reorder = [
"Ag", "B1u", "B3u", "B2g", "B2u", "B3g", "B1g", "Au"
]
elif pg == 'c1':
fcidump_sym = ["A"]
optimal_reorder = ["A"]
else:
assert False
# SCF
m = scf.RHF(mol)
m.kernel()
mo_coeff = m.mo_coeff
n_ao = mo_coeff.shape[0]
n_mo = mo_coeff.shape[1]
orb_sym_str = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb,
mo_coeff)
orb_sym = np.array([fcidump_sym.index(i) + 1 for i in orb_sym_str])
# Sort the orbitals by symmetry for more efficient DMRG
if pg_reorder:
idx = np.argsort([optimal_reorder.index(i) for i in orb_sym_str])
orb_sym = orb_sym[idx]
mo_coeff = mo_coeff[:, idx]
ridx = np.argsort(idx)
else:
ridx = np.array(list(range(n_mo)), dtype=int)
h1e = mo_coeff.T @ m.get_hcore() @ mo_coeff
g2e = ao2mo.restore(8, ao2mo.kernel(mol, mo_coeff), n_mo)
ecore = mol.energy_nuc()
del m, mol
with HamilTools._init(**kwargs) as ():
fcidump = FCIDUMP()
n_elec = n_sites
tol = 1E-13
mh1e = np.zeros((n_sites * (n_sites + 1) // 2))
k = 0
for i in range(0, n_sites):
for j in range(0, i + 1):
assert abs(h1e[i, j] - h1e[j, i]) < tol
mh1e[k] = h1e[i, j]
k += 1
mg2e = g2e.flatten().copy()
mh1e[np.abs(mh1e) < tol] = 0.0
mg2e[np.abs(mg2e) < tol] = 0.0
fcidump.initialize_su2(n_sites, n_elec, 0, 1, ecore, mh1e, mg2e)
fcidump.orb_sym = VectorUInt8(orb_sym)
with HamilTools._from_fcidump(fcidump, pg=pg) as hamil:
yield hamil
mol = gto.M(atom='C 0 0 0; C 0 0 1.24253', basis='cc-pvdz', symmetry=1,
symmetry_subgroup='D2h')
# run HF and store HF results in mf
mf = scf.RHF(mol).run()
# run MP2 and store MP2 results in mp2
mp2 = mp.MP2(mf).run()
rdm1 = numpy.diag(mf.mo_occ) # The HF 1-particle density matrix in MO representation
rdm1 += mp2.make_rdm1() # Add the correlation part
natocc, natorb = numpy.linalg.eigh(rdm1)
# Note natorb is in MO basis representation
natorb = numpy.dot(mf.mo_coeff, natorb)
try:
natorb_sym = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, natorb)
print(natorb_sym)
except ValueError:
print('The diagonalization for rdm1 breaks the symmetry of the degenerated natural orbitals.')
print('\nIn eigenvalue sovler symm.eigh, we diagonalize the density matrix with the MO symmetry '
'information. The eigenvectors are all symmetry adapted.')
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mf.mo_coeff)
natocc, natorb = symm.eigh(rdm1, orbsym)
natorb = numpy.dot(mf.mo_coeff, natorb)
natorb_sym = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, natorb)
print(natorb_sym)
def canonicalize(mc, mo_coeff=None, ci=None, eris=None, sort=False,
cas_natorb=False, casdm1=None, verbose=logger.NOTE):
'''Canonicalized CASCI/CASSCF orbitals of effecitve Fock matrix.
Effective Fock matrix is built with one-particle density matrix (see
also :func:`mcscf.casci.get_fock`)
Args:
mc : a CASSCF/CASCI object or RHF object
Returns:
A tuple, (natural orbitals, CI coefficients, orbital energies)
The orbital energies are the diagonal terms of general Fock matrix.
'''
from pyscf.lo import orth
from pyscf.tools import dump_mat
log = logger.new_logger(mc, verbose)
if mo_coeff is None: mo_coeff = mc.mo_coeff
if ci is None: ci = mc.ci
if casdm1 is None:
casdm1 = mc.fcisolver.make_rdm1(ci, mc.ncas, mc.nelecas)
ncore = mc.ncore
nocc = ncore + mc.ncas
nmo = mo_coeff.shape[1]
fock_ao = mc.get_fock(mo_coeff, ci, eris, casdm1, verbose)
fock = reduce(numpy.dot, (mo_coeff.T, fock_ao, mo_coeff))
mo_energy = fock.diagonal().copy()
if cas_natorb:
mo_coeff1, ci, occ = mc.cas_natorb(mo_coeff, ci, eris, sort, casdm1,
verbose)
ma = mo_coeff1[:,ncore:nocc]
mo_energy[ncore:nocc] = numpy.einsum('ji,ji->i', ma, fock_ao.dot(ma))
else:
# Keep the active space unchanged by default. The rotation in active space
# may cause problem for external CI solver eg DMRG.
mo_coeff1 = numpy.empty_like(mo_coeff)
mo_coeff1[:,ncore:nocc] = mo_coeff[:,ncore:nocc]
if ncore > 0:
# note the last two args of ._eig for mc1step_symm
# mc._eig function is called to handle symmetry adapated fock
w, c1 = mc._eig(fock[:ncore,:ncore], 0, ncore)
if sort:
idx = numpy.argsort(w.round(9), kind='mergesort')
w = w[idx]
c1 = c1[:,idx]
mo_coeff1[:,:ncore] = numpy.dot(mo_coeff[:,:ncore], c1)
mo_energy[:ncore] = w
if nmo-nocc > 0:
w, c1 = mc._eig(fock[nocc:,nocc:], nocc, nmo)
if sort:
idx = numpy.argsort(w.round(9), kind='mergesort')
w = w[idx]
c1 = c1[:,idx]
mo_coeff1[:,nocc:] = numpy.dot(mo_coeff[:,nocc:], c1)
mo_energy[nocc:] = w
if hasattr(mo_coeff, 'orbsym'):
if sort:
orbsym = symm.label_orb_symm(mc.mol, mc.mol.irrep_id,
mc.mol.symm_orb, mo_coeff1)
else:
orbsym = mo_coeff.orbsym
mo_coeff1 = lib.tag_array(mo_coeff1, orbsym=orbsym)
if log.verbose >= logger.DEBUG:
for i in range(nmo):
log.debug('i = %d <i|F|i> = %12.8f', i+1, mo_energy[i])
# still return ci coefficients, in case the canonicalization funciton changed
# cas orbitals, the ci coefficients should also be updated.
return mo_coeff1, ci, mo_energy
def get_mo_from_h5(mol, h5fname, symmetry=None):
''' Get MO vectors for a pyscf molecule from an h5 file written by OpenMolcas
Args:
mol : instance gto.mole
Must be in the same point group as the OpenMolcas calculation,
or set the symmetry argument
h5fname : str
Path to an h5 file generated by OpenMolcas containing (at
least) groups 'BASIS_FUNCTION_IDS', 'MO_OCCUPATIONS',
'MO_VECTORS', and 'MO_ENERGIES' and additionally 'DESYM_MATRIX'
and 'DESYM_BASIS_FUNCTION_IDS' if symmetry is used.
Kwargs:
symmetry : str
Point group of the calculation in OpenMolcas. If not provided,
mol.groupname is used instead
Returns:
mo_coeff : ndarray of shape (nao_nr, nao_nr)
'''
if symmetry is not None:
mol = mol.copy()
mol.build(symmetry=symmetry)
nao = mol.nao_nr()
with h5py.File(h5fname, 'r') as f:
try:
molcas_basids = f['DESYM_BASIS_FUNCTION_IDS'][()]
molcas_usymm = f['DESYM_MATRIX'][()].reshape(nao, nao)
except KeyError:
assert (not mol.symmetry
), "Can't find desym_ data; mol.symmetry = {}".format(
mol.symmetry)
molcas_basids = f['BASIS_FUNCTION_IDS'][()]
molcas_coeff = f['MO_VECTORS'][()]
mo_energy = f['MO_ENERGIES'][()]
mo_occ = f['MO_OCCUPATIONS'][()]
idx_ao = []
for (c, n, l, m) in molcas_basids:
# 0-index atom list in PySCF, 1-index atom list in Molcas
c -= 1
# Actual principal quantum number in PySCF, 1-indexed list in Molcas
n += l
# l=1, ml=(-1,0,1) is (x,y,z) in PySCF, (y,z,x) in Molcas
if l == 1:
m = m - 2 if m > 0 else m + 1
idx_ao.append(mol.search_ao_nr(c, l, m, n))
idx_ao = np.argsort(np.asarray(idx_ao))
if mol.symmetry:
# I have to figure out what order the Molcas irreps are in on the fly
# because it seems to change depending on the xyz
molcas_usymm = molcas_usymm[:, idx_ao]
proj = np.stack([(np.dot(molcas_usymm, ir_coeff)**2).sum(1)
for ir_coeff in mol.symm_orb],
axis=0)
errstr = ("Can't interpret h5 symmetry information; wrong mol? "
" <mol.symm_orb|desym_matrix> =\n{}").format(proj)
assert (np.allclose(np.amax(proj), 1)), errstr
ix_irrep = np.argmax(proj, axis=0)
uniq_idx = np.sort(np.unique(ix_irrep, return_index=True)[1])
uniq_idx = np.append(uniq_idx, len(ix_irrep))
nmo_irrep = []
for ix, i in enumerate(uniq_idx[:-1]):
j = uniq_idx[ix + 1]
assert (len(np.unique(ix_irrep[i:j])) == 1), errstr
nmo_irrep.append(j - i)
nmo_irrep = np.asarray(nmo_irrep)
usymm_irrep_offset = np.cumsum(nmo_irrep) - nmo_irrep
coeff_irrep_offset = np.cumsum(nmo_irrep**2) - nmo_irrep**2
mo_coeff = np.zeros((nao, nao), dtype=np.float_)
for m_ir, usymm_off, coeff_off in zip(nmo_irrep, usymm_irrep_offset,
coeff_irrep_offset):
i, j = usymm_off, usymm_off + m_ir
u, v = coeff_off, coeff_off + (m_ir**2)
usymm = molcas_usymm[i:j, :].T
coeff = molcas_coeff[u:v].reshape(m_ir, m_ir).T
mo_coeff[:, i:j] = np.dot(usymm, coeff)
else:
assert (molcas_coeff.shape == (
nao**2, )), 'mo_vectors.shape = {} but {} AOs'.format(
molcas_coeff.shape, nao)
mo_coeff = molcas_coeff.reshape(nao, nao)[:, idx_ao].T
# 'mergesort' keeps degenerate or active-space orbitals in the provided order!
# idx_ene = np.argsort (mo_energy, kind='mergesort')
# modified by Dayou: sort by mo_occ first, then mo_energy
sort_key = np.min(mo_energy) * 100000 * mo_occ + mo_energy
idx_ene = np.argsort(sort_key, kind='mergesort')
mo_coeff = mo_coeff[:, idx_ene]
mo_occ = mo_occ[idx_ene]
mo_energy = mo_energy[idx_ene]
if mol.verbose > logger.INFO:
fname = str(mol.output)[:-4] + "_h5debug.molden"
molden.from_mo(mol, fname, mo_coeff, occ=mo_occ, ene=mo_energy)
if mol.symmetry: # assert (symmetry is right)
try:
orbsym = label_orb_symm(mol, mol.irrep_name, mol.symm_orb,
mo_coeff)
except ValueError as e:
raise ValueError(("Problem understanding Molcas symmetry?\n"
"{}").format(str(e)))
return mo_coeff
mf.verbose = 3
mf.scf()
#############################
# Build the Hamiltonian #
#############################
L = mf.mol.nao_nr()
N = mf.mol.nelectron
CONST = mf.mol.energy_nuc()
OEImo = np.dot(
np.dot(mf.mo_coeff.T,
mf.mol.intor('cint1e_kin_sph') +
mf.mol.intor('cint1e_nuc_sph')), mf.mo_coeff)
TEImo = ao2mo.outcore.full_iofree(mf.mol, mf.mo_coeff,
compact=False).reshape(L, L, L, L)
orb2irrep = np.array(symm.label_orb_symm(mf.mol, mf.mol.irrep_id,
mf.mol.symm_orb, mf.mo_coeff),
dtype=ctypes.c_int)
for cnt in range(len(orb2irrep)):
orb2irrep[cnt] = orb2irrep[cnt] % 10
#######################################
# PySCF FCI calculation and 4-RDM #
#######################################
fci_solver = fci.FCI(mol, mf.mo_coeff)
fci_energy, fci_vector = fci_solver.kernel()
print "PySCF FCI energy =", fci_energy + CONST
pyscf_start = time.time()
dm1, dm2, dm3, dm4 = fci.rdm.make_dm1234('FCI4pdm_kern_spin0', fci_vector,
fci_vector, L, N)
dm1, dm2, dm3, dm4 = fci.rdm.reorder_dm1234(dm1,
dm2,
def label_symmetry_(mc, mo_coeff, ci0=None):
log = logger.Logger(mc.stdout, mc.verbose)
#irrep_name = mc.mol.irrep_name
irrep_name = mc.mol.irrep_id
s = mc._scf.get_ovlp()
try:
orbsym = scf.hf_symm.get_orbsym(mc._scf.mol, mo_coeff, s, True)
except ValueError:
log.warn('mc1step_symm symmetrizes input orbitals')
ncore = mc.ncore
nocc = mc.ncore + mc.ncas
mo_cor = symm.symmetrize_space(mc.mol, mo_coeff[:, :ncore], s=s, check=False)
mo_act = symm.symmetrize_space(mc.mol, mo_coeff[:,ncore:nocc], s=s, check=False)
mo_vir = symm.symmetrize_space(mc.mol, mo_coeff[:,nocc: ], s=s, check=False)
mo_coeff = numpy.hstack((mo_cor,mo_act,mo_vir))
orbsym = symm.label_orb_symm(mc.mol, irrep_name,
mc.mol.symm_orb, mo_coeff, s=s)
mo_coeff_with_orbsym = lib.tag_array(mo_coeff, orbsym=orbsym)
active_orbsym = getattr(mc.fcisolver, 'orbsym', [])
if (not hasattr(active_orbsym, '__len__')) or len(active_orbsym) == 0:
ncore = mc.ncore
nocc = mc.ncore + mc.ncas
mc.fcisolver.orbsym = orbsym[ncore:nocc]
log.debug('Active space irreps %s', str(mc.fcisolver.orbsym))
wfnsym = 0
if getattr(mc.fcisolver, 'wfnsym', None) is not None:
wfnsym = mc.fcisolver.wfnsym
elif ci0 is None:
# Guess wfnsym based on HF determinant. mo_coeff may not be HF
# canonical orbitals. Some checks are needed to ensure that mo_coeff
# are derived from the symmetry adapted SCF calculations.
if mo_coeff is mc._scf.mo_coeff:
wfnsym = 0
for ir in orbsym[mc._scf.mo_occ == 1]:
wfnsym ^= ir
mc.fcisolver.wfnsym = wfnsym
log.debug('Set CASCI wfnsym %s based on HF determinant', wfnsym)
elif hasattr(mo_coeff, 'orbsym'): # It may be reordered SCF orbitals
ncore = mc.ncore
nocc = mc.ncore + mc.ncas
cas_orb = mo_coeff[:,ncore:nocc]
s = reduce(numpy.dot, (cas_orb.T, mc._scf.get_ovlp(), mc._scf.mo_coeff))
if numpy.all(numpy.max(s, axis=1) > 1-1e-9):
idx = numpy.argmax(s, axis=1)
cas_orbsym = orbsym[ncore:nocc]
cas_occ = mc._scf.mo_occ[idx]
wfnsym = 0
for ir in cas_orbsym[cas_occ == 1]:
wfnsym ^= ir
mc.fcisolver.wfnsym = wfnsym
log.debug('Active space are constructed from canonical SCF '
'orbitals %s', idx)
log.debug('Set CASCI wfnsym %s based on HF determinant', wfnsym)
elif hasattr(mc.fcisolver, 'guess_wfnsym'):
wfnsym = mc.fcisolver.guess_wfnsym(mc.ncas, mc.nelecas, ci0, verbose=log)
log.debug('CASCI wfnsym %s (based on CI initial guess)', wfnsym)
if isinstance(wfnsym, (int, numpy.integer)):
wfnsym = symm.irrep_id2name(mc.mol.groupname, wfnsym)
log.info('Active space CI wfn symmetry = %s', wfnsym)
return mo_coeff_with_orbsym
'B3': 2
},
'Cs': {
"A'": 1,
'A"': 2
},
'C2': {
'A': 1,
'B': 2
},
'Ci': {
'Ag': 1,
'Au': 2
},
'C1': {
'A': 1,
}
}
orbsym = [
MOLPRO_ID[mol.groupname][i]
for i in symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, c)
]
tools.fcidump.from_integrals('fcidump.example3',
h1e,
eri,
c.shape[1],
mol.nelectron,
ms=0,
orbsym=orbsym)
)
fspt.write('La matriz D es:\n')
for i in range(nmo):
for j in range(nmo):
fspt.write('%i %i %.16f\n' % ((i + 1), (j + 1), rdm1[i, j]))
fspt.write('La matriz d es:\n')
for i in range(nmo):
for j in range(nmo):
for k in range(nmo):
for l in range(nmo):
if (abs(rdm2[i, j, k, l]) > 1e-12):
fspt.write('%i %i %i %i %.16f\n' %
((i + 1), (j + 1), (k + 1),
(l + 1), rdm2[i, j, k, l]))
fspt.close()
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb,
mc.mo_coeff[:, :nmo])
natocc, natorb = symm.eigh(-rdm1, orbsym)
for i, k in enumerate(numpy.argmax(abs(natorb), axis=0)):
if natorb[k, i] < 0:
natorb[:, i] *= -1
natorb = numpy.dot(mc.mo_coeff[:, :nmo], natorb)
natocc = -natocc
with open('n2_cas.det', 'w') as f3:
write_ci(f3, mc.ci, mc.ncas, mc.nelecas, mc.ncore)
with open('n2_ref_nat.mol', 'w') as f2:
molden.header(mol, f2)
molden.orbital_coeff(mol, f2, natorb, occ=natocc)
with open('n2_ref.mol', 'w') as f2:
molden.header(mol, f2)
molden.orbital_coeff(mol,
f2,
def __init__(self, mol_or_hdf5, c=None, network=None, verbose=None):
'''Initializing the T3NS calculation.
Args:
mol_or_hdf5: An instance of :class:`Mole` from PySCF
or a string to a path of the hdf5 file. In this case c and network
should be left as defaults.
c: The orbital coefficients.
The default are the RHF orbitals.
network: Network of the tensor network.
This can be the string 'DMRG' for a linear chain or 'T3NS' for a
T3NS that is radially extended (i.e. the maximal distance between
two sites is minimal). An instance of :class:`Network` is also
accepted for custom networks or a path to a network file.
Default is 'T3NS' if Mole instance was passed, else None.
'''
from pyscf import symm
if isinstance(mol_or_hdf5, pyscf.gto.Mole):
# Initialize with RHF
mol = mol_or_hdf5
if network is None:
network = 'T3NS'
if verbose is None:
self.verbose = mol.verbose
self.mol = mol
# if no orbital coefficients are given, use RHF orbitals
if c is None:
myhf = pyscf.scf.RHF(mol)
myhf.verbose = self.verbose
myhf.kernel()
c = myhf.mo_coeff
self._c = c
self._mol = mol
self._eri = pyscf.ao2mo.kernel(mol, c)
self.symmetries = ['Z2', 'U1', 'SU2']
self.target = [int(mol.nelectron % 2), mol.nelectron, mol.spin]
try:
irrep_ids = symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, c)
newsym = mol.groupname
if mol.groupname == 'Dooh' or mol.groupname == 'Coov':
newsym = 'D2h' if mol.groupname else 'C2v'
if self.verbose > 1:
print(f'Changed point group from {mol.groupname} to '
f'{newsym}')
# mod 10 needed for translation Coov and Dooh
# See https://sunqm.github.io/pyscf/symm.html
self._pg_irrep = [
symm.irrep_id2name(newsym, int(ii % 10))
for ii in irrep_ids
]
self.symmetries.append(newsym)
self.target.append(symm.irrep_id2name(newsym, 0))
except (ValueError, TypeError):
self._pg_irrep = None
if isinstance(network, netw.Network):
self._netw = network
elif network == 'DMRG' or network == 'T3NS':
isDMRG = network == 'DMRG'
self._netw = netw.Network(c.shape[1], isDMRG=isDMRG)
# exchange matrix
# Kij = numpy.zeros((c.shape[1],) * 2)
# trids = numpy.tril_indices(c.shape[1], 0)
# for el, r, c in zip(self._eri.diagonal(), trids[0], trids[1]):
# Kij[r, c] = el
# Kij[c, r] = el
# cost = self._netw.optimize(Kij)
# if self.verbose >= 2:
# print(f'Optimization Exchange-cost: {cost}')
elif isinstance(network, str):
self._netw = netw.Network()
self._netw.readnetworkfile(network)
else:
raise ValueError(f'{network} is invalid for network')
self._netw.pass_network()
elif isinstance(mol_or_hdf5, str):
# h5path = mol_or_hdf5
if verbose is None:
self.verbose = 1
if c is not None or network is not None:
raise ValueError(
'A hdf5 file does not expect a defined c or network')
raise ValueError('Need to implement hdf5 readin still')
else:
raise ValueError(
'Expects a Mole instance or a path to a hdf5 file')
def analyze(self, verbose=logger.DEBUG, **kwargs):
from pyscf.lo import orth
from pyscf.tools import dump_mat
if not self.mol.symmetry:
return rohf.ROHF.analyze(self, verbose, **kwargs)
mo_energy = self.mo_energy
mo_occ = self.mo_occ
mo_coeff = self.mo_coeff
log = logger.Logger(self.stdout, verbose)
mol = self.mol
nirrep = len(mol.irrep_id)
ovlp_ao = self.get_ovlp()
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_coeff,
ovlp_ao, False)
orbsym = numpy.array(orbsym)
wfnsym = 0
ndoccs = []
nsoccs = []
for k, ir in enumerate(mol.irrep_id):
ndoccs.append(sum(orbsym[mo_occ == 2] == ir))
nsoccs.append(sum(orbsym[mo_occ == 1] == ir))
if nsoccs[k] % 2:
wfnsym ^= ir
if mol.groupname in ('Dooh', 'Coov'):
log.info('TODO: total symmetry for %s', mol.groupname)
else:
log.info('total symmetry = %s',
symm.irrep_id2name(mol.groupname, wfnsym))
log.info('occupancy for each irrep: ' + (' %4s' * nirrep),
*mol.irrep_name)
log.info('double occ ' + (' %4d' * nirrep), *ndoccs)
log.info('single occ ' + (' %4d' * nirrep), *nsoccs)
log.info('**** MO energy ****')
irname_full = {}
for k, ir in enumerate(mol.irrep_id):
irname_full[ir] = mol.irrep_name[k]
irorbcnt = {}
if self._focka_ao is None:
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note('MO #%-3d (%s #%-2d), energy= %-18.15g occ= %g',
k + 1, irname_full[j], irorbcnt[j], mo_energy[k],
mo_occ[k])
else:
mo_ea = numpy.einsum('ik,ik->k', mo_coeff,
self._focka_ao.dot(mo_coeff))
mo_eb = numpy.einsum('ik,ik->k', mo_coeff,
self._fockb_ao.dot(mo_coeff))
log.note(
' Roothaan | alpha | beta'
)
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note(
'MO #%-4d(%-3s #%-2d) energy= %-18.15g | %-18.15g | %-18.15g occ= %g',
k + 1, irname_full[j], irorbcnt[j], mo_energy[k], mo_ea[k],
mo_eb[k], mo_occ[k])
if verbose >= logger.DEBUG:
label = mol.spheric_labels(True)
molabel = []
irorbcnt = {}
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
molabel.append('#%-d(%s #%d)' %
(k + 1, irname_full[j], irorbcnt[j]))
log.debug(' ** MO coefficients (expansion on meta-Lowdin AOs) **')
orth_coeff = orth.orth_ao(mol, 'meta_lowdin', s=ovlp_ao)
c = reduce(numpy.dot, (orth_coeff.T, ovlp_ao, mo_coeff))
dump_mat.dump_rec(self.stdout,
c,
label,
molabel,
start=1,
**kwargs)
dm = self.make_rdm1(mo_coeff, mo_occ)
return self.mulliken_meta(mol, dm, s=ovlp_ao, verbose=verbose)
def run(b, dm_guess, mo_guess, ci=None):
mol = gto.Mole()
mol.verbose = 5
mol.output = 'cr2-%3.2f.out' % b
mol.atom = [
['Cr', (0., 0., -b / 2)],
['Cr', (0., 0., b / 2)],
]
mol.basis = 'ccpvdzdk'
mol.symmetry = True
mol.build()
mf = scf.RHF(mol).x2c()
mf.max_cycle = 100
mf.conv_tol = 1e-9
mf.kernel(dm_guess)
#---------------------
# CAS(12,12)
#
# The active space of CAS(12,42) can be generated by function sort_mo_by_irrep,
# or AVAS, dmet_cas methods. Here we first run a CAS(12,12) calculation and
# using the lowest CASSCF canonicalized orbitals in the CAS(12,42) calculation
# as the core and valence orbitals.
mc = mcscf.CASSCF(mf, 12, 12)
if mo_guess is None:
# the initial guess for first calculation
ncas = {
'A1g': 2,
'E1gx': 1,
'E1gy': 1,
'E2gx': 1,
'E2gy': 1,
'A1u': 2,
'E1ux': 1,
'E1uy': 1,
'E2ux': 1,
'E2uy': 1
}
mo_guess = mcscf.sort_mo_by_irrep(mc, mf.mo_coeff, ncas, ncore)
else:
mo_guess = mcscf.project_init_guess(mc, mo_guess)
# Projection may destroy the spatial symmetry of the MCSCF orbitals.
try:
print(
'Irreps of the projected CAS(12,12) orbitals',
symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_guess))
except:
print('Projected CAS(12,12) orbitals does not have right symmetry')
# FCI solver with multi-threads is not stable enough for this sytem
mc.fcisolver.threads = 1
# To avoid spin contamination
mc.fix_spin_()
# By default, canonicalization as well as the CASSCF optimization do not
# change the orbital symmetry labels. "Orbital energy" mc.mo_energy, the
# diagonal elements of the general fock matrix, may have wrong ordering.
# To use the lowest CASSCF orbitals as the core + active orbitals in the next
# step, we have to sort the orbitals based on the "orbital energy". This
# operation will change the orbital symmetry labels.
mc.sorting_mo_energy = True
# "mc.natorb = True" will transform the active space, to its natural orbital
# representation. By default, the active space orbitals are NOT reordered
# even the option sorting_mo_energy is enabled. Transforming the active space
# orbitals is a dangerous operation because it needs also to update the CI
# wavefunction. For DMRG solver (or other approximate FCI solver), the CI
# wavefunction may not be able to consistently converged and it leads to
# inconsistency between the orbital space and the CI wavefunction
# representations. Unless required by the following CAS calculation, setting
# mc.natorb=True should be avoided
# mc.natorb = True
mc.kernel(mo_guess, ci)
mc.analyze()
#---------------------
# CAS(12,42)
#
# Using the lowest CASSCF canonicalized orbitals in the CAS(12,42) DMRG-CASSCF
# calculation.
norb = 42
nelec = 12
mc1 = DMRGSCF(mf, norb, nelec)
mc1.fcisolver.maxM = 4000
# Enable internal rotation since the bond dimension of DMRG calculation is
# small, the active space energy can be optimized wrt to the orbital rotation
# within the active space.
mc1.internal_rotation = True
# Sorting the orbital energy is not a step of must here.
# mc1.sorting_mo_energy = True
# mc1.natorb = True
mc1.kernel()
