def get_eri(mydf, kpts=None, compact=True):
if mydf._cderi is None or mydf.auxcell is None:
mydf.build()
kptijkl = _format_kpts(kpts)
eri = aft_ao2mo.get_eri(mydf, kptijkl, compact=compact)
eri += df_ao2mo.get_eri(mydf, kptijkl, compact=compact)
return eri
def get_eri(mydf, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_get_eri_compact', True)):
if mydf._cderi is None:
mydf.build()
kptijkl = _format_kpts(kpts)
eri = aft_ao2mo.get_eri(mydf, kptijkl, compact=compact)
eri += df_ao2mo.get_eri(mydf, kptijkl, compact=compact)
return eri
def get_eri(mydf, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_get_eri_compact', True)):
if mydf._cderi is None:
mydf.build()
kptijkl = _format_kpts(kpts)
eri = aft_ao2mo.get_eri(mydf, kptijkl, compact=compact)
eri += df_ao2mo.get_eri(mydf, kptijkl, compact=compact)
return eri
def general(mydf, mo_coeffs, kpts=None, compact=True):
if mydf._cderi is None or mydf.auxcell is None:
mydf.build()
kptijkl = _format_kpts(kpts)
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs, ) * 4
eri_mo = aft_ao2mo.general(mydf, mo_coeffs, kptijkl, compact=compact)
eri_mo += df_ao2mo.general(mydf, mo_coeffs, kptijkl, compact=compact)
return eri_mo
def general(mydf, mo_coeffs, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_general_compact', True)):
if mydf._cderi is None:
mydf.build()
kptijkl = _format_kpts(kpts)
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
eri_mo = aft_ao2mo.general(mydf, mo_coeffs, kptijkl, compact=compact)
eri_mo += df_ao2mo.general(mydf, mo_coeffs, kptijkl, compact=compact)
return eri_mo
def general(mydf, mo_coeffs, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_general_compact', True)):
if mydf._cderi is None:
mydf.build()
kptijkl = _format_kpts(kpts)
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
eri_mo = aft_ao2mo.general(mydf, mo_coeffs, kptijkl, compact=compact)
eri_mo += df_ao2mo.general(mydf, mo_coeffs, kptijkl, compact=compact)
return eri_mo
def ao2mo(mydf, mo_coeffs, kpts):
"""
For ctf, this function needs to be used with caution,
this function calls read on j3c twice, if other process does not explicitly perform ao2mo transformation, j3c needs to be read twice
eg,
if rank==0:
eri = mydf.ao2mo(mo_coeffs, kpts)
else:
mydf.j3c.read([])
mydf.j3c.read([])
"""
if mydf.j3c is None: mydf.build()
log = Logger(mydf.stdout, mydf.verbose)
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, np.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
if not _iskconserv(cell, kptijkl):
log.warn('df_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return np.zeros([mo.shape[1] for mo in mo_coeffs])
ijid, ijdagger = get_member(kpti, kptj, mydf.kptij_lst)
klid, kldagger = get_member(kptk, kptl, mydf.kptij_lst)
aux_idx = np.arange(mydf.j3c.size).reshape(mydf.j3c.shape)
nao, naux = mydf.j3c.shape[1], mydf.j3c.shape[-1]
ijid = aux_idx[ijid].ravel()
klid = aux_idx[klid].ravel()
ijL = mydf.j3c.read(ijid).reshape(nao,nao,naux)
if ijdagger:
ijL = ijL.transpose(1,0,2).conj()
klL = mydf.j3c.read(klid).reshape(nao,nao,naux)
if kldagger:
klL = klL.transpose(1,0,2).conj()
pvL = np.dot(mo_coeffs[0].conj().T, ijL.transpose(1,0,2))
pqL = np.dot(mo_coeffs[1].T, pvL).transpose(1,0,2)
pvL = ijL = None
rvL = np.dot(mo_coeffs[2].conj().T, klL.transpose(1,0,2))
rLs = np.dot(mo_coeffs[3].T, rvL).transpose(1,2,0)
rvL = klL = None
eri = np.dot(pqL,rLs)
return eri
def get_eri(mydf, kpts=None):
"""
For ctf, this function needs to be used with caution,
this function calls read on j3c twice, if other process does not explicitly call this func, j3c still needs to be read twice
eg,
if rank==0:
eri = mydf.get_eri(kpts)
else:
mydf.j3c.read([])
mydf.j3c.read([])
"""
if mydf.j3c is None: mydf.build()
log = Logger(mydf.stdout, mydf.verbose)
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if not _iskconserv(cell, kptijkl):
log.warn('df_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return np.zeros([mo.shape[1] for mo in mo_coeffs])
ijid, ijdagger = get_member(kpti, kptj, mydf.kptij_lst)
klid, kldagger = get_member(kptk, kptl, mydf.kptij_lst)
aux_idx = np.arange(mydf.j3c.size).reshape(mydf.j3c.shape)
nao, naux = mydf.j3c.shape[1], mydf.j3c.shape[-1]
ijid = aux_idx[ijid].ravel()
klid = aux_idx[klid].ravel()
ijL = mydf.j3c.read(ijid).reshape(nao,nao,naux)
if ijdagger:
ijL = ijL.transpose(1,0,2).conj()
klL = mydf.j3c.read(klid).reshape(nao,nao,naux)
if kldagger:
klL = klL.transpose(1,0,2).conj()
eri = np.dot(ijL,klL.transpose(0,2,1))
return eri
def get_eri(mydf, kpts=None, compact=True):
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
nao = cell.nao_nr()
nao_pair = nao * (nao+1) // 2
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .8)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL:
coulG = mydf.weighted_coulG(kptj-kpti, False, mydf.gs)
eriR = numpy.zeros((nao_pair,nao_pair))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], max_memory=max_memory,
aosym='s2'):
vG = numpy.sqrt(coulG[p0:p1])
pqkR *= vG
pqkI *= vG
lib.ddot(pqkR, pqkR.T, 1, eriR, 1)
