mirror of
https://github.com/triqs/dft_tools
synced 2024-06-25 22:52:20 +02:00
Merged lattice_gf_matsubara and lattice_gf_realfreq into single function
This commit is contained in:
Priyanka Seth
parent
cc3a9deaa8
commit
259fd64824
|
|
@ -1,67 +0,0 @@
|
|||
def lattice_gf(self, ik, mu, iw_or_w="iw", beta=40, broadening, mesh=None, with_Sigma=True, with_dc=True):
|
||||
"""Calculates the lattice Green function from the DFT hopping and the self energy at k-point number ik
|
||||
and chemical potential mu."""
|
||||
|
||||
ntoi = self.spin_names_to_ind[self.SO]
|
||||
spn = self.spin_block_names[self.SO]
|
||||
if (iw_or_w != "iw") and (iw_or_w != "w"):
|
||||
raise ValueError, "lattice_gf: implemented only for Re/Im frequency functions."
|
||||
|
||||
# Are we including Sigma?
|
||||
if with_Sigma:
|
||||
if with_dc: sigma_inc_dc = self.add_dc()
|
||||
Sigma_imp = getattr(self,"Sigma_imp_"+iw_or_w)
|
||||
if iw_or_w == "iw": beta = Sigma_imp[0].mesh.beta # override beta if Sigma_iw is present
|
||||
else:
|
||||
if (iw_or_w == "w") and (mesh is None):
|
||||
raise ValueError, "Give the mesh=(om_min,om_max,n_points) for the lattice GfReFreq."
|
||||
|
||||
# Check if G_upfold is present
|
||||
set_up_G_upfold = False # Assume not
|
||||
if not hasattr(self,"G_upfold_"+iw_or_w)):
|
||||
set_up_G_upfold = True # Need to create G_upfold_iw
|
||||
setattr(self,"G_upfold_"+iw_or_w,0) # Set temporarily to zero
|
||||
else: # Check that existing GF is consistent
|
||||
GFsize = [ gf.N1 for bname,gf in getattr(self,"G_upfold_"+iw_or_w)]
|
||||
unchangedsize = all( [ self.n_orbitals[ik,ntoi[spn[isp]]]==GFsize[isp]
|
||||
for isp in range(self.n_spin_blocks[self.SO]) ] )
|
||||
if not unchangedsize: set_up_G_upfold = True
|
||||
if (iw_or_w != "iw") and (self.G_upfold_iw.mesh.beta != beta): # additional check for ImFreq
|
||||
set_up_G_upfold = True
|
||||
G_upfold = getattr(self,"G_upfold_"+iw_or_w)
|
||||
|
||||
# Set up G_upfold
|
||||
if set_up_G_upfold:
|
||||
block_structure = [ range(self.n_orbitals[ik,ntoi[sp]]) for sp in spn ]
|
||||
gf_struct = [ (spn[isp], block_structure[isp]) for isp in range(self.n_spin_blocks[self.SO]) ]
|
||||
block_ind_list = [block for block,inner in gf_struct]
|
||||
if with_Sigma:
|
||||
glist = lambda : [ GfImFreq(indices=inner,mesh=Sigma_imp[0].mesh) for block,inner in gf_struct]
|
||||
else:
|
||||
if iw_or_w == "iw":
|
||||
glist = lambda : [ GfImFreq(indices=inner,beta=beta) for block,inner in gf_struct]
|
||||
elif iw_or_w == "w":
|
||||
glist = lambda : [ GfImFreq(indices=inner,window=(mesh[0],mesh[1]),n_points=mesh[2]) for block,inner in gf_struct]
|
||||
G_upfold = BlockGf(name_list = block_ind_list, block_list = glist(), make_copies = False)
|
||||
G_upfold.zero()
|
||||
|
||||
if iw_or_w == "iw":
|
||||
G_upfold << iOmega_n
|
||||
elif iw_or_w == "w":
|
||||
G_upfold << Omega + 1j*broadening
|
||||
|
||||
idmat = [numpy.identity(self.n_orbitals[ik,ntoi[sp]],numpy.complex_) for sp in spn]
|
||||
M = copy.deepcopy(idmat)
|
||||
for ibl in range(self.n_spin_blocks[self.SO]):
|
||||
ind = ntoi[spn[ibl]]
|
||||
n_orb = self.n_orbitals[ik,ind]
|
||||
M[ibl] = self.hopping[ik,ind,0:n_orb,0:n_orb] - (idmat[ibl]*mu) - (idmat[ibl] * self.h_field * (1-2*ibl))
|
||||
G_upfold -= M
|
||||
|
||||
if with_Sigma:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bname,gf in G_upfold: gf -= self.upfold(ik,icrsh,bname,sigma_inc_dc[icrsh][bname],gf)
|
||||
|
||||
G_upfold.invert()
|
||||
|
||||
return G_upfold
|
||||
|
|
@ -49,7 +49,7 @@ class SumkDFT:
|
|||
self.symmpar_data = symmpar_data
|
||||
self.bands_data = bands_data
|
||||
self.transp_data = transp_data
|
||||
self.G_upfold = None
|
||||
#self.G_latt_iw = None # DEBUG -- remove later
|
||||
self.h_field = h_field
|
||||
|
||||
# Read input from HDF:
|
||||
|
|
@ -128,7 +128,6 @@ class SumkDFT:
|
|||
if (len(things_to_read) != 0): mpi.report("Loading failed: No %s subgroup in HDF5!"%subgrp)
|
||||
subgroup_present = False
|
||||
value_read = False
|
||||
|
||||
del ar
|
||||
# now do the broadcasting:
|
||||
for it in things_to_read: setattr(self,it,mpi.bcast(getattr(self,it)))
|
||||
|
|
@ -163,7 +162,7 @@ class SumkDFT:
|
|||
try:
|
||||
list_to_return.append(ar[subgrp][it])
|
||||
except:
|
||||
raise ValueError, "%s not found, and so not loaded."%it
|
||||
raise ValueError, "load: %s not found, and so not loaded."%it
|
||||
del ar
|
||||
return list_to_return
|
||||
|
||||
|
|
@ -203,7 +202,7 @@ class SumkDFT:
|
|||
"""Local <-> Global rotation of a GF block.
|
||||
direction: 'toLocal' / 'toGlobal' """
|
||||
|
||||
assert ((direction == 'toLocal') or (direction == 'toGlobal')),"Give direction 'toLocal' or 'toGlobal' in rotloc!"
|
||||
assert ((direction == 'toLocal') or (direction == 'toGlobal')),"rotloc: Give direction 'toLocal' or 'toGlobal'."