# Passing the results as an initial guess to the next point.
return mf.make_rdm1(), mc.mo_coeff, mc.ci
def init(self,
molecule,
charge,
spin,
basis_set,
orb_basis='scf',
cas=False,
cas_nstart=None,
cas_nstop=None,
cas_nel=None,
loc_nstart=None,
loc_nstop=None,
scf_conv_tol=1e-14):
# {{{
import pyscf
from pyscf import gto, scf, ao2mo, molden, lo
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
#PYSCF inputs
print(" ---------------------------------------------------------")
print(" Using Pyscf:")
print(" ---------------------------------------------------------")
print(" ")
mol = gto.Mole()
mol.atom = molecule
mol.max_memory = 1000 # MB
mol.symmetry = True
mol.charge = charge
mol.spin = spin
mol.basis = basis_set
mol.build()
print("symmertry")
print(mol.topgroup)
#SCF
#mf = scf.RHF(mol).run(init_guess='atom')
mf = scf.RHF(mol).run(conv_tol=scf_conv_tol)
#C = mf.mo_coeff #MO coeffs
enu = mf.energy_nuc()
print(" SCF Total energy: %12.8f" % mf.e_tot)
print(" SCF Elec energy: %12.8f" % (mf.e_tot - enu))
print(mf.get_fock())
print(np.linalg.eig(mf.get_fock())[0])
if mol.symmetry == True:
from pyscf import symm
mo = symm.symmetrize_orb(mol, mf.mo_coeff)
osym = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mo)
#symm.addons.symmetrize_space(mol, mo, s=None, check=True, tol=1e-07)
for i in range(len(osym)):
print("%4d %8s %16.8f" % (i + 1, osym[i], mf.mo_energy[i]))
#orbitals and lectrons
n_orb = mol.nao_nr()
n_b, n_a = mol.nelec
nel = n_a + n_b
self.n_orb = mol.nao_nr()
if cas == True:
cas_norb = cas_nstop - cas_nstart
from pyscf import mcscf
assert (cas_nstart != None)
assert (cas_nstop != None)
assert (cas_nel != None)
else:
cas_nstart = 0
cas_nstop = n_orb
cas_nel = nel
##AO 2 MO Transformation: orb_basis or scf
if orb_basis == 'scf':
print("\nUsing Canonical Hartree Fock orbitals...\n")
C = cp.deepcopy(mf.mo_coeff)
print("C shape")
print(C.shape)
elif orb_basis == 'lowdin':
assert (cas == False)
S = mol.intor('int1e_ovlp_sph')
print("Using lowdin orthogonalized orbitals")
C = lowdin(S)
#end
elif orb_basis == 'boys':
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
cl_c = mf.mo_coeff[:, :cas_nstart]
cl_a = lo.Boys(mol,
mf.mo_coeff[:,
cas_nstart:cas_nstop]).kernel(verbose=4)
cl_v = mf.mo_coeff[:, cas_nstop:]
C = np.column_stack((cl_c, cl_a, cl_v))
elif orb_basis == 'boys2':
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
cl_c = mf.mo_coeff[:, :loc_nstart]
cl_a = lo.Boys(mol,
mf.mo_coeff[:,
loc_nstart:loc_nstop]).kernel(verbose=4)
cl_v = mf.mo_coeff[:, loc_nstop:]
C = np.column_stack((cl_c, cl_a, cl_v))
elif orb_basis == 'PM':
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
cl_c = mf.mo_coeff[:, :cas_nstart]
cl_a = lo.PM(mol,
mf.mo_coeff[:,
cas_nstart:cas_nstop]).kernel(verbose=4)
cl_v = mf.mo_coeff[:, cas_nstop:]
C = np.column_stack((cl_c, cl_a, cl_v))
elif orb_basis == 'PM2':
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
cl_c = mf.mo_coeff[:, :loc_nstart]
cl_a = lo.PM(mol,
mf.mo_coeff[:,
loc_nstart:loc_nstop]).kernel(verbose=4)
cl_v = mf.mo_coeff[:, loc_nstop:]
C = np.column_stack((cl_c, cl_a, cl_v))
elif orb_basis == 'ER':
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
cl_c = mf.mo_coeff[:, :cas_nstart]
cl_a = lo.PM(mol,
mf.mo_coeff[:,
cas_nstart:cas_nstop]).kernel(verbose=4)
cl_v = mf.mo_coeff[:, cas_nstop:]
C = np.column_stack((cl_c, cl_a, cl_v))
elif orb_basis == 'ER2':
pyscf.lib.num_threads(
1
) #with degenerate states and multiple processors there can be issues
cl_c = mf.mo_coeff[:, :loc_nstart]
cl_a = lo.ER(mol,
mf.mo_coeff[:,
loc_nstart:loc_nstop]).kernel(verbose=4)
cl_v = mf.mo_coeff[:, loc_nstop:]
C = np.column_stack((cl_c, cl_a, cl_v))
elif orb_basis == 'ibmo':
loc_vstop = loc_nstop - n_a
print(loc_vstop)
mo_occ = mf.mo_coeff[:, mf.mo_occ > 0]
mo_vir = mf.mo_coeff[:, mf.mo_occ == 0]
c_core = mo_occ[:, :loc_nstart]
iao_occ = lo.iao.iao(mol, mo_occ[:, loc_nstart:])
iao_vir = lo.iao.iao(mol, mo_vir[:, :loc_vstop])
c_out = mo_vir[:, loc_vstop:]
# Orthogonalize IAO
iao_occ = lo.vec_lowdin(iao_occ, mf.get_ovlp())
iao_vir = lo.vec_lowdin(iao_vir, mf.get_ovlp())
#
# Method 1, using Knizia's alogrithm to localize IAO orbitals
#
'''
Generate IBOS from orthogonal IAOs
'''
ibo_occ = lo.ibo.ibo(mol, mo_occ[:, loc_nstart:], iaos=iao_occ)
ibo_vir = lo.ibo.ibo(mol, mo_vir[:, :loc_vstop], iaos=iao_vir)
C = np.column_stack((c_core, ibo_occ, ibo_vir, c_out))
else:
print("Error:NO orbital basis defined")
molden.from_mo(mol, 'orbitals.molden', C)
if cas == True:
print(C.shape)
print(cas_norb)
print(cas_nel)
mycas = mcscf.CASSCF(mf, cas_norb, cas_nel)
h1e_cas, ecore = mycas.get_h1eff(
mo_coeff=C) #core core orbs to form ecore and eff
h2e_cas = ao2mo.kernel(mol,
C[:, cas_nstart:cas_nstop],
aosym='s4',
compact=False).reshape(4 * ((cas_norb), ))
print(h1e_cas)
print(h1e_cas.shape)
#return h1e_cas,h2e_cas,ecore,C,mol,mf
self.h = h1e_cas
self.g = h2e_cas
self.ecore = ecore
self.mf = mf
self.mol = mol
self.C = cp.deepcopy(C[:, cas_nstart:cas_nstop])
J, K = mf.get_jk()
self.J = self.C.T @ J @ self.C
self.K = self.C.T @ J @ self.C
#HF density
if orb_basis == 'scf':
#C = C[:,cas_nstart:cas_nstop]
D = mf.make_rdm1(mo_coeff=C)
S = mf.get_ovlp()
sal, svec = np.linalg.eigh(S)
idx = sal.argsort()[::-1]
sal = sal[idx]
svec = svec[:, idx]
sal = sal**-0.5
sal = np.diagflat(sal)
X = svec @ sal @ svec.T
C_ao2mo = np.linalg.inv(X) @ C
Cocc = C_ao2mo[:, :n_a]
D = Cocc @ Cocc.T
DMO = C_ao2mo.T @ D @ C_ao2mo
#only for cas space
DMO = DMO[cas_nstart:cas_nstop, cas_nstart:cas_nstop]
self.dm_aa = DMO
self.dm_bb = DMO
print("DENSITY")
print(self.dm_aa.shape)
if 0:
h = C.T.dot(mf.get_hcore()).dot(C)
g = ao2mo.kernel(mol, C, aosym='s4',
compact=False).reshape(4 * ((n_orb), ))
const, heff = get_eff_for_casci(cas_nstart, cas_nstop, h, g)
print(heff)
print("const", const)
print("ecore", ecore)
idx = range(cas_nstart, cas_nstop)
h = h[:, idx]
h = h[idx, :]
g = g[:, :, :, idx]
g = g[:, :, idx, :]
g = g[:, idx, :, :]
g = g[idx, :, :, :]
self.ecore = const
self.h = h + heff
self.g = g
elif cas == False:
h = C.T.dot(mf.get_hcore()).dot(C)
g = ao2mo.kernel(mol, C, aosym='s4',
compact=False).reshape(4 * ((n_orb), ))
print(h)
#return h, g, enu, C,mol,mf
self.h = h
self.g = g
self.ecore = enu
self.mf = mf
self.mol = mol
self.C = C
J, K = mf.get_jk()
self.J = self.C.T @ J @ self.C
self.K = self.C.T @ J @ self.C
#HF density
if orb_basis == 'scf':
D = mf.make_rdm1(mo_coeff=None)
S = mf.get_ovlp()
sal, svec = np.linalg.eigh(S)
idx = sal.argsort()[::-1]
sal = sal[idx]
svec = svec[:, idx]
sal = sal**-0.5
sal = np.diagflat(sal)
X = svec @ sal @ svec.T
C_ao2mo = np.linalg.inv(X) @ C
Cocc = C_ao2mo[:, :n_a]
D = Cocc @ Cocc.T
DMO = C_ao2mo.T @ D @ C_ao2mo
self.dm_aa = DMO
self.dm_bb = DMO
print("DENSITY")
print(self.dm_aa)
def caslst_by_irrep(casscf, mo_coeff, cas_irrep_nocc,
cas_irrep_ncore=None, s=None, base=1):
'''Given number of active orbitals for each irrep, return the orbital
indices of active space
Args:
casscf : an :class:`CASSCF` or :class:`CASCI` object
cas_irrep_nocc : list or dict
Number of active orbitals for each irrep. It can be a dict, eg
{'A1': 2, 'B2': 4} to indicate the active space size based on
irrep names, or {0: 2, 3: 4} for irrep Id, or a list [2, 0, 0, 4]
(identical to {0: 2, 3: 4}) in which the list index is served as
the irrep Id.
Kwargs:
cas_irrep_ncore : list or dict
Number of closed shells for each irrep. It can be a dict, eg
{'A1': 6, 'B2': 4} to indicate the closed shells based on
irrep names, or {0: 6, 3: 4} for irrep Id, or a list [6, 0, 0, 4]
(identical to {0: 6, 3: 4}) in which the list index is served as
the irrep Id. If cas_irrep_ncore is not given, the program
will generate a guess based on the lowest :attr:`CASCI.ncore`
orbitals.
s : ndarray
overlap matrix
base : int
0-based (C-like) or 1-based (Fortran-like) caslst
Returns:
A list of orbital indices
Examples:
>>> from pyscf import gto, scf, mcscf
>>> mol = gto.M(atom='N 0 0 0; N 0 0 1', basis='ccpvtz', symmetry=True, verbose=0)
>>> mf = scf.RHF(mol)
>>> mf.kernel()
>>> mc = mcscf.CASSCF(mf, 12, 4)
>>> mcscf.caslst_by_irrep(mc, mf.mo_coeff, {'E1gx':4, 'E1gy':4, 'E1ux':2, 'E1uy':2})
[5, 7, 8, 10, 11, 14, 15, 20, 25, 26, 31, 32]
'''
mol = casscf.mol
log = logger.Logger(casscf.stdout, casscf.verbose)
if s is None:
s = casscf._scf.get_ovlp()
orbsym = symm.label_orb_symm(mol, mol.irrep_id,
mol.symm_orb, mo_coeff, s)
orbsym = numpy.asarray(orbsym)
ncore = casscf.ncore
irreps = set(orbsym)
if cas_irrep_ncore is not None:
irrep_ncore = {}
for k, v in cas_irrep_ncore.items():
if isinstance(k, str):
irrep_ncore[symm.irrep_name2id(mol.groupname, k)] = v
else:
irrep_ncore[k] = v
ncore_rest = casscf.ncore - sum(irrep_ncore.values())
if ncore_rest > 0: # guess core configuration
mask = numpy.ones(len(orbsym), dtype=bool)
for ir in irrep_ncore:
mask[orbsym == ir] = False
core_rest = orbsym[mask][:ncore_rest]
core_rest = dict([(ir, numpy.count_nonzero(core_rest==ir))
for ir in set(core_rest)])
log.info('Given core space %s < casscf core size %d',
cas_irrep_ncore, casscf.ncore)
log.info('Add %s to core configuration', core_rest)
irrep_ncore.update(core_rest)
elif ncore_rest < 0:
raise ValueError('Given core space %s > casscf core size %d'
% (cas_irrep_ncore, casscf.ncore))
else:
irrep_ncore = dict([(ir, sum(orbsym[:ncore]==ir)) for ir in irreps])
if not isinstance(cas_irrep_nocc, dict):
# list => dict
cas_irrep_nocc = dict([(ir, n) for ir,n in enumerate(cas_irrep_nocc)
if n > 0])
irrep_ncas = {}
for k, v in cas_irrep_nocc.items():
if isinstance(k, str):
irrep_ncas[symm.irrep_name2id(mol.groupname, k)] = v
else:
irrep_ncas[k] = v
ncas_rest = casscf.ncas - sum(irrep_ncas.values())
if ncas_rest > 0:
mask = numpy.ones(len(orbsym), dtype=bool)
# remove core and specified active space
for ir in irrep_ncas:
mask[orbsym == ir] = False
for ir, ncore in irrep_ncore.items():
idx = numpy.where(orbsym == ir)[0]
mask[idx[:ncore]] = False
cas_rest = orbsym[mask][:ncas_rest]
cas_rest = dict([(ir, numpy.count_nonzero(cas_rest==ir))
for ir in set(cas_rest)])
log.info('Given active space %s < casscf active space size %d',
cas_irrep_nocc, casscf.ncas)
log.info('Add %s to active space', cas_rest)
irrep_ncas.update(cas_rest)
elif ncas_rest < 0:
raise ValueError('Given active space %s > casscf active space size %d'
% (cas_irrep_nocc, casscf.ncas))
caslst = []
for ir, ncas in irrep_ncas.items():
if ncas > 0:
if ir in irrep_ncore:
nc = irrep_ncore[ir]
else:
nc = 0
no = nc + ncas
idx = numpy.where(orbsym == ir)[0]
caslst.extend(idx[nc:no])
caslst = numpy.sort(numpy.asarray(caslst)) + base
if len(caslst) < casscf.ncas:
raise ValueError('Not enough orbitals found for core %s, cas %s' %
(cas_irrep_ncore, cas_irrep_nocc))
if log.verbose >= logger.INFO:
log.info('ncore for each irreps %s',
dict([(symm.irrep_id2name(mol.groupname, k), v)
for k,v in irrep_ncore.items()]))
log.info('ncas for each irreps %s',
dict([(symm.irrep_id2name(mol.groupname, k), v)
for k,v in irrep_ncas.items()]))
log.info('(%d-based) caslst = %s', base, caslst)
return caslst
H 2.49475714 0. -0.00736748
H 1.24762314 2.16037824 -0.00925948
H -1.24752386 2.16043824 -0.01063248
H -2.49460686 0. -0.00886348
''',
basis = 'ccpvdz')
mf = scf.RHF(mol)
mf.kernel()