lib.ddot(pqkI, pqkI.T, 1, eriR, 1)
pqkR = pqkI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2,-1)
return eriR
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
# complex integrals, N^4 elements
elif (abs(kpti-kptl).sum() < KPT_DIFF_TOL) and (abs(kptj-kptk).sum() < KPT_DIFF_TOL):
coulG = mydf.weighted_coulG(kptj-kpti, False, mydf.gs)
eriR = numpy.zeros((nao**2,nao**2))
eriI = numpy.zeros((nao**2,nao**2))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], max_memory=max_memory):
vG = numpy.sqrt(coulG[p0:p1])
pqkR *= vG
pqkI *= vG
# rho_pq(G+k_pq) * conj(rho_rs(G-k_rs))
zdotNC(pqkR, pqkI, pqkR.T, pqkI.T, 1, eriR, eriI, 1)
pqkR = pqkI = None
pqkR = pqkI = coulG = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
# rho_rs(-G+k_rs) = conj(transpose(rho_sr(G+k_sr), (0,2,1)))
eri = lib.transpose((eriR+eriI*1j).reshape(-1,nao,nao), axes=(0,2,1))
return eri.reshape(nao**2,-1)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
coulG = mydf.weighted_coulG(kptj-kpti, False, mydf.gs)
eriR = numpy.zeros((nao**2,nao**2))
eriI = numpy.zeros((nao**2,nao**2))
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mydf.gs, kptijkl[:2], max_memory=max_memory*.5),
mydf.pw_loop(mydf.gs,-kptijkl[2:], max_memory=max_memory*.5)):
pqkR *= coulG[p0:p1]
pqkI *= coulG[p0:p1]
# rho'_rs(G-k_rs) = conj(rho_rs(-G+k_rs))
# = conj(rho_rs(-G+k_rs) - d_{k_rs:Q,rs} * Q(-G+k_rs))
# = rho_rs(G-k_rs) - conj(d_{k_rs:Q,rs}) * Q(G-k_rs)
# rho_pq(G+k_pq) * conj(rho'_rs(G-k_rs))
zdotNC(pqkR, pqkI, rskR.T, rskI.T, 1, eriR, eriI, 1)
pqkR = pqkI = rskR = rskI = None
return (eriR+eriI*1j)
def get_eri(mydf, kpts=None, compact=True):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
nao = cell.nao_nr()
nao_pair = nao * (nao + 1) // 2
max_memory = max(2000, mydf.max_memory - lib.current_memory()[0] - nao ** 4 * 8 / 1e6)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL:
eriR = numpy.zeros((nao_pair, nao_pair))
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, True):
lib.ddot(LpqR.T, LpqR, 1, eriR, 1)
LpqR = LpqI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao ** 2, -1)
return eriR
elif (abs(kpti - kptk).sum() < KPT_DIFF_TOL) and (abs(kptj - kptl).sum() < KPT_DIFF_TOL):
eriR = numpy.zeros((nao * nao, nao * nao))
eriI = numpy.zeros((nao * nao, nao * nao))
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNN(LpqR.T, LpqI.T, LpqR, LpqI, 1, eriR, eriI, 1)
LpqR = LpqI = None
return eriR + eriI * 1j
####################
# (kpt) i == j == k == l != 0
#
# (kpt) i == l && j == k && i != j && j != k =>
# both vbar and ovlp are zero. It corresponds to the exchange integral.
#
# complex integrals, N^4 elements
elif (abs(kpti - kptl).sum() < KPT_DIFF_TOL) and (abs(kptj - kptk).sum() < KPT_DIFF_TOL):
eriR = numpy.zeros((nao * nao, nao * nao))
eriI = numpy.zeros((nao * nao, nao * nao))
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNC(LpqR.T, LpqI.T, LpqR, LpqI, 1, eriR, eriI, 1)
LpqR = LpqI = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
eri = lib.transpose((eriR + eriI * 1j).reshape(-1, nao, nao), axes=(0, 2, 1))
return eri.reshape(nao ** 2, -1)
####################
# aosym = s1, complex integrals
#
# kpti == kptj => kptl == kptk
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1.
#
else:
eriR = numpy.zeros((nao * nao, nao * nao))
eriI = numpy.zeros((nao * nao, nao * nao))
for (LpqR, LpqI), (LrsR, LrsI) in lib.izip(
mydf.sr_loop(kptijkl[:2], max_memory, False), mydf.sr_loop(kptijkl[2:], max_memory, False)
):
zdotNN(LpqR.T, LpqI.T, LrsR, LrsI, 1, eriR, eriI, 1)
LpqR = LpqI = LrsR = LrsI = None
return eriR + eriI * 1j
def get_eri(mydf, kpts=None, compact=True):
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
q = kptj - kpti
coulG = mydf.weighted_coulG(q, False, mydf.gs)
nao = cell.nao_nr()
nao_pair = nao * (nao + 1) // 2
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .8)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl):
eriR = numpy.zeros((nao_pair, nao_pair))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], q, max_memory=max_memory,
aosym='s2'):
vG = numpy.sqrt(coulG[p0:p1])
pqkR *= vG
pqkI *= vG
lib.ddot(pqkR, pqkR.T, 1, eriR, 1)
lib.ddot(pqkI, pqkI.T, 1, eriR, 1)
pqkR = pqkI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2, -1)
return eriR
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
# complex integrals, N^4 elements
elif is_zero(kpti - kptl) and is_zero(kptj - kptk):
eriR = numpy.zeros((nao**2, nao**2))
eriI = numpy.zeros((nao**2, nao**2))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], q, max_memory=max_memory):
vG = numpy.sqrt(coulG[p0:p1])
pqkR *= vG
pqkI *= vG
# rho_pq(G+k_pq) * conj(rho_rs(G-k_rs))
zdotNC(pqkR, pqkI, pqkR.T, pqkI.T, 1, eriR, eriI, 1)
pqkR = pqkI = None
pqkR = pqkI = coulG = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
# rho_rs(-G+k_rs) = conj(transpose(rho_sr(G+k_sr), (0,2,1)))
eri = lib.transpose((eriR + eriI * 1j).reshape(-1, nao, nao),
axes=(0, 2, 1))
return eri.reshape(nao**2, -1)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