|
||||
|
||||
gf_rotated = gf_to_rotate.copy()
|
||||
|
||||
|
|
@ -226,76 +225,99 @@ class SumkDFT:
|
|||
return gf_rotated
|
||||
|
||||
|
||||
def lattice_gf_matsubara(self,ik,mu,beta=40,with_Sigma=True):
|
||||
def lattice_gf(self, ik, mu, iw_or_w="iw", beta=40, broadening=None, mesh=None, with_Sigma=True, with_dc=True):
|
||||
"""Calculates the lattice Green function from the DFT hopping and the self energy at k-point number ik
|
||||
and chemical potential mu."""
|
||||
|
||||
ntoi = self.spin_names_to_ind[self.SO]
|
||||
spn = self.spin_block_names[self.SO]
|
||||
if (iw_or_w != "iw") and (iw_or_w != "w"): raise ValueError, "lattice_gf: Implemented only for Re/Im frequency functions."
|
||||
if not hasattr(self,"Sigma_imp_"+iw_or_w): with_Sigma = False
|
||||
if broadening is None:
|
||||
if mesh is None:
|
||||
broadening = 0.01
|
||||
else: # broadening = 2 * \Delta omega, where \Delta omega is the spacing of omega points
|
||||
broadening = 2.0 * ( (mesh[1]-mesh[0])/(mesh[2]-1) )
|
||||
|
||||
if not hasattr(self,"Sigma_imp"): with_Sigma = False
|
||||
|
||||
# Are we including Sigma?
|
||||
if with_Sigma:
|
||||
stmp = self.add_dc()
|
||||
beta = self.Sigma_imp[0].mesh.beta # override beta if Sigma is present
|
||||
if with_dc: sigma_minus_dc = self.add_dc(iw_or_w)
|
||||
Sigma_imp = getattr(self,"Sigma_imp_"+iw_or_w)
|
||||
if iw_or_w == "iw": beta = Sigma_imp[0].mesh.beta # override beta if Sigma_iw is present
|
||||
else:
|
||||
if (iw_or_w == "w") and (mesh is None):
|
||||
raise ValueError, "lattice_gf: Give the mesh=(om_min,om_max,n_points) for the lattice GfReFreq."
|
||||
|
||||
# Do we need to set up G_upfold?
|
||||
set_up_G_upfold = False # assume not
|
||||
if self.G_upfold is None: # yes if not G_upfold provided
|
||||
set_up_G_upfold = True
|
||||
else: # yes if inconsistencies present in existing G_upfold
|
||||
GFsize = [ gf.N1 for bname,gf in self.G_upfold]
|
||||
unchangedsize = all( [ self.n_orbitals[ik,ntoi[spn[isp]]] == GFsize[isp]
|
||||
for isp in range(self.n_spin_blocks[self.SO]) ] )
|
||||
if (not unchangedsize) or (self.G_upfold.mesh.beta != beta): set_up_G_upfold = True
|
||||
# Check if G_latt is present
|
||||
set_up_G_latt = False # Assume not
|
||||
if not hasattr(self,"G_latt_"+iw_or_w):
|
||||
set_up_G_latt = True # Need to create G_latt_(i)w
|
||||
else: # Check that existing GF is consistent
|
||||
G_latt = getattr(self,"G_latt_"+iw_or_w)
|
||||
GFsize = [ gf.N1 for bname,gf in G_latt]
|
||||
unchangedsize = all( [ self.n_orbitals[ik,ntoi[spn[isp]]]==GFsize[isp] for isp in range(self.n_spin_blocks[self.SO]) ] )
|
||||
if not unchangedsize: set_up_G_latt = True
|
||||
if (iw_or_w == "iw") and (self.G_latt_iw.mesh.beta != beta): set_up_G_latt = True # additional check for ImFreq
|
||||
|
||||
# Set up G_upfold
|
||||
if set_up_G_upfold:
|
||||
# Set up G_latt
|
||||
if set_up_G_latt:
|
||||
block_structure = [ range(self.n_orbitals[ik,ntoi[sp]]) for sp in spn ]
|
||||
gf_struct = [ (spn[isp], block_structure[isp]) for isp in range(self.n_spin_blocks[self.SO]) ]
|
||||
block_ind_list = [block for block,inner in gf_struct]
|
||||
if with_Sigma:
|
||||
glist = lambda : [ GfImFreq(indices = inner, mesh = self.Sigma_imp[0].mesh) for block,inner in gf_struct]
|
||||
else:
|
||||
glist = lambda : [ GfImFreq(indices = inner, beta = beta) for block,inner in gf_struct]
|
||||
self.G_upfold = BlockGf(name_list = block_ind_list, block_list = glist(), make_copies = False)
|
||||
self.G_upfold.zero()
|
||||
if iw_or_w == "iw":
|
||||
glist = lambda : [ GfImFreq(indices=inner,beta=beta) for block,inner in gf_struct]
|
||||
elif iw_or_w == "w":
|
||||
if with_Sigma:
|
||||
glist = lambda : [ GfReFreq(indices=inner,mesh=Sigma_imp[0].mesh) for block,inner in gf_struct]
|
||||
else:
|
||||
glist = lambda : [ GfReFreq(indices=inner,window=(mesh[0],mesh[1]),n_points=mesh[2]) for block,inner in gf_struct]
|
||||
G_latt = BlockGf(name_list = block_ind_list, block_list = glist(), make_copies = False)
|
||||
G_latt.zero()
|
||||
|
||||
if iw_or_w == "iw":
|
||||
G_latt << iOmega_n
|
||||
elif iw_or_w == "w":
|
||||
G_latt << Omega + 1j*broadening
|
||||
|
||||
self.G_upfold << iOmega_n
|
||||
idmat = [numpy.identity(self.n_orbitals[ik,ntoi[sp]],numpy.complex_) for sp in spn]
|
||||
M = copy.deepcopy(idmat)
|
||||
for isp in range(self.n_spin_blocks[self.SO]):
|
||||
ind = ntoi[spn[isp]]
|
||||
for ibl in range(self.n_spin_blocks[self.SO]):
|
||||
ind = ntoi[spn[ibl]]
|
||||
n_orb = self.n_orbitals[ik,ind]
|
||||
M[isp] = self.hopping[ik,ind,0:n_orb,0:n_orb] - (idmat[isp]*mu) - (idmat[isp] * self.h_field * (1-2*isp))
|
||||
self.G_upfold -= M
|
||||
M[ibl] = self.hopping[ik,ind,0:n_orb,0:n_orb] - (idmat[ibl]*mu) - (idmat[ibl] * self.h_field * (1-2*ibl))
|
||||
G_latt -= M
|
||||
|
||||
if with_Sigma:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bname,gf in self.G_upfold: gf -= self.upfold(ik,icrsh,bname,stmp[icrsh][bname],gf)
|
||||
for bname,gf in G_latt: gf -= self.upfold(ik,icrsh,bname,sigma_minus_dc[icrsh][bname],gf)
|
||||
|
||||
self.G_upfold.invert()
|
||||
G_latt.invert()
|
||||
setattr(self,"G_latt_"+iw_or_w,G_latt)
|
||||
|
||||
return self.G_upfold
|
||||
return G_latt
|
||||
|
||||
|
||||
def put_Sigma(self, Sigma_imp):
|
||||
"""Puts the impurity self energies for inequivalent atoms into the class, respects the multiplicity of the atoms."""