# Change error tolerence (to 0.1 Bohr, default is 1e-5 Bohr) for symmetry
# detection, so that the program can find the raw symmetry.
symm.geom.GEOM_THRESHOLD = .1
symm.geom.PLACE = 1
mol.symmetry = True
mol.build(False, False)
print('Pseudo symmetry %s' % mol.groupname)
# Call mol.build again to avoid the atom coordinates changed
mol.symmetry = mol.groupname
mol.build(False, False)
irname = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mf.mo_coeff, check=False)
s = mol.intor('cint1e_ovlp_sph')
print('MO id irreps likely')
for i, ir in enumerate(irname):
k = mol.irrep_name.index(ir)
s1 = reduce(numpy.dot, (mol.symm_orb[k].T, s, mf.mo_coeff[:,i]))
s0 = reduce(numpy.dot, (mol.symm_orb[k].T, s, mol.symm_orb[k]))
print('MO %3d %-3s %8.5f' % (i, ir, numpy.dot(s1, numpy.linalg.solve(s0, s1))))
def writeNevpt2Integrals(mc, dm1, dm2, dm1eff, aaavsplit, frozen):
eris = _ERIS(mc, mc.mo_coeff)
nocc = mc.ncore + mc.ncas
ncore = mc.ncore
nact = mc.ncas
norbs = eris['ppaa'].shape[0]
nvirt = norbs-ncore-nact
eris_sp={}
#eris_sp['cvcv']= numpy.zeros(shape=(1,1)) #numpy.zeros(shape=(mc.ncore, norbs-mc.ncore-mc.ncas, mc.ncore, norbs-mc.ncas-mc.ncore))
eris_sp['h1eff']= 1.*eris['h1eff'] #numpy.zeros(shape=(norbs, norbs))
int1 = reduce(numpy.dot, (mc.mo_coeff.T, mc.get_hcore(), mc.mo_coeff))
#eris_sp['h1eff'] = makeheff(int1, eris['papa'], eris['ppaa'], dm1, ncore, nvirt)
eris_sp['h1eff'][:mc.ncore,:mc.ncore] += numpy.einsum('abcd,cd', eris['ppaa'][:mc.ncore, :mc.ncore,:,:], dm1eff)
eris_sp['h1eff'][:mc.ncore,:mc.ncore] -= numpy.einsum('abcd,bd', eris['papa'][:mc.ncore, :, :mc.ncore,:], dm1eff)*0.5
eris_sp['h1eff'][mc.ncas+mc.ncore:,mc.ncas+mc.ncore:] += numpy.einsum('abcd,cd', eris['ppaa'][mc.ncas+mc.ncore:,mc.ncas+mc.ncore:,:,:], dm1eff)
eris_sp['h1eff'][mc.ncas+mc.ncore:,mc.ncas+mc.ncore:] -= numpy.einsum('abcd,bd', eris['papa'][mc.ncas+mc.ncore:,:,mc.ncas+mc.ncore:,:], dm1eff)*0.5
offdiagonal = 0.0
#zero out off diagonal core
for k in range(mc.ncore):
for l in range(mc.ncore):
if(k != l):
offdiagonal = max(abs(offdiagonal), abs(eris_sp['h1eff'][k,l] ))
#zero out off diagonal virtuals
for k in range(mc.ncore+mc.ncas, norbs):
for l in range(mc.ncore+mc.ncas,norbs):
if(k != l):
offdiagonal = max(abs(offdiagonal), abs(eris_sp['h1eff'][k,l] ))
if (abs(offdiagonal) > 1e-6):
print "WARNING ***** Have to use natorual orbitals from casscf ****"
print "offdiagonal elements ", offdiagonal
eriscvcv = eris['cvcv']
if (not isinstance(eris['cvcv'], type(eris_sp['h1eff']))):
#eriscvcv = h5py.File(eris['cvcv'].name,'r')["eri_mo"]
eriscvcv = lib.chkfile.load(eris['cvcv'].name, "eri_mo")#h5py.File(eris['cvcv'].name,'r')["eri_mo"]
eris_sp['cvcv'] = eriscvcv.reshape(mc.ncore, norbs-mc.ncore-mc.ncas, mc.ncore, norbs-mc.ncore-mc.ncas)
import os
os.system("mkdir int")
numpy.save("int/W:caac", numpy.asfortranarray(eris['papa'][frozen:mc.ncore, :, frozen:mc.ncore, :].transpose(0,3,1,2)))
numpy.save("int/W:aeca", numpy.asfortranarray(eris['papa'][frozen:mc.ncore, :, mc.ncore+mc.ncas:, :].transpose(1,2,0,3)))
numpy.save("int/W:ccaa", numpy.asfortranarray(eris['papa'][frozen:mc.ncore, :, frozen:mc.ncore, :].transpose(0,2,1,3)))
numpy.save("int/W:eeaa", numpy.asfortranarray(eris['papa'][mc.ncore+mc.ncas:, :, mc.ncore+mc.ncas:, :].transpose(0,2,1,3)))
numpy.save("int/W:caca", numpy.asfortranarray(eris['ppaa'][frozen:mc.ncore, frozen:mc.ncore, :, :].transpose(0,2,1,3)))
numpy.save("int/W:eaca", numpy.asfortranarray(eris['ppaa'][mc.ncore+mc.ncas:, frozen:mc.ncore, :, :].transpose(0,2,1,3)))
numpy.save("int/W:eecc", numpy.asfortranarray(eris_sp['cvcv'][frozen:,:,frozen:,:].transpose(1,3,0,2)))
numpy.save("int/W:ccae", numpy.asfortranarray(eris['pacv'][frozen:mc.ncore,:,frozen:,:].transpose(0,2,1,3)))
numpy.save("int/W:aaaa", numpy.asfortranarray(eris['ppaa'][mc.ncore:mc.ncore+mc.ncas, mc.ncore:mc.ncore+mc.ncas, :, :].transpose(0,2,1,3)))
numpy.save("int/W:eeca", numpy.asfortranarray(eris['pacv'][mc.ncore+mc.ncas:, :, frozen:, :].transpose(3,0,2,1)))
numpy.save("int/int1eff", numpy.asfortranarray(eris_sp['h1eff'][frozen:,frozen:]))
numpy.save("int/E1.npy", numpy.asfortranarray(dm1))
numpy.save("int/E2.npy", numpy.asfortranarray(dm2))
#numpy.save("int/E3",dm3)
#numpy.save("int/E3B.npy", dm3.transpose(0,3,1,4,2,5))
#numpy.save("int/E3C.npy", dm3.transpose(5,0,2,4,1,3))
nc = mc.ncore+mc.ncas
energyE0 = 1.0*numpy.einsum('ij,ij', eris_sp['h1eff'][ncore:nc, ncore:nc], dm1)
energyE0 += 0.5*numpy.einsum('ijkl,ijkl', eris['ppaa'][mc.ncore:mc.ncore+mc.ncas, mc.ncore:mc.ncore+mc.ncas, :, :].transpose(0,2,1,3), dm2)
mo = mc.mo_coeff
dmcore = numpy.dot(mo[:,:ncore], mo[:,:ncore].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
energyE0 += numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
energyE0 += mc.mol.energy_nuc()
print "Energy = ", energyE0
from pyscf import symm
mol = mc.mol
orbsymout=[]
orbsym = []
if (mol.symmetry):
orbsym = symm.label_orb_symm(mc.mol, mc.mol.irrep_id,
mc.mol.symm_orb, mc.mo_coeff, s=mc._scf.get_ovlp())
if mol.symmetry and orbsym:
if mol.groupname.lower() == 'dooh':
orbsymout = [dmrg_sym.IRREP_MAP['D2h'][i % 10] for i in orbsym]
elif mol.groupname.lower() == 'coov':
orbsymout = [dmrg_sym.IRREP_MAP['C2v'][i % 10] for i in orbsym]
else:
orbsymout = [dmrg_sym.IRREP_MAP[mol.groupname][i] for i in orbsym]
else:
orbsymout = []
ncore = mc.ncore
mo = mc.mo_coeff
dmcore = numpy.dot(mo[:,:ncore], mo[:,:ncore].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
energy_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
print energy_core
virtOrbs = range(ncore+mc.ncas, eris_sp['h1eff'].shape[0])
chunks = len(virtOrbs)/aaavsplit
virtRange = [virtOrbs[i:i+chunks] for i in xrange(0, len(virtOrbs), chunks)]
for K in range(aaavsplit):
currentOrbs = range(ncore, mc.ncas+ncore)+virtRange[K]
fout = open('FCIDUMP_aaav%d'%(K),'w')
#tools.fcidump.write_head(fout, eris_sp['h1eff'].shape[0]-ncore, mol.nelectron-2*ncore, orbsym= orbsymout[ncore:])
tools.fcidump.write_head(fout, mc.ncas+len(virtRange[K]), mol.nelectron-2*ncore, orbsym= (orbsymout[ncore:ncore+mc.ncas]+orbsymout[virtRange[K][0]:virtRange[K][-1]+1]) )
ij = ncore*(ncore+1)/2
for i in range(len(currentOrbs)):
for j in range(ncore, mc.ncas+ncore):
for k in range(mc.ncas):
for l in range(k+1):
I = currentOrbs[i]
if abs(eris['ppaa'][I,j,k,l]) > 1.e-8 :
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (eris['ppaa'][I,j,k,l], i+1, j+1-ncore, k+1, l+1))
h1eff = numpy.zeros(shape=(mc.ncas+len(virtRange[K]), mc.ncas+len(virtRange[K])))
h1eff[:mc.ncas, :mc.ncas] = eris_sp['h1eff'][ncore:ncore+mc.ncas,ncore:ncore+mc.ncas]
h1eff[mc.ncas:, mc.ncas:] = eris_sp['h1eff'][virtRange[K][0]:virtRange[K][-1]+1, virtRange[K][0]:virtRange[K][-1]+1]
h1eff[:mc.ncas, mc.ncas:] = eris_sp['h1eff'][ncore:ncore+mc.ncas, virtRange[K][0]:virtRange[K][-1]+1]
h1eff[mc.ncas:, :mc.ncas] = eris_sp['h1eff'][virtRange[K][0]:virtRange[K][-1]+1, ncore:ncore+mc.ncas]
tools.fcidump.write_hcore(fout, h1eff, mc.ncas+len(virtRange[K]), tol=1e-8)
#tools.fcidump.write_hcore(fout, eris_sp['h1eff'][virtRange[K][0]:virtRange[K][-1]+1, virtRange[K][0]:virtRange[K][-1]+1], len(virtRange[K]), tol=1e-8)
fout.write(' %17.9e 0 0 0 0\n' %( mol.energy_nuc()+energy_core-energyE0))
fout.close()
nc = ncore+mc.ncas
fout = open('FCIDUMP_aaac','w')
tools.fcidump.write_head(fout, nc-frozen, mol.nelectron-2*frozen, orbsym= orbsymout[frozen:nc])
for i in range(frozen,nc):
for j in range(ncore, nc):
for k in range(ncore, nc):
for l in range(ncore,k+1):
if abs(eris['ppaa'][i,j,k-ncore,l-ncore]) > 1.e-8 :
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (eris['ppaa'][i,j,k-ncore,l-ncore], i+1-frozen, j+1-frozen, k+1-frozen, l+1-frozen))
dmrge = energyE0-mol.energy_nuc()-energy_core
ecore_aaac = 0.0;
for i in range(frozen,ncore):
ecore_aaac += 2.0*eris_sp['h1eff'][i,i]
tools.fcidump.write_hcore(fout, eris_sp['h1eff'][frozen:nc,frozen:nc], nc-frozen, tol=1e-8)
fout.write(' %17.9e 0 0 0 0\n' %( -dmrge-ecore_aaac))
fout.close()
return norbs, energyE0
mol.verbose = 0
mol.atom = [
['O', (0.000000, 0.000000, 1.210000)],
['C', (0.000000, 0.000000, 0.000000)],
['H', (0.000000, 0.943435, -0.599878)],
['H', (0.000000, -0.943435, -0.599878)],
]
mol.basis = {'H': 'cc-pVTZ', 'C': 'cc-pVTZ', 'O': 'cc-pVTZ'}
mol.symmetry = 'c1'
mol.build()
m = scf.RHF(mol)
m.kernel()
irrep_name = m.mol.irrep_id
sym = symm.label_orb_symm(m.mol, irrep_name,m.mol.symm_orb,m.mo_coeff)
orbsym = [IRREP_MAP['C1'][i % 10] for i in sym]
m.verbose = 4
ehf = m.scf()
mc=mcscf.CASCI(m,16,16)
mc.verbose = 4
# ci_e = mc.kernel()[0]
# print 'CI energy', ci_e
# mc.casci()
mo_cas_coeff = mc.mo_coeff[:,mc.ncore:mc.ncore+mc.ncas]
AOdipInt = mol.intor('cint1e_r_sph', comp=3)
MOdipInt = numpy.zeros([3,mo_cas_coeff.shape[1],mo_cas_coeff.shape[1]])
def get_occ(self, mo_energy=None, mo_coeff=None, orbsym=None):
''' We assumed mo_energy are grouped by symmetry irreps, (see function
self.eig). The orbitals are sorted after SCF.
'''
if mo_energy is None: mo_energy = self.mo_energy
mol = self.mol
if orbsym is None:
if mo_coeff is not None:
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
else:
orbsym = [numpy.repeat(ir, mol.symm_orb[i].shape[1])
for i, ir in enumerate(mol.irrep_id)]
orbsym = numpy.hstack(orbsym)
else:
orbsym = numpy.asarray(orbsym)
assert(mo_energy.size == orbsym.size)
mo_occ = numpy.zeros_like(mo_energy)
rest_idx = []
nelec_fix = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = numpy.where(orbsym == ir)[0]
if irname in self.irrep_nelec:
n = self.irrep_nelec[irname]
occ_sort = numpy.argsort(mo_energy[ir_idx].round(9))
occ_idx = ir_idx[occ_sort[:n//2]]
mo_occ[occ_idx] = 2
nelec_fix += n
else:
rest_idx.append(ir_idx)
nelec_float = mol.nelectron - nelec_fix
assert(nelec_float >= 0)
if nelec_float > 0:
rest_idx = numpy.hstack(rest_idx)
occ_sort = numpy.argsort(mo_energy[rest_idx].round(9))
occ_idx = rest_idx[occ_sort[:nelec_float//2]]
mo_occ[occ_idx] = 2
vir_idx = (mo_occ==0)
if self.verbose >= logger.INFO and numpy.count_nonzero(vir_idx) > 0:
ehomo = max(mo_energy[mo_occ>0 ])
elumo = min(mo_energy[mo_occ==0])
noccs = []
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = (orbsym == ir)
noccs.append(int(mo_occ[ir_idx].sum()))
if ehomo in mo_energy[ir_idx]:
irhomo = irname
if elumo in mo_energy[ir_idx]:
irlumo = irname
logger.info(self, 'H**O (%s) = %.15g LUMO (%s) = %.15g',
irhomo, ehomo, irlumo, elumo)
logger.debug(self, 'irrep_nelec = %s', noccs)
_dump_mo_energy(mol, mo_energy, mo_occ, ehomo, elumo, orbsym,
verbose=self.verbose)
return mo_occ
def label_symmetry_(mc, mo_coeff, ci0=None):
log = logger.Logger(mc.stdout, mc.verbose)
#irrep_name = mc.mol.irrep_name
irrep_name = mc.mol.irrep_id
s = mc._scf.get_ovlp()
ncore = mc.ncore
nocc = ncore + mc.ncas
try:
orbsym = scf.hf_symm.get_orbsym(mc._scf.mol, mo_coeff, s, True)
except ValueError:
log.warn('mc1step_symm symmetrizes input orbitals')
mo_cor = symm.symmetrize_space(mc.mol, mo_coeff[:, :ncore], s=s, check=False)
mo_act = symm.symmetrize_space(mc.mol, mo_coeff[:,ncore:nocc], s=s, check=False)
mo_vir = symm.symmetrize_space(mc.mol, mo_coeff[:,nocc: ], s=s, check=False)
mo_coeff = numpy.hstack((mo_cor,mo_act,mo_vir))
orbsym = symm.label_orb_symm(mc.mol, irrep_name,
mc.mol.symm_orb, mo_coeff, s=s)
mo_coeff_with_orbsym = lib.tag_array(mo_coeff, orbsym=orbsym)
active_orbsym = getattr(mc.fcisolver, 'orbsym', [])
if (not getattr(active_orbsym, '__len__', None)) or len(active_orbsym) == 0:
mc.fcisolver.orbsym = orbsym[ncore:nocc]
log.debug('Active space irreps %s', str(mc.fcisolver.orbsym))
wfnsym = 0
if getattr(mc.fcisolver, 'wfnsym', None) is not None:
wfnsym = mc.fcisolver.wfnsym
elif ci0 is None:
# Guess wfnsym based on HF determinant. mo_coeff may not be HF
# canonical orbitals. Some checks are needed to ensure that mo_coeff
# are derived from the symmetry adapted SCF calculations.
if mo_coeff is mc._scf.mo_coeff:
wfnsym = 0
for ir in orbsym[mc._scf.mo_occ == 1]:
wfnsym ^= ir
mc.fcisolver.wfnsym = wfnsym
log.debug('Set CASCI wfnsym %s based on HF determinant', wfnsym)
elif getattr(mo_coeff, 'orbsym', None) is not None: # It may be reordered SCF orbitals
cas_orb = mo_coeff[:,ncore:nocc]
s = reduce(numpy.dot, (cas_orb.T, mc._scf.get_ovlp(), mc._scf.mo_coeff))
if numpy.all(numpy.max(s, axis=1) > 1-1e-9):
idx = numpy.argmax(s, axis=1)
cas_orbsym = orbsym[ncore:nocc]
cas_occ = mc._scf.mo_occ[idx]
wfnsym = 0
for ir in cas_orbsym[cas_occ == 1]:
wfnsym ^= ir
mc.fcisolver.wfnsym = wfnsym
log.debug('Active space are constructed from canonical SCF '
'orbitals %s', idx)
log.debug('Set CASCI wfnsym %s based on HF determinant', wfnsym)
elif getattr(mc.fcisolver, 'guess_wfnsym', None):
wfnsym = mc.fcisolver.guess_wfnsym(mc.ncas, mc.nelecas, ci0, verbose=log)
log.debug('CASCI wfnsym %s (based on CI initial guess)', wfnsym)
if isinstance(wfnsym, (int, numpy.integer)):
wfnsym = symm.irrep_id2name(mc.mol.groupname, wfnsym)
log.info('Active space CI wfn symmetry = %s', wfnsym)
return mo_coeff_with_orbsym
def writeNumpyforMRLCC(mc, E1, E2, frozen):
ncore = mc.ncore
nact = mc.ncas
norbs = mc.mo_coeff.shape[1]
nelec = mc.nelecas[0] + mc.nelecas[1]
nvirt = norbs - ncore - nact
nc = ncore + nact
nactElec = nelec - 2 * ncore
#this is chemistry notation
int2popo = ao2mo.outcore.general_iofree(
mc.mol,
(mc.mo_coeff, mc.mo_coeff[:, :nc], mc.mo_coeff, mc.mo_coeff[:, :nc]),
compact=False)
int2ppoo = ao2mo.outcore.general_iofree(
mc.mol,
(mc.mo_coeff, mc.mo_coeff, mc.mo_coeff[:, :nc], mc.mo_coeff[:, :nc]),
compact=False)
int2popo.shape = (norbs, nc, norbs, nc)
int2ppoo.shape = (norbs, norbs, nc, nc)
mo = mc.mo_coeff
dmcore = numpy.dot(mo[:, :frozen], mo[:, :frozen].T) * 2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj - vk * 0.5, mo))
int1 = reduce(numpy.dot,
(mc.mo_coeff.T, mc.get_hcore(), mc.mo_coeff)) + vhfcore
dmcore = numpy.dot(mo[:, :ncore], mo[:, :ncore].T) * 2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj - vk * 0.5, mo))
int1_eff = reduce(numpy.dot,
(mc.mo_coeff.T, mc.get_hcore(), mc.mo_coeff)) + vhfcore
#int1_eff = makeheff(int1, int2popo, int2ppoo, E1, ncore, nvirt, frozen)
energy_frozen_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
#numpy.save("int/E3",E3)
#numpy.save("int/E3B.npy", E3.transpose(0,3,1,4,2,5))
#numpy.save("int/E3C.npy", E3.transpose(5,0,2,4,1,3))
numpy.save("int/E2", numpy.asfortranarray(E2))
numpy.save("int/E1", numpy.asfortranarray(E1))
#numpy.save("int/int2",int2)
numpy.save("int/int1", numpy.asfortranarray(int1[frozen:, frozen:]))
numpy.save("int/int1eff", numpy.asfortranarray(int1_eff[frozen:, frozen:]))
numpy.save(
"int/W:caca",
numpy.asfortranarray(int2ppoo[frozen:ncore, frozen:ncore, ncore:nc,
ncore:nc].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:caac",
numpy.asfortranarray(int2popo[frozen:ncore, ncore:nc, ncore:nc,
frozen:ncore].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:cece",
numpy.asfortranarray(int2ppoo[nc:, nc:, frozen:ncore,
frozen:ncore].transpose(2, 0, 3, 1)))
numpy.save(
"int/W:ceec",
numpy.asfortranarray(int2popo[nc:, frozen:ncore, nc:,
frozen:ncore].transpose(1, 2, 0, 3)))
numpy.save(
"int/W:aeae",
numpy.asfortranarray(int2ppoo[nc:, nc:, ncore:nc,
ncore:nc].transpose(2, 0, 3, 1)))
numpy.save(
"int/W:aeea",
numpy.asfortranarray(int2popo[nc:, ncore:nc, nc:,
ncore:nc].transpose(1, 2, 0, 3)))
numpy.save(
"int/W:cccc",
numpy.asfortranarray(int2ppoo[frozen:ncore, frozen:ncore, frozen:ncore,
frozen:ncore].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:aaaa",
numpy.asfortranarray(int2ppoo[ncore:nc, ncore:nc, ncore:nc,
ncore:nc].transpose(0, 2, 1, 3)))
feri = h5py.File("int/int2eeee.hdf5", 'w')
ao2mo.full(mc.mol, mc.mo_coeff[:, nc:], feri, compact=False)
for o in range(nvirt):
int2eee = feri['eri_mo'][o * (norbs - nc):(o + 1) * (norbs - nc), :]
numpy.asfortranarray(int2eee).tofile("int/W:eeee%04d" % (o))
#store perturbers
numpy.save(
"int/W:eecc",
numpy.asfortranarray(int2popo[nc:, frozen:ncore, nc:,
frozen:ncore].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:eeca",
numpy.asfortranarray(int2popo[nc:, frozen:ncore, nc:,
ncore:nc].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:ccaa",
numpy.asfortranarray(int2popo[frozen:ncore, ncore:nc, frozen:ncore,
ncore:nc].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:eeaa",
numpy.asfortranarray(int2popo[nc:, ncore:nc, nc:,
ncore:nc].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:eaca",
numpy.asfortranarray(int2popo[nc:, frozen:ncore, ncore:nc,
ncore:nc].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:aeca",
numpy.asfortranarray(int2popo[ncore:nc, frozen:ncore, nc:,
ncore:nc].transpose(0, 2, 1, 3)))
numpy.save(
"int/W:ccae",
numpy.asfortranarray(int2popo[frozen:ncore, ncore:nc, nc:,
frozen:ncore].transpose(0, 3, 1, 2)))
#write FCIDUMP_AAAV and FCIDUMP_AAAC
from pyscf import symm
mol = mc.mol
orbsymout = []
orbsym = []
if (mol.symmetry):
orbsym = symm.label_orb_symm(mc.mol,
mc.mol.irrep_id,
mc.mol.symm_orb,
mc.mo_coeff,
s=mc._scf.get_ovlp())
if mol.symmetry and orbsym:
if mol.groupname.lower() == 'dooh':
orbsymout = [dmrg_sym.IRREP_MAP['D2h'][i % 10] for i in orbsym]
elif mol.groupname.lower() == 'coov':
orbsymout = [dmrg_sym.IRREP_MAP['C2v'][i % 10] for i in orbsym]
else:
orbsymout = [dmrg_sym.IRREP_MAP[mol.groupname][i] for i in orbsym]
else:
orbsymout = []
'''
dmcore = numpy.dot(mo[:,frozen:ncore], mo[:,frozen:ncore].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
h1eff = int1+vhfcore
energy_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5\
+energy_frozen_core
'''
dmcore = numpy.dot(mo[:, :ncore], mo[:, :ncore].T) * 2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj - vk * 0.5, mo))
h1eff = int1_eff
energy_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
#print energy_core2+mc.mol.energy_nuc(), energy_core+mc.mol.energy_nuc(), energy_frozen_core+mc.mol.energy_nuc()
nc = mc.ncore + mc.ncas
energyE0 = 1.0 * numpy.einsum('ij,ij', h1eff[ncore:nc, ncore:nc], E1)
#+ 0.5*numpy.einsum('ikjl,ijkl', E2, int2ppoo[ncore:,ncore:,ncore:,ncore:])
for i in range(mc.ncas):
for j in range(mc.ncas):
for k in range(mc.ncas):
for l in range(mc.ncas):
I, J = max(i, j) + ncore, min(i, j) + ncore
K, L = max(k, l) + ncore, min(k, l) + ncore
energyE0 += 0.5 * E2[i, k, j,
l] * int2ppoo[i + ncore, j + ncore,
k + ncore, l + ncore]
energyE0 += energy_core
energyE0 += mc.mol.energy_nuc()
print "Energy = ", energyE0
fout = open('FCIDUMP_aaav0', 'w')
tools.fcidump.write_head(fout,
int1.shape[0] - ncore,
mc.mol.nelectron - 2 * ncore,
orbsym=orbsymout[ncore:])
for i in range(ncore, int1.shape[0]):
for j in range(ncore, i + 1):
for k in range(mc.ncas):
for l in range(k + 1):
if abs(int2ppoo[i, j, k + ncore, l + ncore]) > 1.e-8:
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (int2ppoo[i,j, k+ncore,l+ncore], i+1-ncore, j+1-ncore, k+1, l+1))
if (j >= nc and
abs(int2popo[i, k + ncore, j, l + ncore]) > 1.e-8):
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (int2popo[i,k+ncore,j, l+ncore], i+1-ncore, k+1, l+1, j+1-ncore))
if (j >= nc and
abs(int2popo[i, l + ncore, j, k + ncore]) > 1.e-8):
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (int2popo[i,l+ncore, j, k+ncore], i+1-ncore, l+1, k+1, j+1-ncore))
tools.fcidump.write_hcore(fout,
h1eff[ncore:, ncore:],
int1.shape[0] - ncore,
tol=1e-8)
fout.write(' %17.9e 0 0 0 0\n' %
(mc.mol.energy_nuc() + energy_core - energyE0))
fout.close()
nc = ncore + mc.ncas
eri1cas = ao2mo.outcore.general_iofree(
mc.mol, (mc.mo_coeff[:, frozen:nc], mc.mo_coeff[:, frozen:nc],
mc.mo_coeff[:, frozen:nc], mc.mo_coeff[:, frozen:nc]),
compact=True)
tools.fcidump.from_integrals("FCIDUMP_aaac",
int1[frozen:nc, frozen:nc],
eri1cas,
nc - frozen,
mc.mol.nelectron - 2 * frozen,
nuc=mc.mol.energy_nuc() - energyE0,
orbsym=orbsymout[frozen:nc],
tol=1e-8)
return energyE0, norbs
def analyze(mf, verbose=logger.DEBUG):
from pyscf.lo import orth
from pyscf.tools import dump_mat
mo_energy = mf.mo_energy
mo_occ = mf.mo_occ
mo_coeff = mf.mo_coeff
mol = mf.mol
log = pyscf.lib.logger.Logger(mf.stdout, verbose)
nirrep = len(mol.irrep_id)
ovlp_ao = mf.get_ovlp()
orbsyma = symm.label_orb_symm(mol,
mol.irrep_id,
mol.symm_orb,
mo_coeff[0],
s=ovlp_ao)
orbsymb = symm.label_orb_symm(mol,
mol.irrep_id,
mol.symm_orb,
mo_coeff[1],
s=ovlp_ao)
orbsyma = numpy.array(orbsyma)
orbsymb = numpy.array(orbsymb)
tot_sym = 0
noccsa = [sum(orbsyma[mo_occ[0] > 0] == ir) for ir in mol.irrep_id]
noccsb = [sum(orbsymb[mo_occ[1] > 0] == ir) for ir in mol.irrep_id]
for i, ir in enumerate(mol.irrep_id):
if (noccsa[i] + noccsb[i]) % 2:
tot_sym ^= ir
if mol.groupname in ('Dooh', 'Coov', 'SO3'):
log.note('TODO: total symmetry for %s', mol.groupname)
else:
log.note('total symmetry = %s',
symm.irrep_id2name(mol.groupname, tot_sym))
log.note('alpha occupancy for each irrep: ' + (' %4s' * nirrep),
*mol.irrep_name)
log.note(' ' + (' %4d' * nirrep), *noccsa)
log.note('beta occupancy for each irrep: ' + (' %4s' * nirrep),
*mol.irrep_name)
log.note(' ' + (' %4d' * nirrep), *noccsb)
ss, s = mf.spin_square(
(mo_coeff[0][:, mo_occ[0] > 0], mo_coeff[1][:, mo_occ[1] > 0]),
ovlp_ao)
log.note('multiplicity <S^2> = %.8g 2S+1 = %.8g', ss, s)
if verbose >= logger.NOTE:
log.note('**** MO energy ****')
irname_full = {}
for k, ir in enumerate(mol.irrep_id):
irname_full[ir] = mol.irrep_name[k]
irorbcnt = {}
for k, j in enumerate(orbsyma):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note('alpha MO #%d (%s #%d), energy= %.15g occ= %g', k + 1,
irname_full[j], irorbcnt[j], mo_energy[0][k],
mo_occ[0][k])
irorbcnt = {}
for k, j in enumerate(orbsymb):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note('beta MO #%d (%s #%d), energy= %.15g occ= %g', k + 1,
irname_full[j], irorbcnt[j], mo_energy[1][k],
mo_occ[1][k])
ovlp_ao = mf.get_ovlp()
if mf.verbose >= logger.DEBUG:
label = mol.spheric_labels(True)
molabel = []
irorbcnt = {}
for k, j in enumerate(orbsyma):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
molabel.append('#%-d(%s #%d)' %
(k + 1, irname_full[j], irorbcnt[j]))
log.debug(
' ** alpha MO coefficients (expansion on meta-Lowdin AOs) **')
orth_coeff = orth.orth_ao(mol, 'meta_lowdin', s=ovlp_ao)
c_inv = numpy.dot(orth_coeff.T, ovlp_ao)
dump_mat.dump_rec(mol.stdout,
c_inv.dot(mo_coeff[0]),
label,
molabel,
start=1)
molabel = []
irorbcnt = {}
for k, j in enumerate(orbsymb):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
molabel.append('#%-d(%s #%d)' %
(k + 1, irname_full[j], irorbcnt[j]))
log.debug(' ** beta MO coefficients (expansion on meta-Lowdin AOs) **')
dump_mat.dump_rec(mol.stdout,
c_inv.dot(mo_coeff[1]),
label,
molabel,
start=1)
dm = mf.make_rdm1(mo_coeff, mo_occ)
return mf.mulliken_meta(mol, dm, s=ovlp_ao, verbose=log)
def caslst_by_irrep(casscf,
mo_coeff,
cas_irrep_nocc,
cas_irrep_ncore=None,
s=None,
base=1):
'''Given number of active orbitals for each irrep, return the orbital
indices of active space
Args:
casscf : an :class:`CASSCF` or :class:`CASCI` object
cas_irrep_nocc : list or dict
Number of active orbitals for each irrep. It can be a dict, eg
{'A1': 2, 'B2': 4} to indicate the active space size based on
irrep names, or {0: 2, 3: 4} for irrep Id, or a list [2, 0, 0, 4]
(identical to {0: 2, 3: 4}) in which the list index is served as
the irrep Id.