eriR = numpy.zeros((nao**2, nao**2))
eriI = numpy.zeros((nao**2, nao**2))
# rho_rs(-G-k) = rho_rs(conj(G+k)) = conj(rho_sr(G+k))
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mydf.gs, kptijkl[:2], q, max_memory=max_memory*.5),
mydf.pw_loop(mydf.gs,-kptijkl[2:], q, max_memory=max_memory*.5)):
pqkR *= coulG[p0:p1]
pqkI *= coulG[p0:p1]
# rho_pq(G+k_pq) * conj(rho_sr(G+k_pq))
zdotNC(pqkR, pqkI, rskR.T, rskI.T, 1, eriR, eriI, 1)
pqkR = pqkI = rskR = rskI = None
return (eriR + eriI * 1j)
def general(mydf, mo_coeffs, kpts=None, compact=True):
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs, ) * 4
q = kptj - kpti
coulG = mydf.weighted_coulG(q, False, mydf.gs)
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .5)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl) and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0],
mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2],
mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair, nkl_pair))
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2])
and iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
ijR = ijI = klR = klI = buf = None
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], q, max_memory=max_memory,
aosym='s2'):
vG = numpy.sqrt(coulG[p0:p1])
pqkR *= vG
pqkI *= vG
buf = lib.transpose(pqkR, out=buf)
ijR, klR = _dtrans(buf, ijR, ijmosym, moij, ijslice, buf, klR,
klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR, 1, eri_mo, 1)
buf = lib.transpose(pqkI, out=buf)
ijI, klI = _dtrans(buf, ijI, ijmosym, moij, ijslice, buf, klI,
klmosym, mokl, klslice, sym)
lib.ddot(ijI.T, klI, 1, eri_mo, 1)
pqkR = pqkI = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif is_zero(kpti - kptl) and is_zero(kptj - kptk):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair, nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3])
and iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
zij = zlk = buf = None
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], q, max_memory=max_memory):
buf = lib.transpose(pqkR + pqkI * 1j, out=buf)
buf *= numpy.sqrt(coulG[p0:p1]).reshape(-1, 1)
zij, zlk = _ztrans(buf, zij, moij, ijslice, buf, zlk, molk,
lkslice, sym)
lib.dot(zij.T, zlk.conj(), 1, eri_mo, 1)
pqkR = pqkI = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1, nmol, nmok), axes=(0, 2, 1))
return eri_mo.reshape(nij_pair, nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair, nkl_pair), dtype=numpy.complex)
tao = []
ao_loc = None
zij = zkl = buf = None
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mydf.gs, kptijkl[:2], q, max_memory=max_memory*.5),
mydf.pw_loop(mydf.gs,-kptijkl[2:], q, max_memory=max_memory*.5)):
buf = lib.transpose(pqkR + pqkI * 1j, out=buf)
zij = _ao2mo.r_e2(buf, moij, ijslice, tao, ao_loc, out=zij)
buf = lib.transpose(rskR - rskI * 1j, out=buf)
zkl = _ao2mo.r_e2(buf, mokl, klslice, tao, ao_loc, out=zkl)
zij *= coulG[p0:p1].reshape(-1, 1)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
pqkR = pqkI = rskR = rskI = None
return eri_mo
def general(mydf, mo_coeffs, kpts=None, compact=True):
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .5)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair,nkl_pair))
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
coulG = mydf.weighted_coulG(kptj-kpti, False, mydf.gs)
ijR = ijI = klR = klI = buf = None
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], max_memory=max_memory,
aosym='s2'):
vG = numpy.sqrt(coulG[p0:p1])
pqkR *= vG
pqkI *= vG
buf = lib.transpose(pqkR, out=buf)
ijR, klR = _dtrans(buf, ijR, ijmosym, moij, ijslice,
buf, klR, klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR, 1, eri_mo, 1)
buf = lib.transpose(pqkI, out=buf)
ijI, klI = _dtrans(buf, ijI, ijmosym, moij, ijslice,
buf, klI, klmosym, mokl, klslice, sym)
lib.ddot(ijI.T, klI, 1, eri_mo, 1)
pqkR = pqkI = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif (abs(kpti-kptl).sum() < KPT_DIFF_TOL) and (abs(kptj-kptk).sum() < KPT_DIFF_TOL):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair,nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
coulG = mydf.weighted_coulG(kptj-kpti, False, mydf.gs)
zij = zlk = buf = None
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mydf.gs, kptijkl[:2], max_memory=max_memory):
buf = lib.transpose(pqkR+pqkI*1j, out=buf)
buf *= numpy.sqrt(coulG[p0:p1]).reshape(-1,1)
zij, zlk = _ztrans(buf, zij, moij, ijslice,
buf, zlk, molk, lkslice, sym)
lib.dot(zij.T, zlk.conj(), 1, eri_mo, 1)
pqkR = pqkI = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1,nmol,nmok), axes=(0,2,1))
return eri_mo.reshape(nij_pair,nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
tao = []
ao_loc = None
coulG = mydf.weighted_coulG(kptj-kpti, False, mydf.gs)
zij = zkl = buf = None
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mydf.gs, kptijkl[:2], max_memory=max_memory*.5),
mydf.pw_loop(mydf.gs,-kptijkl[2:], max_memory=max_memory*.5)):
buf = lib.transpose(pqkR+pqkI*1j, out=buf)
zij = _ao2mo.r_e2(buf, moij, ijslice, tao, ao_loc, out=zij)