|
||||
"""Sets the impurity self energies for inequivalent atoms into the class, respects the multiplicity of the atoms."""
|
||||
|
||||
assert isinstance(Sigma_imp,list), "Sigma_imp has to be a list of Sigmas for the correlated shells, even if it is of length 1!"
|
||||
assert len(Sigma_imp) == self.n_inequiv_shells, "give exactly one Sigma for each inequivalent corr. shell!"
|
||||
assert isinstance(Sigma_imp,list), "put_Sigma: Sigma_imp has to be a list of Sigmas for the correlated shells, even if it is of length 1!"
|
||||
assert len(Sigma_imp) == self.n_inequiv_shells, "put_Sigma: give exactly one Sigma for each inequivalent corr. shell!"
|
||||
|
||||
# init self.Sigma_imp:
|
||||
# init self.Sigma_imp_(i)w:
|
||||
if all(type(gf) == GfImFreq for bname,gf in Sigma_imp[0]):
|
||||
# Imaginary frequency Sigma:
|
||||
self.Sigma_imp = [ BlockGf( name_block_generator = [ (block,GfImFreq(indices = inner, mesh = Sigma_imp[0].mesh)) for block,inner in self.gf_struct_sumk[icrsh] ],
|
||||
make_copies = False) for icrsh in range(self.n_corr_shells) ]
|
||||
self.Sigma_imp_iw = [ BlockGf( name_block_generator = [ (block,GfImFreq(indices = inner, mesh = Sigma_imp[0].mesh))
|
||||
for block,inner in self.gf_struct_sumk[icrsh] ], make_copies = False)
|
||||
for icrsh in range(self.n_corr_shells) ]
|
||||
SK_Sigma_imp = self.Sigma_imp_iw
|
||||
elif all(type(gf) == GfReFreq for bname,gf in Sigma_imp[0]):
|
||||
# Real frequency Sigma:
|
||||
self.Sigma_imp = [ BlockGf( name_block_generator = [ (block,GfReFreq(indices = inner, mesh = Sigma_imp[0].mesh)) for block,inner in self.gf_struct_sumk[icrsh] ],
|
||||
make_copies = False) for icrsh in range(self.n_corr_shells) ]
|
||||
self.Sigma_imp_w = [ BlockGf( name_block_generator = [ (block,GfReFreq(indices = inner, mesh = Sigma_imp[0].mesh))
|
||||
for block,inner in self.gf_struct_sumk[icrsh] ], make_copies = False)
|
||||
for icrsh in range(self.n_corr_shells) ]
|
||||
SK_Sigma_imp = self.Sigma_imp_w
|
||||
else:
|
||||
raise ValueError, "This type of Sigma is not handled."
|
||||
raise ValueError, "put_Sigma: This type of Sigma is not handled."
|
||||
|
||||
# transform the CTQMC blocks to the full matrix:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
|
|
@ -305,12 +327,12 @@ class SumkDFT:
|
|||
for ind2 in inner:
|
||||
block_sumk,ind1_sumk = self.solver_to_sumk[ish][(block,ind1)]
|
||||
block_sumk,ind2_sumk = self.solver_to_sumk[ish][(block,ind2)]
|
||||
self.Sigma_imp[icrsh][block_sumk][ind1_sumk,ind2_sumk] << Sigma_imp[ish][block][ind1,ind2]
|
||||
SK_Sigma_imp[icrsh][block_sumk][ind1_sumk,ind2_sumk] << Sigma_imp[ish][block][ind1,ind2]
|
||||
|
||||
# rotation from local to global coordinate system:
|
||||
if self.use_rotations:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bname,gf in self.Sigma_imp[icrsh]: self.Sigma_imp[icrsh][bname] << self.rotloc(icrsh, gf, direction = 'toGlobal')
|
||||
for bname,gf in SK_Sigma_imp[icrsh]: gf << self.rotloc(icrsh, gf, direction = 'toGlobal')
|
||||
|
||||
|
||||
def extract_G_loc(self, mu = None, with_Sigma = True):
|
||||
|
|
@ -321,19 +343,19 @@ class SumkDFT:
|
|||
"""
|
||||
|
||||
if mu is None: mu = self.chemical_potential
|
||||
Gloc = [ self.Sigma_imp[icrsh].copy() for icrsh in range(self.n_corr_shells) ] # this list will be returned
|
||||
for icrsh in range(self.n_corr_shells): Gloc[icrsh].zero() # initialize to zero
|
||||
Gloc = [ self.Sigma_imp_iw[icrsh].copy() for icrsh in range(self.n_corr_shells) ] # this list will be returned
|
||||
for icrsh in range(self.n_corr_shells): Gloc[icrsh].zero() # initialize to zero
|
||||
beta = Gloc[0].mesh.beta
|
||||
|
||||
ikarray = numpy.array(range(self.n_k))
|
||||
for ik in mpi.slice_array(ikarray):
|
||||
|
||||
S = self.lattice_gf_matsubara(ik = ik, mu = mu, with_Sigma = with_Sigma, beta = beta)
|
||||
S *= self.bz_weights[ik]
|
||||
G_latt_iw = self.lattice_gf(ik = ik, mu = mu, iw_or_w = "iw", with_Sigma = with_Sigma, beta = beta)
|
||||
G_latt_iw *= self.bz_weights[ik]
|
||||
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
tmp = Gloc[icrsh].copy() # init temporary storage
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold(ik,icrsh,bname,S[bname],gf)
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold(ik,icrsh,bname,G_latt_iw[bname],gf)
|
||||
Gloc[icrsh] += tmp
|
||||
|
||||
# collect data from mpi
|
||||
|
|
@ -350,19 +372,18 @@ class SumkDFT:
|
|||
for bname,gf in Gloc[icrsh]: Gloc[icrsh][bname] << self.rotloc(icrsh,gf,direction = 'toLocal')
|
||||
|
||||
# transform to CTQMC blocks:
|
||||
Glocret = [ BlockGf( name_block_generator = [ (block,GfImFreq(indices = inner, mesh = Gloc[0].mesh)) for block,inner in self.gf_struct_solver[ish].iteritems() ],
|
||||
Gloc_inequiv = [ BlockGf( name_block_generator = [ (block,GfImFreq(indices = inner, mesh = Gloc[0].mesh)) for block,inner in self.gf_struct_solver[ish].iteritems() ],
|
||||
make_copies = False) for ish in range(self.n_inequiv_shells) ]
|
||||
for ish in range(self.n_inequiv_shells):
|
||||
|
||||
for block,inner in self.gf_struct_solver[ish].iteritems():
|
||||
for ind1 in inner:
|
||||
for ind2 in inner:
|
||||
block_sumk,ind1_sumk = self.solver_to_sumk[ish][(block,ind1)]
|
||||
block_sumk,ind2_sumk = self.solver_to_sumk[ish][(block,ind2)]
|
||||
Glocret[ish][block][ind1,ind2] << Gloc[self.inequiv_to_corr[ish]][block_sumk][ind1_sumk,ind2_sumk]
|
||||
Gloc_inequiv[ish][block][ind1,ind2] << Gloc[self.inequiv_to_corr[ish]][block_sumk][ind1_sumk,ind2_sumk]
|
||||
|
||||
# return only the inequivalent shells:
|
||||
return Glocret
|
||||
return Gloc_inequiv
|
||||
|
||||
|
||||
def analyse_block_structure(self, threshold = 0.00001, include_shells = None, dm = None):
|
||||
|
|
@ -451,7 +472,7 @@ class SumkDFT:
|
|||
|
||||
def density_matrix(self, method = 'using_gf', beta = 40.0):
|
||||
"""Calculate density matrices in one of two ways:
|
||||
if 'using_gf': First get upfolded gf (g_loc is not set up), then density matrix.