Kwargs:
cas_irrep_ncore : list or dict
Number of closed shells for each irrep. It can be a dict, eg
{'A1': 6, 'B2': 4} to indicate the closed shells based on
irrep names, or {0: 6, 3: 4} for irrep Id, or a list [6, 0, 0, 4]
(identical to {0: 6, 3: 4}) in which the list index is served as
the irrep Id. If cas_irrep_ncore is not given, the program
will generate a guess based on the lowest :attr:`CASCI.ncore`
orbitals.
s : ndarray
overlap matrix
base : int
0-based (C-like) or 1-based (Fortran-like) caslst
Returns:
A list of orbital indices
Examples:
>>> from pyscf import gto, scf, mcscf
>>> mol = gto.M(atom='N 0 0 0; N 0 0 1', basis='ccpvtz', symmetry=True, verbose=0)
>>> mf = scf.RHF(mol)
>>> mf.kernel()
>>> mc = mcscf.CASSCF(mf, 12, 4)
>>> mcscf.caslst_by_irrep(mc, mf.mo_coeff, {'E1gx':4, 'E1gy':4, 'E1ux':2, 'E1uy':2})
[5, 7, 8, 10, 11, 14, 15, 20, 25, 26, 31, 32]
'''
mol = casscf.mol
log = logger.Logger(casscf.stdout, casscf.verbose)
if s is None:
s = casscf._scf.get_ovlp()
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_coeff, s)
orbsym = numpy.asarray(orbsym)
ncore = casscf.ncore
irreps = set(orbsym)
if cas_irrep_ncore is not None:
irrep_ncore = {}
for k, v in cas_irrep_ncore.items():
if isinstance(k, str):
irrep_ncore[symm.irrep_name2id(mol.groupname, k)] = v
else:
irrep_ncore[k] = v
ncore_rest = casscf.ncore - sum(irrep_ncore.values())
if ncore_rest > 0: # guess core configuration
mask = numpy.ones(len(orbsym), dtype=bool)
for ir in irrep_ncore:
mask[orbsym == ir] = False
core_rest = orbsym[mask][:ncore_rest]
core_rest = dict([(ir, numpy.count_nonzero(core_rest == ir))
for ir in set(core_rest)])
log.info('Given core space %s < casscf core size %d',
cas_irrep_ncore, casscf.ncore)
log.info('Add %s to core configuration', core_rest)
irrep_ncore.update(core_rest)
elif ncore_rest < 0:
raise ValueError('Given core space %s > casscf core size %d' %
(cas_irrep_ncore, casscf.ncore))
else:
irrep_ncore = dict([(ir, sum(orbsym[:ncore] == ir)) for ir in irreps])
if not isinstance(cas_irrep_nocc, dict):
# list => dict
cas_irrep_nocc = dict([(ir, n) for ir, n in enumerate(cas_irrep_nocc)
if n > 0])
irrep_ncas = {}
for k, v in cas_irrep_nocc.items():
if isinstance(k, str):
irrep_ncas[symm.irrep_name2id(mol.groupname, k)] = v
else:
irrep_ncas[k] = v
ncas_rest = casscf.ncas - sum(irrep_ncas.values())
if ncas_rest > 0:
mask = numpy.ones(len(orbsym), dtype=bool)
# remove core and specified active space
for ir in irrep_ncas:
mask[orbsym == ir] = False
for ir, ncore in irrep_ncore.items():
idx = numpy.where(orbsym == ir)[0]
mask[idx[:ncore]] = False
cas_rest = orbsym[mask][:ncas_rest]
cas_rest = dict([(ir, numpy.count_nonzero(cas_rest == ir))
for ir in set(cas_rest)])
log.info('Given active space %s < casscf active space size %d',
cas_irrep_nocc, casscf.ncas)
log.info('Add %s to active space', cas_rest)
irrep_ncas.update(cas_rest)
elif ncas_rest < 0:
raise ValueError(
'Given active space %s > casscf active space size %d' %
(cas_irrep_nocc, casscf.ncas))
caslst = []
for ir, ncas in irrep_ncas.items():
if ncas > 0:
if ir in irrep_ncore:
nc = irrep_ncore[ir]
else:
nc = 0
no = nc + ncas
idx = numpy.where(orbsym == ir)[0]
caslst.extend(idx[nc:no])
caslst = numpy.sort(numpy.asarray(caslst)) + base
if len(caslst) < casscf.ncas:
raise ValueError('Not enough orbitals found for core %s, cas %s' %
(cas_irrep_ncore, cas_irrep_nocc))
if log.verbose >= logger.INFO:
log.info(
'ncore for each irreps %s',
dict([(symm.irrep_id2name(mol.groupname, k), v)
for k, v in irrep_ncore.items()]))
log.info(
'ncas for each irreps %s',
dict([(symm.irrep_id2name(mol.groupname, k), v)
for k, v in irrep_ncas.items()]))
log.info('(%d-based) caslst = %s', base, caslst)
return caslst
def analyze(self, verbose=logger.DEBUG):
from pyscf.lo import orth
from pyscf.tools import dump_mat
mo_energy = self.mo_energy
mo_occ = self.mo_occ
mo_coeff = self.mo_coeff
log = logger.Logger(self.stdout, verbose)
mol = self.mol
nirrep = len(mol.irrep_id)
ovlp_ao = self.get_ovlp()
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_coeff,
s=ovlp_ao)
orbsym = numpy.array(orbsym)
wfnsym = 0
ndoccs = []
nsoccs = []
for k,ir in enumerate(mol.irrep_id):
ndoccs.append(sum(orbsym[mo_occ==2] == ir))
nsoccs.append(sum(orbsym[mo_occ==1] == ir))
if nsoccs[k] % 2:
wfnsym ^= ir
if mol.groupname in ('Dooh', 'Coov'):
log.info('TODO: total symmetry for %s', mol.groupname)
else:
log.info('total symmetry = %s',
symm.irrep_id2name(mol.groupname, wfnsym))
log.info('occupancy for each irrep: ' + (' %4s'*nirrep),
*mol.irrep_name)
log.info('double occ ' + (' %4d'*nirrep), *ndoccs)
log.info('single occ ' + (' %4d'*nirrep), *nsoccs)
log.info('**** MO energy ****')
irname_full = {}
for k,ir in enumerate(mol.irrep_id):
irname_full[ir] = mol.irrep_name[k]
irorbcnt = {}
if self._focka_ao is None:
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note('MO #%-3d (%s #%-2d), energy= %-18.15g occ= %g',
k+1, irname_full[j], irorbcnt[j],
mo_energy[k], mo_occ[k])
else:
mo_ea = numpy.einsum('ik,ik->k', mo_coeff, self._focka_ao.dot(mo_coeff))
mo_eb = numpy.einsum('ik,ik->k', mo_coeff, self._fockb_ao.dot(mo_coeff))
log.note(' Roothaan | alpha | beta')
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
log.note('MO #%-4d(%-3s #%-2d) energy= %-18.15g | %-18.15g | %-18.15g occ= %g',
k+1, irname_full[j], irorbcnt[j],
mo_energy[k], mo_ea[k], mo_eb[k], mo_occ[k])
if verbose >= logger.DEBUG:
label = mol.spheric_labels(True)
molabel = []
irorbcnt = {}
for k, j in enumerate(orbsym):
if j in irorbcnt:
irorbcnt[j] += 1
else:
irorbcnt[j] = 1
molabel.append('#%-d(%s #%d)' % (k+1, irname_full[j], irorbcnt[j]))
log.debug(' ** MO coefficients (expansion on meta-Lowdin AOs) **')
orth_coeff = orth.orth_ao(mol, 'meta_lowdin', s=ovlp_ao)
c = reduce(numpy.dot, (orth_coeff.T, ovlp_ao, mo_coeff))
dump_mat.dump_rec(self.stdout, c, label, molabel, start=1)
dm = self.make_rdm1(mo_coeff, mo_occ)
return self.mulliken_meta(mol, dm, s=ovlp_ao, verbose=verbose)
def get_occ(self, mo_energy=None, mo_coeff=None, orbsym=None):
''' We assumed mo_energy are grouped by symmetry irreps, (see function
self.eig). The orbitals are sorted after SCF.
'''
if mo_energy is None: mo_energy = self.mo_energy
mol = self.mol
if not mol.symmetry:
return hf.RHF.get_occ(self, mo_energy, mo_coeff)
if orbsym is None:
if mo_coeff is not None:
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
else:
orbsym = [
numpy.repeat(ir, mol.symm_orb[i].shape[1])
for i, ir in enumerate(mol.irrep_id)
]
orbsym = numpy.hstack(orbsym)
else:
orbsym = numpy.asarray(orbsym)
assert (mo_energy.size == orbsym.size)
mo_occ = numpy.zeros_like(mo_energy)
rest_idx = []
nelec_fix = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = numpy.where(orbsym == ir)[0]
if irname in self.irrep_nelec:
n = self.irrep_nelec[irname]
occ_sort = numpy.argsort(mo_energy[ir_idx].round(9))
occ_idx = ir_idx[occ_sort[:n // 2]]
mo_occ[occ_idx] = 2
nelec_fix += n
else:
rest_idx.append(ir_idx)
nelec_float = mol.nelectron - nelec_fix
assert (nelec_float >= 0)
if nelec_float > 0:
rest_idx = numpy.hstack(rest_idx)
occ_sort = numpy.argsort(mo_energy[rest_idx].round(9))
occ_idx = rest_idx[occ_sort[:nelec_float // 2]]
mo_occ[occ_idx] = 2
vir_idx = (mo_occ == 0)
if self.verbose >= logger.INFO and numpy.count_nonzero(vir_idx) > 0:
ehomo = max(mo_energy[mo_occ > 0])
elumo = min(mo_energy[mo_occ == 0])
noccs = []
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = (orbsym == ir)
noccs.append(int(mo_occ[ir_idx].sum()))
if ehomo in mo_energy[ir_idx]:
irhomo = irname
if elumo in mo_energy[ir_idx]:
irlumo = irname
logger.info(self, 'H**O (%s) = %.15g LUMO (%s) = %.15g', irhomo,
ehomo, irlumo, elumo)
logger.debug(self, 'irrep_nelec = %s', noccs)
_dump_mo_energy(mol,
mo_energy,
mo_occ,
ehomo,
elumo,
orbsym,
verbose=self.verbose)
return mo_occ
def writeNumpyforMRLCC(mc, E1, E2, frozen) :
ncore = mc.ncore
nact = mc.ncas
norbs = mc.mo_coeff.shape[1]
nelec = mc.nelecas[0]+mc.nelecas[1]
nvirt = norbs - ncore-nact
nc = ncore+nact
nactElec = nelec - 2*ncore
#this is chemistry notation
int2popo = ao2mo.outcore.general_iofree(mc.mol, (mc.mo_coeff, mc.mo_coeff[:,:nc], mc.mo_coeff, mc.mo_coeff[:,:nc]), compact=False)
int2ppoo = ao2mo.outcore.general_iofree(mc.mol, (mc.mo_coeff, mc.mo_coeff, mc.mo_coeff[:,:nc], mc.mo_coeff[:,:nc]), compact=False)
int2popo.shape=(norbs, nc, norbs, nc)
int2ppoo.shape=(norbs, norbs, nc, nc)
mo = mc.mo_coeff
dmcore = numpy.dot(mo[:,:frozen], mo[:,:frozen].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
int1 = reduce(numpy.dot, (mc.mo_coeff.T, mc.get_hcore(), mc.mo_coeff)) +vhfcore
dmcore = numpy.dot(mo[:,:ncore], mo[:,:ncore].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
int1_eff = reduce(numpy.dot, (mc.mo_coeff.T, mc.get_hcore(), mc.mo_coeff)) +vhfcore
#int1_eff = makeheff(int1, int2popo, int2ppoo, E1, ncore, nvirt, frozen)
energy_frozen_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
#numpy.save("int/E3",E3)
#numpy.save("int/E3B.npy", E3.transpose(0,3,1,4,2,5))
#numpy.save("int/E3C.npy", E3.transpose(5,0,2,4,1,3))
numpy.save("int/E2",numpy.asfortranarray(E2))
numpy.save("int/E1",numpy.asfortranarray(E1))
#numpy.save("int/int2",int2)
numpy.save("int/int1",numpy.asfortranarray(int1[frozen:,frozen:]))
numpy.save("int/int1eff",numpy.asfortranarray(int1_eff[frozen:, frozen:]))
numpy.save("int/W:caca", numpy.asfortranarray(int2ppoo[frozen:ncore, frozen:ncore, ncore:nc, ncore:nc].transpose(0,2,1,3)))
numpy.save("int/W:caac", numpy.asfortranarray(int2popo[frozen:ncore,ncore:nc, ncore:nc, frozen:ncore].transpose(0,2,1,3)))
numpy.save("int/W:cece", numpy.asfortranarray(int2ppoo[nc:, nc:, frozen:ncore, frozen:ncore].transpose(2,0,3,1)))
numpy.save("int/W:ceec", numpy.asfortranarray(int2popo[nc:, frozen:ncore, nc:, frozen:ncore].transpose(1,2,0,3)))
numpy.save("int/W:aeae", numpy.asfortranarray(int2ppoo[nc:, nc:, ncore:nc,ncore:nc].transpose(2,0,3,1)))
numpy.save("int/W:aeea", numpy.asfortranarray(int2popo[nc:, ncore:nc,nc:, ncore:nc].transpose(1,2,0,3)))
numpy.save("int/W:cccc", numpy.asfortranarray(int2ppoo[frozen:ncore,frozen:ncore, frozen:ncore, frozen:ncore].transpose(0,2,1,3)))
numpy.save("int/W:aaaa", numpy.asfortranarray(int2ppoo[ncore:nc,ncore:nc, ncore:nc, ncore:nc].transpose(0,2,1,3)))
feri = h5py.File("int/int2eeee.hdf5", 'w')