buf = lib.transpose(rskR-rskI*1j, out=buf)
zkl = _ao2mo.r_e2(buf, mokl, klslice, tao, ao_loc, out=zkl)
zij *= coulG[p0:p1].reshape(-1,1)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
pqkR = pqkI = rskR = rskI = None
return eri_mo
def get_eri(mydf, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_get_eri_compact', True)):
cell = mydf.cell
nao = cell.nao_nr()
kptijkl = _format_kpts(kpts)
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'aft_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros((nao,nao,nao,nao))
kpti, kptj, kptk, kptl = kptijkl
q = kptj - kpti
mesh = mydf.mesh
coulG = mydf.weighted_coulG(q, False, mesh)
nao_pair = nao * (nao+1) // 2
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .8)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl):
eriR = numpy.zeros((nao_pair,nao_pair))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory,
aosym='s2'):
lib.ddot(pqkR*coulG[p0:p1], pqkR.T, 1, eriR, 1)
lib.ddot(pqkI*coulG[p0:p1], pqkI.T, 1, eriR, 1)
pqkR = pqkI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2,-1)
return eriR
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
# complex integrals, N^4 elements
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
eriR = numpy.zeros((nao**2,nao**2))
eriI = numpy.zeros((nao**2,nao**2))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory):
# rho_pq(G+k_pq) * conj(rho_rs(G-k_rs))
zdotNC(pqkR*coulG[p0:p1], pqkI*coulG[p0:p1], pqkR.T, pqkI.T,
1, eriR, eriI, 1)
pqkR = pqkI = None
pqkR = pqkI = coulG = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
# rho_rs(-G+k_rs) = conj(transpose(rho_sr(G+k_sr), (0,2,1)))
eri = lib.transpose((eriR+eriI*1j).reshape(-1,nao,nao), axes=(0,2,1))
return eri.reshape(nao**2,-1)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
eriR = numpy.zeros((nao**2,nao**2))
eriI = numpy.zeros((nao**2,nao**2))
#
# (pq|rs) = \sum_G 4\pi rho_pq rho_rs / |G+k_{pq}|^2
# rho_pq = 1/N \sum_{Tp,Tq} \int exp(-i(G+k_{pq})*r) p(r-Tp) q(r-Tq) dr
# = \sum_{Tq} exp(i k_q*Tq) \int exp(-i(G+k_{pq})*r) p(r) q(r-Tq) dr
# Note the k-point wrap-around for rho_rs, which leads to G+k_{pq} in FT
# rho_rs = 1/N \sum_{Tr,Ts} \int exp( i(G+k_{pq})*r) r(r-Tr) s(r-Ts) dr
# = \sum_{Ts} exp(i k_s*Ts) \int exp( i(G+k_{pq})*r) r(r) s(r-Ts) dr
# rho_pq can be directly evaluated by AFT (function pw_loop)
# rho_pq = pw_loop(k_q, G+k_{pq})
# Assuming r(r) and s(r) are real functions, rho_rs is evaluated
# rho_rs = 1/N \sum_{Tr,Ts} \int exp( i(G+k_{pq})*r) r(r-Tr) s(r-Ts) dr
# = conj(\sum_{Ts} exp(-i k_s*Ts) \int exp(-i(G+k_{pq})*r) r(r) s(r-Ts) dr)
# = conj( pw_loop(-k_s, G+k_{pq}) )
#
# TODO: For complex AO function r(r) and s(r), pw_loop function needs to be
# extended to include Gv vector in the arguments
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory*.5),
mydf.pw_loop(mesh,-kptijkl[2:], q, max_memory=max_memory*.5)):
pqkR *= coulG[p0:p1]
pqkI *= coulG[p0:p1]
zdotNC(pqkR, pqkI, rskR.T, rskI.T, 1, eriR, eriI, 1)
pqkR = pqkI = rskR = rskI = None
return (eriR+eriI*1j)
def get_eri(mydf, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_get_eri_compact', True)):
cell = mydf.cell
nao = cell.nao_nr()
kptijkl = _format_kpts(kpts)
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'aft_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros((nao,nao,nao,nao))
kpti, kptj, kptk, kptl = kptijkl
q = kptj - kpti
mesh = mydf.mesh
coulG = mydf.weighted_coulG(q, False, mesh)
nao_pair = nao * (nao+1) // 2
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .8)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl):
eriR = numpy.zeros((nao_pair,nao_pair))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory,
aosym='s2'):
lib.ddot(pqkR*coulG[p0:p1], pqkR.T, 1, eriR, 1)
lib.ddot(pqkI*coulG[p0:p1], pqkI.T, 1, eriR, 1)
pqkR = pqkI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2,-1)
return eriR
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
# complex integrals, N^4 elements
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
eriR = numpy.zeros((nao**2,nao**2))
eriI = numpy.zeros((nao**2,nao**2))
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory):
# rho_pq(G+k_pq) * conj(rho_rs(G-k_rs))
zdotNC(pqkR*coulG[p0:p1], pqkI*coulG[p0:p1], pqkR.T, pqkI.T,
1, eriR, eriI, 1)
pqkR = pqkI = None
pqkR = pqkI = coulG = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
# rho_rs(-G+k_rs) = conj(transpose(rho_sr(G+k_sr), (0,2,1)))
eri = lib.transpose((eriR+eriI*1j).reshape(-1,nao,nao), axes=(0,2,1))
return eri.reshape(nao**2,-1)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
eriR = numpy.zeros((nao**2,nao**2))
eriI = numpy.zeros((nao**2,nao**2))