|
||||
if 'using_gf': First get lattice gf (g_loc is not set up), then density matrix.
|
||||
It is useful for Hubbard I, and very quick.
|
||||
No assumption on the hopping structure is made (ie diagonal or not).
|
||||
if 'using_point_integration': Only works for diagonal hopping matrix (true in wien2k).
|
||||
|
|
@ -466,9 +487,9 @@ class SumkDFT:
|
|||
|
||||
if method == "using_gf":
|
||||
|
||||
G_upfold = self.lattice_gf_matsubara(ik = ik, beta = beta, mu = self.chemical_potential)
|
||||
G_upfold *= self.bz_weights[ik]
|
||||
dm = G_upfold.density()
|
||||
G_latt_iw = self.lattice_gf(ik = ik, mu = self.chemical_potential, iw_or_w = "iw", beta = beta)
|
||||
G_latt_iw *= self.bz_weights[ik]
|
||||
dm = G_latt_iw.density()
|
||||
MMat = [dm[sp] for sp in self.spin_block_names[self.SO]]
|
||||
|
||||
elif method == "using_point_integration":
|
||||
|
|
@ -494,10 +515,10 @@ class SumkDFT:
|
|||
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for isp, sp in enumerate(self.spin_block_names[self.corr_shells[icrsh]['SO']]):
|
||||
isp = self.spin_names_to_ind[self.corr_shells[icrsh]['SO']][sp]
|
||||
ind = self.spin_names_to_ind[self.corr_shells[icrsh]['SO']][sp]
|
||||
dim = self.corr_shells[icrsh]['dim']
|
||||
n_orb = self.n_orbitals[ik,isp]
|
||||
projmat = self.proj_mat[ik,isp,icrsh,0:dim,0:n_orb]
|
||||
n_orb = self.n_orbitals[ik,ind]
|
||||
projmat = self.proj_mat[ik,ind,icrsh,0:dim,0:n_orb]
|
||||
if method == "using_gf":
|
||||
dens_mat[icrsh][sp] += numpy.dot( numpy.dot(projmat,MMat[isp]),
|
||||
projmat.transpose().conjugate() )
|
||||
|
|
@ -507,8 +528,8 @@ class SumkDFT:
|
|||
|
||||
# get data from nodes:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bname in dens_mat[icrsh]:
|
||||
dens_mat[icrsh][bname] = mpi.all_reduce(mpi.world, dens_mat[icrsh][bname], lambda x,y : x+y)
|
||||
for sp in dens_mat[icrsh]:
|
||||
dens_mat[icrsh][sp] = mpi.all_reduce(mpi.world, dens_mat[icrsh][sp], lambda x,y : x+y)
|
||||
mpi.barrier()
|
||||
|
||||
if self.symm_op != 0: dens_mat = self.symmcorr.symmetrize(dens_mat)
|
||||
|
|
@ -516,9 +537,9 @@ class SumkDFT:
|
|||
# Rotate to local coordinate system:
|
||||
if self.use_rotations:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bl in dens_mat[icrsh]:
|
||||
if self.rot_mat_time_inv[icrsh] == 1: dens_mat[icrsh][bl] = dens_mat[icrsh][bl].conjugate()
|
||||
dens_mat[icrsh][bl] = numpy.dot( numpy.dot(self.rot_mat[icrsh].conjugate().transpose(),dens_mat[icrsh][bl]),
|
||||
for sp in dens_mat[icrsh]:
|
||||
if self.rot_mat_time_inv[icrsh] == 1: dens_mat[icrsh][sp] = dens_mat[icrsh][sp].conjugate()
|
||||
dens_mat[icrsh][sp] = numpy.dot( numpy.dot(self.rot_mat[icrsh].conjugate().transpose(),dens_mat[icrsh][sp]),
|
||||
self.rot_mat[icrsh] )
|
||||
|
||||
return dens_mat
|
||||
|
|
@ -533,54 +554,41 @@ class SumkDFT:
|
|||
for ish in range(self.n_inequiv_shells):
|
||||
for sp in self.spin_block_names[self.corr_shells[self.inequiv_to_corr[ish]]['SO']]:
|
||||
eff_atlevels[ish][sp] = numpy.identity(self.corr_shells[self.inequiv_to_corr[ish]]['dim'], numpy.complex_)
|
||||
|
||||
# Chemical Potential:
|
||||
for ish in range(self.n_inequiv_shells):
|
||||
for ii in eff_atlevels[ish]:
|
||||
eff_atlevels[ish][ii] *= -self.chemical_potential
|
||||
|
||||
# double counting term:
|
||||
for ish in range(self.n_inequiv_shells):
|
||||
for ii in eff_atlevels[ish]:
|
||||
eff_atlevels[ish][ii] -= self.dc_imp[self.inequiv_to_corr[ish]][ii]
|
||||
eff_atlevels[ish][sp] *= -self.chemical_potential
|
||||
eff_atlevels[ish][sp] -= self.dc_imp[self.inequiv_to_corr[ish]][sp]
|
||||
|
||||
# sum over k:
|
||||
if not hasattr(self,"Hsumk"):
|
||||
# calculate the sum over k. Does not depend on mu, so do it only once:
|
||||
self.Hsumk = [ {} for icrsh in range(self.n_corr_shells) ]
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for sp in self.spin_block_names[self.corr_shells[icrsh]['SO']]:
|
||||
dim = self.corr_shells[icrsh]['dim'] #*(1+self.corr_shells[icrsh]['SO'])
|
||||
self.Hsumk[icrsh][sp] = numpy.zeros([dim,dim],numpy.complex_)
|
||||
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
dim = self.corr_shells[icrsh]['dim']
|
||||
for sp in self.spin_block_names[self.corr_shells[icrsh]['SO']]:
|
||||
self.Hsumk[icrsh][sp] = numpy.zeros([dim,dim],numpy.complex_)
|
||||
for isp, sp in enumerate(self.spin_block_names[self.corr_shells[icrsh]['SO']]):