ao2mo.full(mc.mol, mc.mo_coeff[:,nc:], feri, compact=False)
for o in range(nvirt):
int2eee = feri['eri_mo'][o*(norbs-nc):(o+1)*(norbs-nc),:]
numpy.asfortranarray(int2eee).tofile("int/W:eeee%04d"%(o))
#store perturbers
numpy.save("int/W:eecc", numpy.asfortranarray(int2popo[nc:,frozen:ncore,nc:,frozen:ncore].transpose(0,2,1,3)))
numpy.save("int/W:eeca", numpy.asfortranarray(int2popo[nc:,frozen:ncore, nc:, ncore:nc].transpose(0,2,1,3)))
numpy.save("int/W:ccaa", numpy.asfortranarray(int2popo[frozen:ncore,ncore:nc, frozen:ncore, ncore:nc].transpose(0,2,1,3)))
numpy.save("int/W:eeaa", numpy.asfortranarray(int2popo[nc:,ncore:nc, nc:, ncore:nc].transpose(0,2,1,3)))
numpy.save("int/W:eaca", numpy.asfortranarray(int2popo[nc:,frozen:ncore, ncore:nc, ncore:nc].transpose(0,2,1,3)))
numpy.save("int/W:aeca", numpy.asfortranarray(int2popo[ncore:nc,frozen:ncore, nc:,ncore:nc].transpose(0,2,1,3)))
numpy.save("int/W:ccae", numpy.asfortranarray(int2popo[frozen:ncore,ncore:nc, nc:, frozen:ncore].transpose(0,3,1,2)))
#write FCIDUMP_AAAV and FCIDUMP_AAAC
from pyscf import symm
mol = mc.mol
orbsymout=[]
orbsym = []
if (mol.symmetry):
orbsym = symm.label_orb_symm(mc.mol, mc.mol.irrep_id,
mc.mol.symm_orb, mc.mo_coeff, s=mc._scf.get_ovlp())
if mol.symmetry and orbsym:
if mol.groupname.lower() == 'dooh':
orbsymout = [dmrg_sym.IRREP_MAP['D2h'][i % 10] for i in orbsym]
elif mol.groupname.lower() == 'coov':
orbsymout = [dmrg_sym.IRREP_MAP['C2v'][i % 10] for i in orbsym]
else:
orbsymout = [dmrg_sym.IRREP_MAP[mol.groupname][i] for i in orbsym]
else:
orbsymout = []
'''
dmcore = numpy.dot(mo[:,frozen:ncore], mo[:,frozen:ncore].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
h1eff = int1+vhfcore
energy_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5\
+energy_frozen_core
'''
dmcore = numpy.dot(mo[:,:ncore], mo[:,:ncore].T)*2
vj, vk = mc._scf.get_jk(mc.mol, dmcore)
vhfcore = reduce(numpy.dot, (mo.T, vj-vk*0.5, mo))
h1eff = int1_eff
energy_core = numpy.einsum('ij,ji', dmcore, mc.get_hcore()) \
+ numpy.einsum('ij,ji', dmcore, vj-0.5*vk) * .5
#print energy_core2+mc.mol.energy_nuc(), energy_core+mc.mol.energy_nuc(), energy_frozen_core+mc.mol.energy_nuc()
nc = mc.ncore+mc.ncas
energyE0 = 1.0*numpy.einsum('ij,ij', h1eff[ncore:nc, ncore:nc], E1)
#+ 0.5*numpy.einsum('ikjl,ijkl', E2, int2ppoo[ncore:,ncore:,ncore:,ncore:])
for i in range(mc.ncas):
for j in range(mc.ncas):
for k in range(mc.ncas):
for l in range(mc.ncas):
I,J = max(i,j)+ncore, min(i,j)+ncore
K,L = max(k,l)+ncore, min(k,l)+ncore
energyE0 += 0.5*E2[i,k,j,l] * int2ppoo[i+ncore, j+ncore, k+ncore, l+ncore]
energyE0 += energy_core
energyE0 += mc.mol.energy_nuc()
print "Energy = ", energyE0
fout = open('FCIDUMP_aaav0','w')
tools.fcidump.write_head(fout, int1.shape[0]-ncore, mc.mol.nelectron-2*ncore, orbsym= orbsymout[ncore:])
for i in range(ncore,int1.shape[0]):
for j in range(ncore, i+1):
for k in range(mc.ncas):
for l in range(k+1):
if abs(int2ppoo[i,j, k+ncore,l+ncore]) > 1.e-8 :
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (int2ppoo[i,j, k+ncore,l+ncore], i+1-ncore, j+1-ncore, k+1, l+1))
if (j >= nc and abs(int2popo[i, k+ncore, j, l+ncore]) > 1.e-8):
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (int2popo[i,k+ncore,j, l+ncore], i+1-ncore, k+1, l+1, j+1-ncore))
if (j >= nc and abs(int2popo[i, l+ncore, j, k+ncore]) > 1.e-8):
fout.write(' %17.9e %4d %4d %4d %4d\n' \
% (int2popo[i,l+ncore, j, k+ncore], i+1-ncore, l+1, k+1, j+1-ncore))
tools.fcidump.write_hcore(fout, h1eff[ncore:,ncore:], int1.shape[0]-ncore, tol=1e-8)
fout.write(' %17.9e 0 0 0 0\n' %( mc.mol.energy_nuc()+energy_core-energyE0))
fout.close()
nc = ncore+mc.ncas
eri1cas = ao2mo.outcore.general_iofree(mc.mol, (mc.mo_coeff[:,frozen:nc], mc.mo_coeff[:,frozen:nc], mc.mo_coeff[:,frozen:nc], mc.mo_coeff[:,frozen:nc]), compact=True)
tools.fcidump.from_integrals("FCIDUMP_aaac", int1[frozen:nc,frozen:nc], eri1cas, nc-frozen, mc.mol.nelectron-2*frozen, nuc=mc.mol.energy_nuc()-energyE0, orbsym = orbsymout[frozen:nc], tol=1e-8)
return energyE0, norbs
#
# call mol.build to construct symmetry adapted basis.
#
# NOTE the molecule orientation. Simply assigning mol.build(symmetry=True)
# may change the orientation of the molecule. If the orientation is different
# to the orientation of the orbital space, the orbitals cannot be symmetrized.
# To keep the molecule orientation fixed, we need specify the molecular
# symmetry.
#
mol.build(0, 0, symmetry='D2')
#
# H**O-2 H**O-1 H**O are degenerated. They may not be properly symmetrized.
#
try:
irrep_ids = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mo)
except ValueError:
print('The orbital symmetry cannot be labelled because some '
'degenerated orbitals are not symmetrized.\n'
'Degenerated H**O energy: %s' % mf.mo_energy[2:5])
nocc = mol.nelectron // 2
occ_orb = symm.symmetrize_space(mol, mo[:,:nocc])
irrep_ids = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, occ_orb)
print('Occupied orbital symmetry: %s' % irrep_ids)
virt_orb = symm.symmetrize_space(mol, mo[:,nocc:])
irrep_ids = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, virt_orb)
print('Virtual orbital symmetry: %s' % irrep_ids)
'O': 'sto-3g',}
mol.symmetry = 1
mol.build()
m = scf.RHF(mol)
ehf = m.scf()
norb = m.mo_coeff.shape[1]
nelec = mol.nelectron
h1e = reduce(numpy.dot, (m.mo_coeff.T, scf.hf.get_hcore(mol), m.mo_coeff))
eri = ao2mo.incore.full(m._eri, m.mo_coeff)
numpy.random.seed(1)
na = cistring.num_strings(norb, nelec//2)
fcivec = numpy.random.random((na,na))
fcivec = fcivec + fcivec.T
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, m.mo_coeff)
print(numpy.allclose(orbsym, [0, 0, 2, 0, 3, 0, 2]))
cis = FCISolver(mol)
cis.orbsym = cis.orbsym
ci1 = cis.contract_2e(eri, fcivec, norb, nelec)
ci1ref = direct_spin0.contract_2e(eri, fcivec, norb, nelec)
print(numpy.allclose(ci1ref, ci1))
mol.atom = [['H', (0, 0, i)] for i in range(8)]
mol.basis = {'H': 'sto-3g'}
mol.symmetry = True
mol.build()
m = scf.RHF(mol)
ehf = m.scf()
norb = m.mo_coeff.shape[1]
def dmrgci(mf, TwoS, Nelec, Irrep, DSU2, Econv, MaxSweeps, NoisePrefac, frozen,
active):
### Check whether the frozen and active arrays make sense ###
Norbs = mf.mol.nao_nr()
assert (np.sum(frozen < Norbs) == len(frozen))
assert (np.sum(active < Norbs) == len(active))
assert (np.sum(frozen >= 0) == len(frozen))
assert (np.sum(active >= 0) == len(active))
mo_occ = mf.mo_occ
for item in frozen:
assert (mo_occ[item] == 2)
for item2 in active:
assert (item != item2)
frozen = frozen[frozen.argsort()]
active = active[active.argsort()]
### Get orbital information ###
if (len(frozen) > 0):
mo_fro = mf.mo_coeff[:, frozen]
mo_act = mf.mo_coeff[:, active]
Orbsym = np.array(
symm.label_orb_symm(
mf.mol, mf.mol.irrep_id, mf.mol.symm_orb,
mf.mo_coeff))[active] # Same conventions in PySCF and CheMPS2
for cnt in range(len(Orbsym)):
# https://github.com/sunqm/pyscf/blob/master/symm/basis.py#L128
Orbsym[cnt] = Orbsym[cnt] % 10
### Get the JK matrix for the doubly occupied frozen orbitals ###
if (len(frozen) > 0):
DM_docc = np.zeros([Norbs], dtype=float)
DM_docc[frozen] = 2.0
JK_docc = fetchJK_mo(mf, np.diag(DM_docc), mf.mo_coeff)
JK_fro = (JK_docc[:, frozen])[frozen, :]
JK_act = (JK_docc[:, active])[active, :]
### Build the rotated MO matrix elements ###
Lrot = len(active)
OEIao = mf.mol.intor('cint1e_kin_sph') + mf.mol.intor('cint1e_nuc_sph')
CONST = mf.mol.energy_nuc()
OEImo = np.dot(np.dot(mo_act.T, OEIao), mo_act)
if (len(frozen) > 0):
CONST += np.einsum(
'ii->', 2 * np.dot(np.dot(mo_fro.T, OEIao), mo_fro) + JK_fro)
OEImo += JK_act
#TEINT in chemical notation; also possible to pass different shapes; see http://www.sunqm.net/pyscf/tutorial.html#hf-mp2-mcscf
TEImo = ao2mo.outcore.full_iofree(mf.mol, mo_act, compact=False).reshape(
Lrot, Lrot, Lrot, Lrot)
### Reorder per irrep ### --> not strictly necessary for CheMPS2, but converges faster
idx = Orbsym.argsort()
OEImo = OEImo[:, idx]
OEImo = OEImo[idx, :]
TEImo = TEImo[:, :, :, idx]
TEImo = TEImo[:, :, idx, :]
TEImo = TEImo[:, idx, :, :]
TEImo = TEImo[idx, :, :, :]
Orbsym = Orbsym[idx]
### Do DMRG calculation with CheMPS2 ###
EnergyDMRG, TwoRDM = call_chemps2(Lrot, mf.mol.groupname, Orbsym, CONST,
OEImo, TEImo, TwoS,
Nelec - 2 * len(frozen), Irrep, DSU2,
Econv, MaxSweeps, NoisePrefac)
### Reorder back to original ordering ###
idx2 = idx.argsort()
assert (np.linalg.norm(idx[idx2] - idx2[idx]) < 1e-10)
TwoRDM = TwoRDM[:, :, :, idx2]
TwoRDM = TwoRDM[:, :, idx2, :]
TwoRDM = TwoRDM[:, idx2, :, :]
TwoRDM = TwoRDM[idx2, :, :, :]
return (EnergyDMRG, TwoRDM)
idx = ordering_diatomics(mol, C, basis_set=basis_set)
norb = cas_nstop - cas_nstart
h, g = reorder_integrals(idx, h, g)
C = C[:, idx]
mo_energy = mo_energy[idx]
dm_aa = dm_aa[:, idx]
dm_aa = dm_aa[idx, :]
dm_bb = dm_bb[:, idx]
dm_bb = dm_bb[idx, :]
print(h)
print(dm_aa)
from pyscf import symm
mo = symm.symmetrize_orb(mol, C)
osym = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mo)
#symm.addons.symmetrize_space(mol, mo, s=None, check=True, tol=1e-07)
for i in range(len(osym)):
print("%4d %8s %16.8f" % (i, osym[i], mo_energy[i]))
print("r:", r0)
print(h)
if do_tci:
oocmf = CmfSolver(h, g, ecore, blocks, init_fspace, C, max_roots=100)
oocmf.init((dm_aa, dm_bb))
oocmf.form_extra_fspace() #form excited fock space configurations
h = oocmf.h
g = oocmf.g
#
# Symmetry adapted FCI solver can be called with arbitrary Hamiltonian. In the
# following example, you need to prepare 1-electron and 2-electron integrals,
# core energy shift, and the symmetry of orbitals.
#
cas_idx = numpy.arange(2, 10)
core_idx = numpy.arange(2)
mo_cas = m.mo_coeff[:, cas_idx]
mo_core = m.mo_coeff[:, core_idx]
dm_core = mo_core.dot(mo_core.T) * 2
vhf_core = m.get_veff(mol, dm_core)
h1 = mo_cas.T.dot(m.get_hcore() + vhf_core).dot(mo_cas)
h2 = ao2mo.kernel(mol, mo_cas)
ecore = (numpy.einsum('ij,ji', dm_core, m.get_hcore()) +
.5 * numpy.einsum('ij,ji', dm_core, vhf_core) + m.energy_nuc())
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, mo_cas)
norb = mo_cas.shape[1]
ncore = mo_core.shape[1]
nelec = mol.nelectron - ncore * 2
fs = fci.direct_spin0_symm.FCI(mol)
fs.wfnsym = 'A2'
e, c = fs.kernel(h1, h2, norb, nelec, ecore=ecore, orbsym=orbsym, verbose=5)
print('Energy of %s state %.12f' % (fs.wfnsym, e))