#
# (pq|rs) = \sum_G 4\pi rho_pq rho_rs / |G+k_{pq}|^2
# rho_pq = 1/N \sum_{Tp,Tq} \int exp(-i(G+k_{pq})*r) p(r-Tp) q(r-Tq) dr
# = \sum_{Tq} exp(i k_q*Tq) \int exp(-i(G+k_{pq})*r) p(r) q(r-Tq) dr
# Note the k-point wrap-around for rho_rs, which leads to G+k_{pq} in FT
# rho_rs = 1/N \sum_{Tr,Ts} \int exp( i(G+k_{pq})*r) r(r-Tr) s(r-Ts) dr
# = \sum_{Ts} exp(i k_s*Ts) \int exp( i(G+k_{pq})*r) r(r) s(r-Ts) dr
# rho_pq can be directly evaluated by AFT (function pw_loop)
# rho_pq = pw_loop(k_q, G+k_{pq})
# Assuming r(r) and s(r) are real functions, rho_rs is evaluated
# rho_rs = 1/N \sum_{Tr,Ts} \int exp( i(G+k_{pq})*r) r(r-Tr) s(r-Ts) dr
# = conj(\sum_{Ts} exp(-i k_s*Ts) \int exp(-i(G+k_{pq})*r) r(r) s(r-Ts) dr)
# = conj( pw_loop(-k_s, G+k_{pq}) )
#
# TODO: For complex AO function r(r) and s(r), pw_loop function needs to be
# extended to include Gv vector in the arguments
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory*.5),
mydf.pw_loop(mesh,-kptijkl[2:], q, max_memory=max_memory*.5)):
pqkR *= coulG[p0:p1]
pqkI *= coulG[p0:p1]
zdotNC(pqkR, pqkI, rskR.T, rskI.T, 1, eriR, eriI, 1)
pqkR = pqkI = rskR = rskI = None
return (eriR+eriI*1j)
def general(mydf, mo_coeffs, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_general_compact', True)):
warn_pbc2d_eri(mydf)
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'aft_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros([mo.shape[1] for mo in mo_coeffs])
q = kptj - kpti
mesh = mydf.mesh
coulG = mydf.weighted_coulG(q, False, mesh)
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .5)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl) and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair,nkl_pair))
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
ijR = ijI = klR = klI = buf = None
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory,
aosym='s2'):
buf = lib.transpose(pqkR, out=buf)
ijR, klR = _dtrans(buf, ijR, ijmosym, moij, ijslice,
buf, klR, klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR*coulG[p0:p1,None], 1, eri_mo, 1)
buf = lib.transpose(pqkI, out=buf)
ijI, klI = _dtrans(buf, ijI, ijmosym, moij, ijslice,
buf, klI, klmosym, mokl, klslice, sym)
lib.ddot(ijI.T, klI*coulG[p0:p1,None], 1, eri_mo, 1)
pqkR = pqkI = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair,nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
zij = zlk = buf = None
for pqkR, pqkI, p0, p1 \
in mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory):
buf = lib.transpose(pqkR+pqkI*1j, out=buf)
zij, zlk = _ztrans(buf, zij, moij, ijslice,
buf, zlk, molk, lkslice, sym)
lib.dot(zij.T, zlk.conj()*coulG[p0:p1,None], 1, eri_mo, 1)
pqkR = pqkI = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1,nmol,nmok), axes=(0,2,1))
return eri_mo.reshape(nij_pair,nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
tao = []
ao_loc = None
zij = zkl = buf = None
for (pqkR, pqkI, p0, p1), (rskR, rskI, q0, q1) in \
lib.izip(mydf.pw_loop(mesh, kptijkl[:2], q, max_memory=max_memory*.5),
mydf.pw_loop(mesh,-kptijkl[2:], q, max_memory=max_memory*.5)):
buf = lib.transpose(pqkR+pqkI*1j, out=buf)
zij = _ao2mo.r_e2(buf, moij, ijslice, tao, ao_loc, out=zij)
buf = lib.transpose(rskR-rskI*1j, out=buf)
zkl = _ao2mo.r_e2(buf, mokl, klslice, tao, ao_loc, out=zkl)
zij *= coulG[p0:p1,None]
lib.dot(zij.T, zkl, 1, eri_mo, 1)
pqkR = pqkI = rskR = rskI = None
return eri_mo
def general(mydf, mo_coeffs, kpts=None, compact=True):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
eri_mo = pwdf_ao2mo.general(mydf, mo_coeffs, kptijkl, compact)
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .5)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
if sym:
eri_mo *= .5 # because we'll do +cc later
ijR = klR = None
for LpqR, LpqI, j3cR, j3cI in mydf.sr_loop(kptijkl[:2], max_memory, True):
ijR, klR = _dtrans(LpqR, ijR, ijmosym, moij, ijslice,
j3cR, klR, klmosym, mokl, klslice, False)
lib.ddot(ijR.T, klR, 1, eri_mo, 1)
if not sym:
ijR, klR = _dtrans(j3cR, ijR, ijmosym, moij, ijslice,
LpqR, klR, klmosym, mokl, klslice, False)
lib.ddot(ijR.T, klR, 1, eri_mo, 1)
LpqR = LpqI = j3cR = j3cI = None
if sym:
eri_mo = lib.transpose_sum(eri_mo, inplace=True)
return eri_mo
####################
# (kpt) i == j == k == l != 0
#
# (kpt) i == l && j == k && i != j && j != k =>
# both vbar and ovlp are zero. It corresponds to the exchange integral.
#
# complex integrals, N^4 elements
elif (abs(kpti-kptl).sum() < KPT_DIFF_TOL) and (abs(kptj-kptk).sum() < KPT_DIFF_TOL):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_lk = numpy.zeros((nij_pair,nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
zij = zlk = buf = None
for LpqR, LpqI, j3cR, j3cI in mydf.sr_loop(kptijkl[:2], max_memory, False):
bufL = LpqR+LpqI*1j
bufj = j3cR+j3cI*1j
zij, zlk = _ztrans(bufL, zij, moij, ijslice,
bufj, zlk, molk, lkslice, False)
lib.dot(zij.T, zlk.conj(), 1, eri_lk, 1)
if not sym:
zij, zlk = _ztrans(bufj, zij, moij, ijslice,
bufL, zlk, molk, lkslice, False)
lib.dot(zij.T, zlk.conj(), 1, eri_lk, 1)
LpqR = LpqI = j3cR = j3cI = bufL = bufj = None
if sym:
eri_lk += lib.transpose(eri_lk).conj()
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_lk = lib.transpose(eri_lk.reshape(-1,nmol,nmok), axes=(0,2,1))
eri_mo += eri_lk.reshape(nij_pair,nlk_pair)
return eri_mo
####################
# aosym = s1, complex integrals
#
# kpti == kptj => kptl == kptk
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1.