|
||||
isp = self.spin_names_to_ind[self.corr_shells[icrsh]['SO']][sp]
|
||||
ind = self.spin_names_to_ind[self.corr_shells[icrsh]['SO']][sp]
|
||||
for ik in range(self.n_k):
|
||||
n_orb = self.n_orbitals[ik,isp]
|
||||
n_orb = self.n_orbitals[ik,ind]
|
||||
MMat = numpy.identity(n_orb, numpy.complex_)
|
||||
MMat = self.hopping[ik,isp,0:n_orb,0:n_orb] - (1-2*isp) * self.h_field * MMat
|
||||
projmat = self.proj_mat[ik,isp,icrsh,0:dim,0:n_orb]
|
||||
MMat = self.hopping[ik,ind,0:n_orb,0:n_orb] - (1-2*isp) * self.h_field * MMat
|
||||
projmat = self.proj_mat[ik,ind,icrsh,0:dim,0:n_orb]
|
||||
self.Hsumk[icrsh][sp] += self.bz_weights[ik] * numpy.dot( numpy.dot(projmat,MMat),
|
||||
projmat.conjugate().transpose() )
|
||||
|
||||
# symmetrisation:
|
||||
if self.symm_op != 0: self.Hsumk = self.symmcorr.symmetrize(self.Hsumk)
|
||||
|
||||
# Rotate to local coordinate system:
|
||||
if self.use_rotations:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bl in self.Hsumk[icrsh]:
|
||||
|
||||
if self.rot_mat_time_inv[icrsh] == 1: self.Hsumk[icrsh][bl] = self.Hsumk[icrsh][bl].conjugate()
|
||||
self.Hsumk[icrsh][bl] = numpy.dot( numpy.dot(self.rot_mat[icrsh].conjugate().transpose(),self.Hsumk[icrsh][bl]) ,
|
||||
for sp in self.Hsumk[icrsh]:
|
||||
if self.rot_mat_time_inv[icrsh] == 1: self.Hsumk[icrsh][sp] = self.Hsumk[icrsh][sp].conjugate()
|
||||
self.Hsumk[icrsh][sp] = numpy.dot( numpy.dot(self.rot_mat[icrsh].conjugate().transpose(),self.Hsumk[icrsh][sp]) ,
|
||||
self.rot_mat[icrsh] )
|
||||
|
||||
# add to matrix:
|
||||
for ish in range(self.n_inequiv_shells):
|
||||
for bl in eff_atlevels[ish]:
|
||||
eff_atlevels[ish][bl] += self.Hsumk[self.inequiv_to_corr[ish]][bl]
|
||||
for sp in eff_atlevels[ish]:
|
||||
eff_atlevels[ish][sp] += self.Hsumk[self.inequiv_to_corr[ish]][sp]
|
||||
|
||||
|
||||
return eff_atlevels
|
||||
|
|
@ -588,6 +596,7 @@ class SumkDFT:
|
|||
|
||||
def init_dc(self):
|
||||
""" Initialise the double counting terms to have the correct shape."""
|
||||
|
||||
self.dc_imp = [ {} for icrsh in range(self.n_corr_shells)]
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
dim = self.corr_shells[icrsh]['dim']
|
||||
|
|
@ -672,25 +681,24 @@ class SumkDFT:
|
|||
mpi.report("DC energy = %s"%self.dc_energ[icrsh])
|
||||
|
||||
|
||||
def add_dc(self):
|
||||
def add_dc(self,iw_or_w="iw"):
|
||||
"""Substracts the double counting term from the impurity self energy."""
|
||||
|
||||
# Be careful: Sigma_imp is already in the global coordinate system!!
|
||||
sres = [s.copy() for s in self.Sigma_imp]
|
||||
sigma_minus_dc = [s.copy() for s in getattr(self,"Sigma_imp_"+iw_or_w)]
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bname,gf in sres[icrsh]:
|
||||
for bname,gf in sigma_minus_dc[icrsh]:
|
||||
# Transform dc_imp to global coordinate system
|
||||
dccont = numpy.dot(self.rot_mat[icrsh],numpy.dot(self.dc_imp[icrsh][bname],self.rot_mat[icrsh].conjugate().transpose()))
|
||||
sres[icrsh][bname] -= dccont
|
||||
sigma_minus_dc[icrsh][bname] -= dccont
|
||||
|
||||
return sres # list of self energies corrected by DC
|
||||
return sigma_minus_dc
|
||||
|
||||
|
||||
def symm_deg_gf(self,gf_to_symm,orb):
|
||||
"""Symmetrises a GF for the given degenerate shells self.deg_shells"""
|
||||
|
||||
for degsh in self.deg_shells[orb]:
|
||||
#loop over degenerate shells:
|
||||
ss = gf_to_symm[degsh[0]].copy()
|
||||
ss.zero()
|
||||
n_deg = len(degsh)
|
||||
|
|
@ -710,10 +718,8 @@ class SumkDFT:
|
|||
dens = 0.0
|
||||
ikarray = numpy.array(range(self.n_k))
|
||||
for ik in mpi.slice_array(ikarray):
|
||||
|
||||
S = self.lattice_gf_matsubara(ik = ik, mu = mu)
|
||||
dens += self.bz_weights[ik] * S.total_density()
|
||||
|
||||
G_latt_iw = self.lattice_gf(ik = ik, mu = mu, iw_or_w = "iw")
|
||||
dens += self.bz_weights[ik] * G_latt_iw.total_density()
|
||||
# collect data from mpi:
|
||||
dens = mpi.all_reduce(mpi.world, dens, lambda x,y : x+y)
|
||||
mpi.barrier()
|
||||
|
|
@ -748,7 +754,7 @@ class SumkDFT:
|
|||
def calc_density_correction(self,filename = 'dens_mat.dat'):
|
||||
""" Calculates the density correction in order to feed it back to the DFT calculations."""
|
||||
|
||||
assert type(filename) == StringType, "filename has to be a string!"
|
||||
assert type(filename) == StringType, "calc_density_correction: filename has to be a string!"