#
# mcscf module has a function h1e_for_cas to generate 1-electron Hamiltonian and
# core energy.
#
cas_idx = numpy.arange(2, 10)
core_idx = numpy.arange(2)
def get_occ(self, mo_energy=None, mo_coeff=None, orbsym=None):
if mo_energy is None: mo_energy = self.mo_energy
mol = self.mol
if mo_coeff is None or self._focka_ao is None:
mo_ea = mo_eb = mo_energy
else:
mo_ea = numpy.einsum('ik,ik->k', mo_coeff, self._focka_ao.dot(mo_coeff))
mo_eb = numpy.einsum('ik,ik->k', mo_coeff, self._fockb_ao.dot(mo_coeff))
nmo = mo_ea.size
mo_occ = numpy.zeros(nmo)
if orbsym is None:
if mo_coeff is not None:
orbsym = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff, self.get_ovlp(), False)
orbsym = numpy.asarray(orbsym)
else:
orbsym = [numpy.repeat(ir, mol.symm_orb[i].shape[1])
for i, ir in enumerate(mol.irrep_id)]
orbsym = numpy.hstack(orbsym)
else:
orbsym = numpy.asarray(orbsym)
assert(mo_energy.size == orbsym.size)
float_idx = []
neleca_fix = 0
nelecb_fix = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = numpy.where(orbsym == ir)[0]
if irname in self.irrep_nelec:
if isinstance(self.irrep_nelec[irname], (int, numpy.integer)):
nelecb = self.irrep_nelec[irname] // 2
neleca = self.irrep_nelec[irname] - nelecb
else:
neleca, nelecb = self.irrep_nelec[irname]
mo_occ[ir_idx] = rohf._fill_rohf_occ(mo_energy[ir_idx],
mo_ea[ir_idx], mo_eb[ir_idx],
nelecb, neleca-nelecb)
neleca_fix += neleca
nelecb_fix += nelecb
else:
float_idx.append(ir_idx)
nelec_float = mol.nelectron - neleca_fix - nelecb_fix
assert(nelec_float >= 0)
if len(float_idx) > 0:
float_idx = numpy.hstack(float_idx)
nopen = mol.spin - (neleca_fix - nelecb_fix)
ncore = (nelec_float - nopen)//2
mo_occ[float_idx] = rohf._fill_rohf_occ(mo_energy[float_idx],
mo_ea[float_idx],
mo_eb[float_idx],
ncore, nopen)
ncore = self.nelec[1]
nocc = self.nelec[0]
nopen = nocc - ncore
vir_idx = (mo_occ==0)
if self.verbose >= logger.INFO and nocc < nmo and ncore > 0:
ehomo = max(mo_energy[mo_occ> 0])
elumo = min(mo_energy[mo_occ==0])
ndoccs = []
nsoccs = []
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idx = (orbsym == ir)
ndoccs.append(numpy.count_nonzero(mo_occ[ir_idx]==2))
nsoccs.append(numpy.count_nonzero(mo_occ[ir_idx]==1))
if ehomo in mo_energy[ir_idx]:
irhomo = irname
if elumo in mo_energy[ir_idx]:
irlumo = irname
# to help self.eigh compute orbital energy
self._irrep_doccs = ndoccs
self._irrep_soccs = nsoccs
logger.info(self, 'H**O (%s) = %.15g LUMO (%s) = %.15g',
irhomo, ehomo, irlumo, elumo)
logger.debug(self, 'double occ irrep_nelec = %s', ndoccs)
logger.debug(self, 'single occ irrep_nelec = %s', nsoccs)
#_dump_mo_energy(mol, mo_energy, mo_occ, ehomo, elumo, orbsym,
# verbose=self.verbose)
if nopen > 0:
core_idx = mo_occ == 2
open_idx = mo_occ == 1
vir_idx = mo_occ == 0
logger.debug(self, ' Roothaan | alpha | beta')
logger.debug(self, ' Highest 2-occ = %18.15g | %18.15g | %18.15g',
max(mo_energy[core_idx]),
max(mo_ea[core_idx]), max(mo_eb[core_idx]))
logger.debug(self, ' Lowest 0-occ = %18.15g | %18.15g | %18.15g',
min(mo_energy[vir_idx]),
min(mo_ea[vir_idx]), min(mo_eb[vir_idx]))
for i in numpy.where(open_idx)[0]:
logger.debug(self, ' 1-occ = %18.15g | %18.15g | %18.15g',
mo_energy[i], mo_ea[i], mo_eb[i])
numpy.set_printoptions(threshold=nmo)
logger.debug(self, ' Roothaan mo_energy =\n%s', mo_energy)
logger.debug1(self, ' alpha mo_energy =\n%s', mo_ea)
logger.debug1(self, ' beta mo_energy =\n%s', mo_eb)
numpy.set_printoptions(threshold=1000)
return mo_occ
def get_occ(self, mo_energy=None, mo_coeff=None, orbsym=None):
''' We assumed mo_energy are grouped by symmetry irreps, (see function
self.eig). The orbitals are sorted after SCF.
'''
if mo_energy is None: mo_energy = self.mo_energy
mol = self.mol
if orbsym is None:
if mo_coeff is not None: # due to linear-dep
ovlp_ao = self.get_ovlp()
orbsyma = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff[0], ovlp_ao, False)
orbsymb = symm.label_orb_symm(self, mol.irrep_id, mol.symm_orb,
mo_coeff[1], ovlp_ao, False)
orbsyma = numpy.asarray(orbsyma)
orbsymb = numpy.asarray(orbsymb)
else:
ovlp_ao = None
orbsyma = [
numpy.repeat(ir, mol.symm_orb[i].shape[1])
for i, ir in enumerate(mol.irrep_id)
]
orbsyma = orbsymb = numpy.hstack(orbsyma)
else:
orbsyma = numpy.asarray(orbsym[0])
orbsymb = numpy.asarray(orbsym[1])
assert (mo_energy[0].size == orbsyma.size)
mo_occ = numpy.zeros_like(mo_energy)
idx_ea_left = []
idx_eb_left = []
neleca_fix = nelecb_fix = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idxa = numpy.where(orbsyma == ir)[0]
ir_idxb = numpy.where(orbsymb == ir)[0]
if irname in self.irrep_nelec:
if isinstance(self.irrep_nelec[irname], (int, numpy.integer)):
nelecb = self.irrep_nelec[irname] // 2
neleca = self.irrep_nelec[irname] - nelecb
else:
neleca, nelecb = self.irrep_nelec[irname]
ea_idx = numpy.argsort(mo_energy[0][ir_idxa])
eb_idx = numpy.argsort(mo_energy[1][ir_idxb])
mo_occ[0, ir_idxa[ea_idx[:neleca]]] = 1
mo_occ[1, ir_idxb[eb_idx[:nelecb]]] = 1
neleca_fix += neleca
nelecb_fix += nelecb
else:
idx_ea_left.append(ir_idxa)
idx_eb_left.append(ir_idxb)
neleca_float = self.nelec[0] - neleca_fix
nelecb_float = self.nelec[1] - nelecb_fix
assert (neleca_float >= 0)
assert (nelecb_float >= 0)
if len(idx_ea_left) > 0:
idx_ea_left = numpy.hstack(idx_ea_left)
ea_left = mo_energy[0][idx_ea_left]
ea_sort = numpy.argsort(ea_left)
occ_idx = idx_ea_left[ea_sort][:neleca_float]
mo_occ[0][occ_idx] = 1
if len(idx_eb_left) > 0:
idx_eb_left = numpy.hstack(idx_eb_left)
eb_left = mo_energy[1][idx_eb_left]
eb_sort = numpy.argsort(eb_left)
occ_idx = idx_eb_left[eb_sort][:nelecb_float]
mo_occ[1][occ_idx] = 1
vir_idx = (mo_occ[0] == 0)
if self.verbose >= logger.INFO and numpy.count_nonzero(vir_idx) > 0:
ehomoa = max(mo_energy[0][mo_occ[0] > 0])
elumoa = min(mo_energy[0][mo_occ[0] == 0])
ehomob = max(mo_energy[1][mo_occ[1] > 0])
elumob = min(mo_energy[1][mo_occ[1] == 0])
noccsa = []
noccsb = []
p0 = 0
for i, ir in enumerate(mol.irrep_id):
irname = mol.irrep_name[i]
ir_idxa = orbsyma == ir
ir_idxb = orbsymb == ir
noccsa.append(numpy.count_nonzero(mo_occ[0][ir_idxa]))
noccsb.append(numpy.count_nonzero(mo_occ[1][ir_idxb]))
if ehomoa in mo_energy[0][ir_idxa]:
irhomoa = irname
if elumoa in mo_energy[0][ir_idxa]:
irlumoa = irname
if ehomob in mo_energy[1][ir_idxb]:
irhomob = irname
if elumob in mo_energy[1][ir_idxb]:
irlumob = irname
logger.info(self, 'alpha H**O (%s) = %.15g LUMO (%s) = %.15g',
irhomoa, ehomoa, irlumoa, elumoa)
logger.info(self, 'beta H**O (%s) = %.15g LUMO (%s) = %.15g',
irhomob, ehomob, irlumob, elumob)
ehomo = max(ehomoa, ehomob)
elumo = min(elumoa, elumob)
logger.debug(self, 'alpha irrep_nelec = %s', noccsa)
logger.debug(self, 'beta irrep_nelec = %s', noccsb)
hf_symm._dump_mo_energy(mol,
mo_energy[0],
mo_occ[0],
ehomo,
elumo,
orbsyma,
'alpha-',
verbose=self.verbose)
hf_symm._dump_mo_energy(mol,
mo_energy[1],
mo_occ[1],
ehomo,
elumo,
orbsymb,
'beta-',
verbose=self.verbose)
if mo_coeff is not None and self.verbose >= logger.DEBUG:
if ovlp_ao is None:
ovlp_ao = self.get_ovlp()
ss, s = self.spin_square((mo_coeff[0][:, mo_occ[0] > 0],
mo_coeff[1][:, mo_occ[1] > 0]),
ovlp_ao)
logger.debug(self, 'multiplicity <S^2> = %.8g 2S+1 = %.8g',
ss, s)
return mo_occ
}
mol.symmetry = 1
mol.build()
m = scf.RHF(mol)
ehf = m.scf()
norb = m.mo_coeff.shape[1]
nelec = mol.nelectron - 1
h1e = reduce(numpy.dot, (m.mo_coeff.T, scf.hf.get_hcore(mol), m.mo_coeff))
eri = ao2mo.incore.full(m._eri, m.mo_coeff)
numpy.random.seed(1)
na = cistring.num_strings(norb, nelec // 2 + 1)
nb = cistring.num_strings(norb, nelec // 2)
fcivec = numpy.random.random((na, nb))
orbsym = symm.label_orb_symm(mol, mol.irrep_id, mol.symm_orb, m.mo_coeff)
cis = FCISolver(mol)
cis.orbsym = orbsym
fcivec = addons.symmetrize_wfn(fcivec, norb, nelec, cis.orbsym, wfnsym=0)
ci1 = cis.contract_2e(eri,
fcivec,
norb,
nelec,
orbsym=cis.orbsym,
wfnsym=0)
ci1ref = direct_spin1.contract_2e(eri, fcivec, norb, nelec)
print(numpy.allclose(ci1ref, ci1))
ci1 = contract_2e(eri, fcivec, norb, nelec, orbsym=orbsym)
ci1ref = direct_spin1.contract_2e(eri, fcivec, norb, nelec)
def test_1():
### PYSCF INPUT
r0 = 2.0
molecule = '''
C -4.308669 0.197146 0.000000
C 4.308669 -0.197146 0.000000
C -3.110874 -0.411353 0.000000
C 3.110874 0.411353 0.000000
H -4.394907 1.280613 0.000000
H 4.394907 -1.280613 0.000000
H -5.234940 -0.367304 0.000000
H 5.234940 0.367304 0.000000
H -3.069439 -1.500574 0.000000
H 3.069439 1.500574 0.000000
C -1.839087 0.279751 0.000000
C 1.839087 -0.279751 0.000000
C -0.634371 -0.341144 0.000000
C 0.634371 0.341144 0.000000
H -1.871161 1.369551 0.000000
H 1.871161 -1.369551 0.000000
H -0.607249 -1.431263 0.000000
H 0.607249 1.431263 0.000000
'''
charge = 0
spin = 0
basis_set = 'sto-3g'
npoly = 4
na = npoly
nb = npoly
### TPSCI BASIS INPUT
orb_basis = 'PM'
cas_nel = 2*npoly
cas_norb = 2*npoly
#Integrals from pyscf
import pyscf
from pyscf import gto, scf, ao2mo, molden, lo
pyscf.lib.num_threads(1) #with degenerate states and multiple processors there can be issues
#PYSCF inputs
mol = gto.Mole()
mol.atom = molecule
mol.max_memory = 1000 # MB
mol.symmetry = True
mol.charge = charge
mol.spin = spin
mol.basis = basis_set
mol.build()
print("symmertry")
print(mol.topgroup)
#SCF
#mf = scf.RHF(mol).run(init_guess='atom')
mf = scf.RHF(mol).run(conv_tol=1e-14)
#C = mf.mo_coeff #MO coeffs
enu = mf.energy_nuc()
if mol.symmetry == True:
from pyscf import symm
mo = symm.symmetrize_orb(mol, mf.mo_coeff)
osym = symm.label_orb_symm(mol, mol.irrep_name, mol.symm_orb, mo)
#symm.addons.symmetrize_space(mol, mo, s=None, check=True, tol=1e-07)
for i in range(len(osym)):
print("%4d %8s %16.8f"%(i+1,osym[i],mf.mo_energy[i]))
h,ecore,g,C = get_pi_space(mol,mf,cas_norb,cas_nel,local=True)
print("ecore %16.8f"%ecore)
print("MULLIKEN")
m1 = mulliken_ordering(mol,h.shape[0],C)
ppp = np.column_stack(np.where(m1>.90))
print(ppp)
idx = list(ppp[:,1])
m2 = np.where(m1>.90)
idx = m2[1]
C = C[:,idx]
h,g = reorder_integrals(idx,h,g)
#molden.from_mo(mol, 'cas.molden', C)
blocks = [[0,1,2,3],[4,5],[6,7]]
init_fspace = ((2,2),(1,1),(1,1))
#blocks = [[0,1,2,3],[4,5,6,7]]
#init_fspace = ((2,2),(2,2))
from scipy import optimize
oocmf = CmfSolver(h, g, ecore, blocks, init_fspace,C)
oocmf.init()
x = np.zeros_like(h)
min_options = {'gtol': 1e-8, 'disp':False}
opt_result = scipy.optimize.minimize(oocmf.energy, x, jac=oocmf.grad, method = 'BFGS', options=min_options )
#opt_result = scipy.optimize.minimize(oocmf.energy, x, jac=oocmf.grad, method = 'BFGS', callback=oocmf.callback)
print(opt_result.x)
Kpq = opt_result.x.reshape(h.shape)
print(Kpq)
e_fcmf = oocmf.energy_dps()
oocmf.rotate(Kpq)
e_ocmf = oocmf.energy_dps()
print("Orbital Frozen CMF:%12.8f"%e_fcmf)
print("Orbital Optimized CMF:%12.8f"%e_ocmf)
h = oocmf.h
g = oocmf.g
clustered_ham = oocmf.clustered_ham
ci_vector = oocmf.ci_vector
edps = build_hamiltonian_diagonal(clustered_ham,ci_vector)
print("%16.10f"%edps)
#ref_grad = np.array([[-0., -0., -0., -0., -0.136637, -0.001116, -0.00094, 0.030398],
# [ 0., 0., -0., -0., -0.001116, -0.136637, 0.030398, -0.00094 ],
# [ 0., 0., 0., 0., 0.001942, -0.033806, 0.123316, -0.002399],
# [ 0., 0., -0., -0., -0.033806, 0.001942, -0.002399, 0.123316],
# [ 0.136637, 0.001116, -0.001942, 0.033806, 0., 0., 0., 0. ],
# [ 0.001116, 0.136637, 0.033806, -0.001942, 0., -0., 0., 0. ],
# [ 0.00094, -0.030398, -0.123316, 0.002399, -0., -0., 0., 0. ],
# [-0.030398, 0.00094, 0.002399, -0.123316, -0., -0., 0., 0. ]])
ref_angles= np.array([[ 0., -0., -0., -0., -0.097782, 0.002467, -0.005287, 0.00192 ],
[ 0., -0., -0., -0., 0.002467, -0.097782, 0.00192, -0.005287],
[ 0., 0., 0., 0., -0.002466, -0.123235, 0.155944, -0.004683],
[ 0., 0., -0., 0., -0.123235, -0.002466, -0.004683, 0.155944],
[ 0.097782, -0.002467, 0.002466, 0.123235, 0., 0., -0.002248, 0.581917],
[-0.002467, 0.097782, 0.123235, 0.002466, -0., -0., 0.581917, -0.002248],
[ 0.005287, -0.00192, -0.155944, 0.004683, 0.002248, -0.581917, 0., -0. ],
[-0.00192, 0.005287, 0.004683, -0.155944, -0.581917, 0.002248, 0., 0. ]])
print(Kpq)
print(ref_angles)
try:
assert(np.allclose(Kpq,ref_angles,atol=1e-5))
except:
assert(np.allclose(-1*Kpq,ref_angles,atol=1e-5))
assert(abs(e_fcmf - -8.266997040181 ) <1e-8)
assert(abs(e_ocmf - -8.528879972678 ) <1e-8)