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
max_memory *= .5
zij = zkl = None
for (LpqR, LpqI, jpqR, jpqI), (LrsR, LrsI, jrsR, jrsI) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False),
mydf.sr_loop(kptijkl[2:], max_memory, False)):
zij, zkl = _ztrans(LpqR+LpqI*1j, zij, moij, ijslice,
jrsR+jrsI*1j, zkl, mokl, klslice, False)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
zij, zkl = _ztrans(jpqR+jpqI*1j, zij, moij, ijslice,
LrsR+LrsI*1j, zkl, mokl, klslice, False)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
LpqR = LpqI = jpqR = jpqI = LrsR = LrsI = jrsR = jrsI = None
return eri_mo
def general(mydf, mo_coeffs, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_general_compact', True)):
warn_pbc2d_eri(mydf)
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'df_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros([mo.shape[1] for mo in mo_coeffs])
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]))
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl) and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair,nkl_pair))
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
ijR = klR = None
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, True):
ijR, klR = _dtrans(LpqR, ijR, ijmosym, moij, ijslice,
LpqR, klR, klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR, sign, eri_mo, 1)
LpqR = LpqI = None
return eri_mo
elif is_zero(kpti-kptk) and is_zero(kptj-kptl):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
zij = zkl = None
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR+LpqI*1j
zij, zkl = _ztrans(buf, zij, moij, ijslice,
buf, zkl, mokl, klslice, sym)
lib.dot(zij.T, zkl, sign, eri_mo, 1)
LpqR = LpqI = buf = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair,nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
zij = zlk = None
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR+LpqI*1j
zij, zlk = _ztrans(buf, zij, moij, ijslice,
buf, zlk, molk, lkslice, sym)
lib.dot(zij.T, zlk.conj(), sign, eri_mo, 1)
LpqR = LpqI = buf = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1,nmol,nmok), axes=(0,2,1))
return eri_mo.reshape(nij_pair,nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
nao = mo_coeffs[0].shape[0]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
blksize = int(min(max_memory*.3e6/16/nij_pair,
max_memory*.3e6/16/nkl_pair,
max_memory*.3e6/16/nao**2))
zij = zkl = None
for (LpqR, LpqI, sign), (LrsR, LrsI, sign1) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False, blksize),
mydf.sr_loop(kptijkl[2:], max_memory, False, blksize)):
zij, zkl = _ztrans(LpqR+LpqI*1j, zij, moij, ijslice,
LrsR+LrsI*1j, zkl, mokl, klslice, False)
lib.dot(zij.T, zkl, sign, eri_mo, 1)
LpqR = LpqI = LrsR = LrsI = None
return eri_mo
def get_eri(mydf, kpts=None, compact=True):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
nao = cell.nao_nr()
nao_pair = nao * (nao+1) // 2
max_memory = max(2000, mydf.max_memory-lib.current_memory()[0]-nao**4*8/1e6)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL:
eriR = numpy.zeros((nao_pair,nao_pair))
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, True):
lib.ddot(LpqR.T, LpqR, 1, eriR, 1)
LpqR = LpqI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2,-1)
return eriR
elif (abs(kpti-kptk).sum() < KPT_DIFF_TOL) and (abs(kptj-kptl).sum() < KPT_DIFF_TOL):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNN(LpqR.T, LpqI.T, LpqR, LpqI, 1, eriR, eriI, 1)
LpqR = LpqI = None
return eriR + eriI*1j
####################
# (kpt) i == j == k == l != 0
#
# (kpt) i == l && j == k && i != j && j != k =>
# both vbar and ovlp are zero. It corresponds to the exchange integral.
#
# complex integrals, N^4 elements
elif (abs(kpti-kptl).sum() < KPT_DIFF_TOL) and (abs(kptj-kptk).sum() < KPT_DIFF_TOL):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNC(LpqR.T, LpqI.T, LpqR, LpqI, 1, eriR, eriI, 1)
LpqR = LpqI = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
eri = lib.transpose((eriR+eriI*1j).reshape(-1,nao,nao), axes=(0,2,1))
return eri.reshape(nao**2,-1)
####################
# aosym = s1, complex integrals
#
# kpti == kptj => kptl == kptk
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1.
#
else:
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for (LpqR, LpqI), (LrsR, LrsI) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False),
mydf.sr_loop(kptijkl[2:], max_memory, False)):
zdotNN(LpqR.T, LpqI.T, LrsR, LrsI, 1, eriR, eriI, 1)
LpqR = LpqI = LrsR = LrsI = None
return eriR + eriI*1j
def general(mydf, mo_coeffs, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_general_compact', True)):
warn_pbc2d_eri(mydf)
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'df_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros([mo.shape[1] for mo in mo_coeffs])
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]))
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl) and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair,nkl_pair))
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
ijR = klR = None
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, True):
ijR, klR = _dtrans(LpqR, ijR, ijmosym, moij, ijslice,
LpqR, klR, klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR, sign, eri_mo, 1)
LpqR = LpqI = None
return eri_mo
elif is_zero(kpti-kptk) and is_zero(kptj-kptl):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
zij = zkl = None
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR+LpqI*1j
zij, zkl = _ztrans(buf, zij, moij, ijslice,
buf, zkl, mokl, klslice, sym)
lib.dot(zij.T, zkl, sign, eri_mo, 1)
LpqR = LpqI = buf = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair,nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
zij = zlk = None
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR+LpqI*1j
zij, zlk = _ztrans(buf, zij, moij, ijslice,
buf, zlk, molk, lkslice, sym)
lib.dot(zij.T, zlk.conj(), sign, eri_mo, 1)
LpqR = LpqI = buf = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1,nmol,nmok), axes=(0,2,1))
return eri_mo.reshape(nij_pair,nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
nao = mo_coeffs[0].shape[0]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
blksize = int(min(max_memory*.3e6/16/nij_pair,
max_memory*.3e6/16/nkl_pair,
max_memory*.3e6/16/nao**2))
zij = zkl = None
for (LpqR, LpqI, sign), (LrsR, LrsI, sign1) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False, blksize),
mydf.sr_loop(kptijkl[2:], max_memory, False, blksize)):
zij, zkl = _ztrans(LpqR+LpqI*1j, zij, moij, ijslice,
LrsR+LrsI*1j, zkl, mokl, klslice, False)
lib.dot(zij.T, zkl, sign, eri_mo, 1)
LpqR = LpqI = LrsR = LrsI = None
return eri_mo
def get_eri(mydf, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_get_eri_compact', True)):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
nao = cell.nao_nr()
kptijkl = _format_kpts(kpts)
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'df_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros((nao,nao,nao,nao))
kpti, kptj, kptk, kptl = kptijkl
nao_pair = nao * (nao+1) // 2
max_memory = max(2000, mydf.max_memory-lib.current_memory()[0]-nao**4*16/1e6)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl):
eriR = numpy.zeros((nao_pair,nao_pair))
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, True):
lib.ddot(LpqR.T, LpqR, sign, eriR, 1)
LpqR = LpqI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2,-1)
return eriR
elif is_zero(kpti-kptk) and is_zero(kptj-kptl):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNN(LpqR.T, LpqI.T, LpqR, LpqI, sign, eriR, eriI, 1)
LpqR = LpqI = None
return eriR + eriI*1j
####################
# (kpt) i == j == k == l != 0
#
# (kpt) i == l && j == k && i != j && j != k =>
# both vbar and ovlp are zero. It corresponds to the exchange integral.
#
# complex integrals, N^4 elements
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNC(LpqR.T, LpqI.T, LpqR, LpqI, sign, eriR, eriI, 1)
LpqR = LpqI = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
eri = lib.transpose((eriR+eriI*1j).reshape(-1,nao,nao), axes=(0,2,1))
return eri.reshape(nao**2,-1)
####################
# aosym = s1, complex integrals
#
# kpti == kptj => kptl == kptk
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1.