|
||||
|
||||
ntoi = self.spin_names_to_ind[self.SO]
|
||||
spn = self.spin_block_names[self.SO]
|
||||
|
|
@ -761,12 +767,12 @@ class SumkDFT:
|
|||
|
||||
ikarray = numpy.array(range(self.n_k))
|
||||
for ik in mpi.slice_array(ikarray):
|
||||
S = self.lattice_gf_matsubara(ik = ik, mu = self.chemical_potential)
|
||||
for bname,gf in S:
|
||||
deltaN[bname][ik] = S[bname].density()
|
||||
dens[bname] += self.bz_weights[ik] * S[bname].total_density()
|
||||
G_latt_iw = self.lattice_gf(ik = ik, mu = self.chemical_potential, iw_or_w = "iw")
|
||||
for bname,gf in G_latt_iw:
|
||||
deltaN[bname][ik] = G_latt_iw[bname].density()
|
||||
dens[bname] += self.bz_weights[ik] * G_latt_iw[bname].total_density()
|
||||
|
||||
#put mpi Barrier:
|
||||
# mpi reduce:
|
||||
for bname in deltaN:
|
||||
for ik in range(self.n_k):
|
||||
deltaN[bname][ik] = mpi.all_reduce(mpi.world, deltaN[bname][ik], lambda x,y : x+y)
|
||||
|
|
@ -783,9 +789,9 @@ class SumkDFT:
|
|||
# write chemical potential (in Rydberg):
|
||||
f.write("%.14f\n"%(self.chemical_potential/self.energy_unit))
|
||||
if self.SP != 0: f1.write("%.14f\n"%(self.chemical_potential/self.energy_unit))
|
||||
# write beta in ryderg-1
|
||||
f.write("%.14f\n"%(S.mesh.beta*self.energy_unit))
|
||||
if self.SP != 0: f1.write("%.14f\n"%(S.mesh.beta*self.energy_unit))
|
||||
# write beta in rydberg-1
|
||||
f.write("%.14f\n"%(G_latt_iw.mesh.beta*self.energy_unit))
|
||||
if self.SP != 0: f1.write("%.14f\n"%(G_latt_iw.mesh.beta*self.energy_unit))
|
||||
|
||||
if self.SP == 0: # no spin-polarization
|
||||
|
||||
|
|
@ -847,12 +853,10 @@ class SumkDFT:
|
|||
return self.chemical_potential
|
||||
|
||||
|
||||
def find_dc(self,orb,guess,dens_mat,dens_req=None,precision=0.01):
|
||||
def calc_dc_for_density(self,orb,dc_init,dens_mat,density=None,precision=0.01):
|
||||
"""Searches for DC in order to fulfill charge neutrality.
|
||||
If dens_req is given, then DC is set such that the LOCAL charge of orbital
|
||||
orb coincides with dens_req."""
|
||||
|
||||
mu = self.chemical_potential
|
||||
If density is given, then DC is set such that the LOCAL charge of orbital
|
||||
orb coincides with the given density."""
|
||||
|
||||
def F(dc):
|
||||
self.calc_dc(dens_mat = dens_mat, U_interact = 0, J_hund = 0, orb = orb, use_dc_value = dc)
|
||||
|
|
@ -861,24 +865,20 @@ class SumkDFT:
|
|||
else:
|
||||
return self.extract_G_loc()[orb].total_density()
|
||||
|
||||
if density is None: density = self.density_required - self.charge_below
|
||||
|
||||
if dens_req is None:
|
||||
density = self.density_required - self.charge_below
|
||||
else:
|
||||
density = dens_req
|
||||
|
||||
dcnew = dichotomy.dichotomy(function = F,
|
||||
x_init = guess, y_value = density,
|
||||
dc = dichotomy.dichotomy(function = F,
|
||||
x_init = dc_init, y_value = density,
|
||||
precision_on_y = precision, delta_x = 0.5,
|
||||
max_loops = 100, x_name = "Double Counting", y_name= "Total Density",
|
||||
verbosity = 3)[0]
|
||||
|
||||
return dcnew
|
||||
return dc
|
||||
|
||||
|
||||
# Check that the density matrix from projectors (DM = P Pdagger) is correct (ie matches DFT)
|
||||
def check_projectors(self):
|
||||
|
||||
"""Calculated the density matrix from projectors (DM = P Pdagger) to check that it is correct and
|
||||
specifically that it matches DFT."""
|
||||
dens_mat = [numpy.zeros([self.corr_shells[icrsh]['dim'],self.corr_shells[icrsh]['dim']],numpy.complex_)
|
||||
for icrsh in range(self.n_corr_shells)]
|
||||
|
||||
|
|
@ -895,27 +895,25 @@ class SumkDFT:
|
|||
if self.use_rotations:
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
if self.rot_mat_time_inv[icrsh] == 1: dens_mat[icrsh] = dens_mat[icrsh].conjugate()
|
||||
dens_mat[icrsh] = numpy.dot( numpy.dot(self.rot_mat[icrsh].conjugate().transpose(),dens_mat[icrsh]) ,
|
||||
dens_mat[icrsh] = numpy.dot( numpy.dot(self.rot_mat[icrsh].conjugate().transpose(),dens_mat[icrsh]),
|
||||
self.rot_mat[icrsh] )
|
||||
|
||||
return dens_mat
|
||||
|
||||
|
||||
# Determine the number of equivalent shells
|
||||
def sorts_of_atoms(self,lst):
|
||||
def sorts_of_atoms(self,shells):
|
||||
"""
|
||||
This routine should determine the number of sorts in the double list lst
|
||||
Determine the number of inequivalent sorts.
|
||||
"""
|
||||
sortlst = [ lst[i][1] for i in range(len(lst)) ]
|
||||
sorts = len(set(sortlst))
|
||||
return sorts
|
||||
sortlst = [ shells[i]['sort'] for i in range(len(shells)) ]
|
||||
n_sorts = len(set(sortlst))
|
||||
return n_sorts
|
||||
|
||||
|
||||
# Determine the number of atoms
|
||||
def number_of_atoms(self,lst):
|
||||
def number_of_atoms(self,shells):
|
||||
"""
|
||||
This routine should determine the number of atoms in the double list lst
|
||||
Determine the number of inequivalent atoms.
|
||||
"""
|
||||
atomlst = [ lst[i][0] for i in range(len(lst)) ]
|
||||
atoms = len(set(atomlst))
|
||||
return atoms
|
||||
atomlst = [ shells[i]['atom'] for i in range(len(shells)) ]
|
||||
n_atoms = len(set(atomlst))
|
||||
return n_atoms
|
||||
|
|
|
|||
|
|
@ -22,7 +22,6 @@
|
|||
|
||||
from types import *
|
||||
import numpy
|
||||
import pytriqs.utility.dichotomy as dichotomy
|
||||
from pytriqs.gf.local import *
|
||||
import pytriqs.utility.mpi as mpi
|
||||
from symmetry import *
|
||||
|
|
@ -36,7 +35,7 @@ class SumkDFTTools(SumkDFT):
|
|||
parproj_data = 'dft_parproj_input', symmpar_data = 'dft_symmpar_input', bands_data = 'dft_bands_input',
|
||||
transp_data = 'dft_transp_input'):
|
||||
|
||||
self.G_upfold_refreq = None
|
||||
#self.G_latt_w = None # DEBUG -- remove later
|
||||
SumkDFT.__init__(self, hdf_file=hdf_file, h_field=h_field, use_dft_blocks=use_dft_blocks,
|
||||
dft_data=dft_data, symmcorr_data=symmcorr_data, parproj_data=parproj_data,
|
||||
symmpar_data=symmpar_data, bands_data=bands_data, transp_data=transp_data)
|
||||
|
|
@ -60,7 +59,7 @@ class SumkDFTTools(SumkDFT):
|
|||
"""Local <-> Global rotation of a GF block.