#
else:
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
blksize = int(max_memory*.4e6/16/nao**2)
for (LpqR, LpqI, sign), (LrsR, LrsI, sign1) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False, blksize),
mydf.sr_loop(kptijkl[2:], max_memory, False, blksize)):
zdotNN(LpqR.T, LpqI.T, LrsR, LrsI, sign, eriR, eriI, 1)
LpqR = LpqI = LrsR = LrsI = None
return eriR + eriI*1j
def general(mydf, mo_coeffs, kpts=None, compact=True):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * .5)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair,nkl_pair))
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
ijR = klR = None
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, True):
ijR, klR = _dtrans(LpqR, ijR, ijmosym, moij, ijslice,
LpqR, klR, klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR, 1, eri_mo, 1)
LpqR = LpqI = None
return eri_mo
elif (abs(kpti-kptk).sum() < KPT_DIFF_TOL) and (abs(kptj-kptl).sum() < KPT_DIFF_TOL):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[3]))
zij = zkl = None
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR+LpqI*1j
zij, zkl = _ztrans(buf, zij, moij, ijslice,
buf, zkl, mokl, klslice, sym)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
LpqR = LpqI = buf = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif (abs(kpti-kptl).sum() < KPT_DIFF_TOL) and (abs(kptj-kptk).sum() < KPT_DIFF_TOL):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair,nlk_pair), dtype=numpy.complex)
sym = (iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and
iden_coeffs(mo_coeffs[1], mo_coeffs[2]))
zij = zlk = None
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR+LpqI*1j
zij, zlk = _ztrans(buf, zij, moij, ijslice,
buf, zlk, molk, lkslice, sym)
lib.dot(zij.T, zlk.conj(), 1, eri_mo, 1)
LpqR = LpqI = buf = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1,nmol,nmok), axes=(0,2,1))
return eri_mo.reshape(nij_pair,nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair,nkl_pair), dtype=numpy.complex)
zij = zkl = None
for (LpqR, LpqI), (LrsR, LrsI) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False),
mydf.sr_loop(kptijkl[2:], max_memory, False)):
zij, zkl = _ztrans(LpqR+LpqI*1j, zij, moij, ijslice,
LrsR+LrsI*1j, zkl, mokl, klslice, False)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
LpqR = LpqI = LrsR = LrsI = None
return eri_mo
def general(mydf, mo_coeffs, kpts=None, compact=True):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
if isinstance(mo_coeffs, numpy.ndarray) and mo_coeffs.ndim == 2:
mo_coeffs = (mo_coeffs,) * 4
all_real = not any(numpy.iscomplexobj(mo) for mo in mo_coeffs)
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0]) * 0.5)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL and all_real:
ijmosym, nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1], compact)
klmosym, nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3], compact)
eri_mo = numpy.zeros((nij_pair, nkl_pair))
sym = iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and iden_coeffs(mo_coeffs[1], mo_coeffs[3])
ijR = klR = None
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, True):
ijR, klR = _dtrans(LpqR, ijR, ijmosym, moij, ijslice, LpqR, klR, klmosym, mokl, klslice, sym)
lib.ddot(ijR.T, klR, 1, eri_mo, 1)
LpqR = LpqI = None
return eri_mo
elif (abs(kpti - kptk).sum() < KPT_DIFF_TOL) and (abs(kptj - kptl).sum() < KPT_DIFF_TOL):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair, nkl_pair), dtype=numpy.complex)
sym = iden_coeffs(mo_coeffs[0], mo_coeffs[2]) and iden_coeffs(mo_coeffs[1], mo_coeffs[3])
zij = zkl = None
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR + LpqI * 1j
zij, zkl = _ztrans(buf, zij, moij, ijslice, buf, zkl, mokl, klslice, sym)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
LpqR = LpqI = buf = None
return eri_mo
####################
# (kpt) i == j == k == l != 0
# (kpt) i == l && j == k && i != j && j != k =>
#
elif (abs(kpti - kptl).sum() < KPT_DIFF_TOL) and (abs(kptj - kptk).sum() < KPT_DIFF_TOL):
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nlk_pair, molk, lkslice = _conc_mos(mo_coeffs[3], mo_coeffs[2])[1:]
eri_mo = numpy.zeros((nij_pair, nlk_pair), dtype=numpy.complex)
sym = iden_coeffs(mo_coeffs[0], mo_coeffs[3]) and iden_coeffs(mo_coeffs[1], mo_coeffs[2])
zij = zlk = None
for LpqR, LpqI in mydf.sr_loop(kptijkl[:2], max_memory, False):
buf = LpqR + LpqI * 1j
zij, zlk = _ztrans(buf, zij, moij, ijslice, buf, zlk, molk, lkslice, sym)
lib.dot(zij.T, zlk.conj(), 1, eri_mo, 1)
LpqR = LpqI = buf = None
nmok = mo_coeffs[2].shape[1]
nmol = mo_coeffs[3].shape[1]
eri_mo = lib.transpose(eri_mo.reshape(-1, nmol, nmok), axes=(0, 2, 1))
return eri_mo.reshape(nij_pair, nlk_pair)
####################
# aosym = s1, complex integrals
#
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1. => kptl == kptk
#
else:
mo_coeffs = _mo_as_complex(mo_coeffs)
nij_pair, moij, ijslice = _conc_mos(mo_coeffs[0], mo_coeffs[1])[1:]
nkl_pair, mokl, klslice = _conc_mos(mo_coeffs[2], mo_coeffs[3])[1:]
eri_mo = numpy.zeros((nij_pair, nkl_pair), dtype=numpy.complex)
zij = zkl = None
for (LpqR, LpqI), (LrsR, LrsI) in lib.izip(
mydf.sr_loop(kptijkl[:2], max_memory, False), mydf.sr_loop(kptijkl[2:], max_memory, False)
):
zij, zkl = _ztrans(LpqR + LpqI * 1j, zij, moij, ijslice, LrsR + LrsI * 1j, zkl, mokl, klslice, False)
lib.dot(zij.T, zkl, 1, eri_mo, 1)
LpqR = LpqI = LrsR = LrsI = None
return eri_mo
def get_eri(mydf, kpts=None,
compact=getattr(__config__, 'pbc_df_ao2mo_get_eri_compact', True)):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
nao = cell.nao_nr()
kptijkl = _format_kpts(kpts)
if not _iskconserv(cell, kptijkl):
lib.logger.warn(cell, 'df_ao2mo: momentum conservation not found in '
'the given k-points %s', kptijkl)
return numpy.zeros((nao,nao,nao,nao))
kpti, kptj, kptk, kptl = kptijkl
nao_pair = nao * (nao+1) // 2
max_memory = max(2000, mydf.max_memory-lib.current_memory()[0]-nao**4*16/1e6)
####################
# gamma point, the integral is real and with s4 symmetry
if gamma_point(kptijkl):
eriR = numpy.zeros((nao_pair,nao_pair))
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, True):
lib.ddot(LpqR.T, LpqR, sign, eriR, 1)
LpqR = LpqI = None
if not compact:
eriR = ao2mo.restore(1, eriR, nao).reshape(nao**2,-1)
return eriR
elif is_zero(kpti-kptk) and is_zero(kptj-kptl):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNN(LpqR.T, LpqI.T, LpqR, LpqI, sign, eriR, eriI, 1)