|
||||
direction: 'toLocal' / 'toGlobal' """
|
||||
|
||||
assert (direction == 'toLocal' or direction == 'toGlobal'),"Give direction 'toLocal' or 'toGlobal' in rotloc!"
|
||||
assert (direction == 'toLocal' or direction == 'toGlobal'),"rotloc_all: Give direction 'toLocal' or 'toGlobal'."
|
||||
|
||||
|
||||
gf_rotated = gf_to_rotate.copy()
|
||||
|
|
@ -82,69 +81,6 @@ class SumkDFTTools(SumkDFT):
|
|||
return gf_rotated
|
||||
|
||||
|
||||
def lattice_gf_realfreq(self, ik, mu, broadening, mesh=None, with_Sigma=True):
|
||||
"""Calculates the lattice Green function on the real frequency axis. If self energy is
|
||||
present and with_Sigma=True, the mesh is taken from Sigma. Otherwise, the mesh has to be given."""
|
||||
|
||||
ntoi = self.spin_names_to_ind[self.SO]
|
||||
spn = self.spin_block_names[self.SO]
|
||||
|
||||
if not hasattr(self,"Sigma_imp"): with_Sigma=False
|
||||
if with_Sigma:
|
||||
assert all(type(gf) == GfReFreq for bname,gf in self.Sigma_imp[0]), "Real frequency Sigma needed for lattice_gf_realfreq!"
|
||||
stmp = self.add_dc()
|
||||
else:
|
||||
assert (not mesh is None),"Without Sigma, give the mesh=(om_min,om_max,n_points) for lattice_gf_realfreq!"
|
||||
|
||||
if self.G_upfold_refreq is None:
|
||||
# first setting up of G_upfold_refreq
|
||||
block_structure = [ range(self.n_orbitals[ik,ntoi[sp]]) for sp in spn ]
|
||||
gf_struct = [ (spn[isp], block_structure[isp]) for isp in range(self.n_spin_blocks[self.SO]) ]
|
||||
block_ind_list = [block for block,inner in gf_struct]
|
||||
if with_Sigma:
|
||||
glist = lambda : [ GfReFreq(indices = inner, mesh=self.Sigma_imp[0].mesh) for block,inner in gf_struct]
|
||||
else:
|
||||
glist = lambda : [ GfReFreq(indices = inner, window=(mesh[0],mesh[1]), n_points=mesh[2]) for block,inner in gf_struct]
|
||||
self.G_upfold_refreq = BlockGf(name_list = block_ind_list, block_list = glist(),make_copies=False)
|
||||
self.G_upfold_refreq.zero()
|
||||
|
||||
GFsize = [ gf.N1 for bname,gf in self.G_upfold_refreq]
|
||||
unchangedsize = all( [ self.n_orbitals[ik,ntoi[spn[isp]]] == GFsize[isp]
|
||||
for isp in range(self.n_spin_blocks[self.SO]) ] )
|
||||
|
||||
if not unchangedsize:
|
||||
block_structure = [ range(self.n_orbitals[ik,ntoi[sp]]) for sp in spn ]
|
||||
gf_struct = [ (spn[isp], block_structure[isp]) for isp in range(self.n_spin_blocks[self.SO]) ]
|
||||
block_ind_list = [block for block,inner in gf_struct]
|
||||
if with_Sigma:
|
||||
glist = lambda : [ GfReFreq(indices = inner, mesh =self.Sigma_imp[0].mesh) for block,inner in gf_struct]
|
||||
else:
|
||||
glist = lambda : [ GfReFreq(indices = inner, window=(mesh[0],mesh[1]), n_points=mesh[2]) for block,inner in gf_struct]
|
||||
self.G_upfold_refreq = BlockGf(name_list = block_ind_list, block_list = glist(),make_copies=False)
|
||||
self.G_upfold_refreq.zero()
|
||||
|
||||
idmat = [numpy.identity(self.n_orbitals[ik,ntoi[sp]],numpy.complex_) for sp in spn]
|
||||
|
||||
self.G_upfold_refreq << Omega + 1j*broadening
|
||||
M = copy.deepcopy(idmat)
|
||||
for isp in range(self.n_spin_blocks[self.SO]):
|
||||
ind = ntoi[spn[isp]]
|
||||
n_orb = self.n_orbitals[ik,ind]
|
||||
M[isp] = self.hopping[ik,ind,0:n_orb,0:n_orb] - (idmat[isp]*mu) - (idmat[isp] * self.h_field * (1-2*isp))
|
||||
self.G_upfold_refreq -= M
|
||||
|
||||
if with_Sigma:
|
||||
tmp = self.G_upfold_refreq.copy() # init temporary storage
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
for bname,gf in tmp: tmp[bname] << self.upfold(ik,icrsh,bname,stmp[icrsh][bname],gf)
|
||||
self.G_upfold_refreq -= tmp # adding to the upfolded GF
|
||||
|
||||
self.G_upfold_refreq.invert()
|
||||
|
||||
return self.G_upfold_refreq
|
||||
|
||||
|
||||
|
||||
def check_input_dos(self, om_min, om_max, n_om, beta=10, broadening=0.01):
|
||||
|
||||
|
||||
|
|
@ -153,16 +89,16 @@ class SumkDFTTools(SumkDFT):
|
|||
for i in range(n_om): om_mesh[i] = om_min + delta_om * i
|
||||
|
||||
DOS = {}
|
||||
for bn in self.spin_block_names[self.SO]:
|
||||
DOS[bn] = numpy.zeros([n_om],numpy.float_)
|
||||
for sp in self.spin_block_names[self.SO]:
|
||||
DOS[sp] = numpy.zeros([n_om],numpy.float_)
|
||||
|
||||
DOSproj = [ {} for ish in range(self.n_inequiv_shells) ]
|
||||
DOSproj_orb = [ {} for ish in range(self.n_inequiv_shells) ]
|
||||
for ish in range(self.n_inequiv_shells):
|
||||
for bn in self.spin_block_names[self.corr_shells[self.inequiv_to_corr[ish]]['SO']]:
|
||||
for sp in self.spin_block_names[self.corr_shells[self.inequiv_to_corr[ish]]['SO']]:
|
||||
dim = self.corr_shells[self.inequiv_to_corr[ish]]['dim']
|
||||
DOSproj[ish][bn] = numpy.zeros([n_om],numpy.float_)
|
||||
DOSproj_orb[ish][bn] = numpy.zeros([n_om,dim,dim],numpy.float_)
|
||||
DOSproj[ish][sp] = numpy.zeros([n_om],numpy.float_)
|
||||
DOSproj_orb[ish][sp] = numpy.zeros([n_om,dim,dim],numpy.float_)