LpqR = LpqI = None
return eriR + eriI*1j
####################
# (kpt) i == j == k == l != 0
#
# (kpt) i == l && j == k && i != j && j != k =>
# both vbar and ovlp are zero. It corresponds to the exchange integral.
#
# complex integrals, N^4 elements
elif is_zero(kpti-kptl) and is_zero(kptj-kptk):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI, sign in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNC(LpqR.T, LpqI.T, LpqR, LpqI, sign, eriR, eriI, 1)
LpqR = LpqI = None
# transpose(0,1,3,2) because
# j == k && i == l =>
# (L|ij).transpose(0,2,1).conj() = (L^*|ji) = (L^*|kl) => (M|kl)
eri = lib.transpose((eriR+eriI*1j).reshape(-1,nao,nao), axes=(0,2,1))
return eri.reshape(nao**2,-1)
####################
# aosym = s1, complex integrals
#
# kpti == kptj => kptl == kptk
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1.
#
else:
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
blksize = int(max_memory*.4e6/16/nao**2)
for (LpqR, LpqI, sign), (LrsR, LrsI, sign1) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False, blksize),
mydf.sr_loop(kptijkl[2:], max_memory, False, blksize)):
zdotNN(LpqR.T, LpqI.T, LrsR, LrsI, sign, eriR, eriI, 1)
LpqR = LpqI = LrsR = LrsI = None
return eriR + eriI*1j
def get_eri(mydf, kpts=None, compact=True):
if mydf._cderi is None:
mydf.build()
cell = mydf.cell
kptijkl = _format_kpts(kpts)
kpti, kptj, kptk, kptl = kptijkl
eri = pwdf_ao2mo.get_eri(mydf, kptijkl, compact=True)
nao = cell.nao_nr()
max_memory = max(2000, (mydf.max_memory - lib.current_memory()[0] - nao**4*8/1e6) * .8)
####################
# gamma point, the integral is real and with s4 symmetry
if abs(kptijkl).sum() < KPT_DIFF_TOL:
eri *= .5 # because we'll do +cc later
for LpqR, LpqI, j3cR, j3cI in mydf.sr_loop(kptijkl[:2], max_memory, True):
lib.ddot(j3cR.T, LpqR, 1, eri, 1)
LpqR = LpqI = j3cR = j3cI = None
eri = lib.transpose_sum(eri, inplace=True)
if not compact:
eri = ao2mo.restore(1, eri, nao).reshape(nao**2,-1)
return eri
####################
# (kpt) i == j == k == l != 0
#
# (kpt) i == l && j == k && i != j && j != k =>
# both vbar and ovlp are zero. It corresponds to the exchange integral.
#
# complex integrals, N^4 elements
elif (abs(kpti-kptl).sum() < KPT_DIFF_TOL) and (abs(kptj-kptk).sum() < KPT_DIFF_TOL):
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
for LpqR, LpqI, j3cR, j3cI in mydf.sr_loop(kptijkl[:2], max_memory, False):
zdotNC(j3cR.T, j3cI.T, LpqR, LpqI, 1, eriR, eriI, 1)
# eri == eri.transpose(3,2,1,0).conj()
# zdotNC(LpqR.T, LpqI.T, j3cR, j3cI, 1, eriR, eriI, 1)
LpqR = LpqI = j3cR = j3cI = None
# eri == eri.transpose(3,2,1,0).conj()
eriR = lib.transpose_sum(eriR, inplace=True)
buf = lib.transpose(eriI)
eriI -= buf
eriR = lib.transpose(eriR.reshape(-1,nao,nao), axes=(0,2,1), out=buf)
eri += eriR.reshape(eri.shape)
eriI = lib.transpose(eriI.reshape(-1,nao,nao), axes=(0,2,1), out=buf)
eri += eriI.reshape(eri.shape)*1j
return eri
####################
# aosym = s1, complex integrals
#
# kpti == kptj => kptl == kptk
# If kpti == kptj, (kptl-kptk)*a has to be multiples of 2pi because of the wave
# vector symmetry. k is a fraction of reciprocal basis, 0 < k/b < 1, by definition.
# So kptl/b - kptk/b must be -1 < k/b < 1.
#
else:
eriR = numpy.zeros((nao*nao,nao*nao))
eriI = numpy.zeros((nao*nao,nao*nao))
max_memory *= .5
for (LpqR, LpqI, jpqR, jpqI), (LrsR, LrsI, jrsR, jrsI) in \
lib.izip(mydf.sr_loop(kptijkl[:2], max_memory, False),
mydf.sr_loop(kptijkl[2:], max_memory, False)):
zdotNN(jpqR.T, jpqI.T, LrsR, LrsI, 1, eriR, eriI, 1)
zdotNN(LpqR.T, LpqI.T, jrsR, jrsI, 1, eriR, eriI, 1)
LpqR = LpqI = jpqR = jpqI = LrsR = LrsI = jrsR = jrsI = None
eri += eriR
eri += eriI*1j
return eri