|
||||
|
||||
# init:
|
||||
Gloc = []
|
||||
|
|
@ -174,18 +110,18 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
for ik in range(self.n_k):
|
||||
|
||||
G_upfold=self.lattice_gf_realfreq(ik=ik,mu=self.chemical_potential,broadening=broadening,mesh=(om_min,om_max,n_om),with_Sigma=False)
|
||||
G_upfold *= self.bz_weights[ik]
|
||||
G_latt_w=self.lattice_gf(ik=ik,mu=self.chemical_potential,iw_or_w="w",broadening=broadening,mesh=(om_min,om_max,n_om),with_Sigma=False)
|
||||
G_latt_w *= self.bz_weights[ik]
|
||||
|
||||
# non-projected DOS
|
||||
for iom in range(n_om):
|
||||
for bname,gf in G_upfold:
|
||||
for bname,gf in G_latt_w:
|
||||
asd = gf.data[iom,:,:].imag.trace()/(-3.1415926535)
|
||||
DOS[bname][iom] += asd
|
||||
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
tmp = Gloc[icrsh].copy()
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold(ik,icrsh,bname,G_upfold[bname],gf) # downfolding G
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold(ik,icrsh,bname,G_latt_w[bname],gf) # downfolding G
|
||||
Gloc[icrsh] += tmp
|
||||
|
||||
|
||||
|
|
@ -205,21 +141,21 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
# output:
|
||||
if mpi.is_master_node():
|
||||
for bn in self.spin_block_names[self.SO]:
|
||||
f=open('DOS%s.dat'%bn, 'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(om_mesh[i],DOS[bn][i]))
|
||||
for sp in self.spin_block_names[self.SO]:
|
||||
f=open('DOS%s.dat'%sp, 'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(om_mesh[i],DOS[sp][i]))
|
||||
f.close()
|
||||
|
||||
for ish in range(self.n_inequiv_shells):
|
||||
f=open('DOS%s_proj%s.dat'%(bn,ish),'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(om_mesh[i],DOSproj[ish][bn][i]))
|
||||
f=open('DOS%s_proj%s.dat'%(sp,ish),'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(om_mesh[i],DOSproj[ish][sp][i]))
|
||||
f.close()
|
||||
|
||||
for i in range(self.corr_shells[self.inequiv_to_corr[ish]]['dim']):
|
||||
for j in range(i,self.corr_shells[self.inequiv_to_corr[ish]]['dim']):
|
||||
Fname = 'DOS'+bn+'_proj'+str(ish)+'_'+str(i)+'_'+str(j)+'.dat'
|
||||
Fname = 'DOS'+sp+'_proj'+str(ish)+'_'+str(i)+'_'+str(j)+'.dat'
|
||||
f=open(Fname,'w')
|
||||
for iom in range(n_om): f.write("%s %s\n"%(om_mesh[iom],DOSproj_orb[ish][bn][iom,i,j]))
|
||||
for iom in range(n_om): f.write("%s %s\n"%(om_mesh[iom],DOSproj_orb[ish][sp][iom,i,j]))
|
||||
f.close()
|
||||
|
||||
|
||||
|
|
@ -239,7 +175,7 @@ class SumkDFTTools(SumkDFT):
|
|||
def dos_partial(self,broadening=0.01):
|
||||
"""calculates the orbitally-resolved DOS"""
|
||||
|
||||
assert hasattr(self,"Sigma_imp"), "Set Sigma First!!"
|
||||
assert hasattr(self,"Sigma_imp_w"), "dos_partial: Set Sigma_imp_w first."
|
||||
|
||||
value_read = self.read_parproj_input_from_hdf()
|
||||
if not value_read: return value_read
|
||||
|
|
@ -248,41 +184,41 @@ class SumkDFTTools(SumkDFT):
|
|||
mu = self.chemical_potential
|
||||
|
||||
gf_struct_proj = [ [ (sp, range(self.shells[i]['dim'])) for sp in self.spin_block_names[self.SO] ] for i in range(self.n_shells) ]
|
||||
Gproj = [BlockGf(name_block_generator = [ (block,GfReFreq(indices = inner, mesh = self.Sigma_imp[0].mesh)) for block,inner in gf_struct_proj[ish] ], make_copies = False )
|
||||
for ish in range(self.n_shells)]
|
||||
Gproj = [BlockGf(name_block_generator = [ (block,GfReFreq(indices = inner, mesh = self.Sigma_imp_w[0].mesh))
|
||||
for block,inner in gf_struct_proj[ish] ], make_copies = False ) for ish in range(self.n_shells)]
|
||||
for ish in range(self.n_shells): Gproj[ish].zero()
|
||||
|
||||
Msh = [x.real for x in self.Sigma_imp[0].mesh]
|
||||
n_om = len(Msh)
|
||||
mesh = [x.real for x in self.Sigma_imp_w[0].mesh]
|
||||
n_om = len(mesh)
|
||||
|
||||
DOS = {}
|
||||
for bn in self.spin_block_names[self.SO]:
|
||||
DOS[bn] = numpy.zeros([n_om],numpy.float_)
|
||||
for sp in self.spin_block_names[self.SO]:
|
||||
DOS[sp] = numpy.zeros([n_om],numpy.float_)
|
||||
|
||||
DOSproj = [ {} for ish in range(self.n_shells) ]
|
||||
DOSproj_orb = [ {} for ish in range(self.n_shells) ]
|
||||
for ish in range(self.n_shells):
|
||||
for bn in self.spin_block_names[self.SO]:
|
||||
for sp in self.spin_block_names[self.SO]:
|
||||
dim = self.shells[ish]['dim']
|
||||
DOSproj[ish][bn] = numpy.zeros([n_om],numpy.float_)
|
||||
DOSproj_orb[ish][bn] = numpy.zeros([n_om,dim,dim],numpy.float_)
|
||||
DOSproj[ish][sp] = numpy.zeros([n_om],numpy.float_)
|
||||
DOSproj_orb[ish][sp] = numpy.zeros([n_om,dim,dim],numpy.float_)
|
||||
|
||||
ikarray=numpy.array(range(self.n_k))
|
||||
|
||||
for ik in mpi.slice_array(ikarray):
|
||||
|
||||
S = self.lattice_gf_realfreq(ik=ik,mu=mu,broadening=broadening)
|
||||
S *= self.bz_weights[ik]
|
||||
G_latt_w = self.lattice_gf(ik=ik,mu=mu,iw_or_w="w",broadening=broadening)
|
||||
G_latt_w *= self.bz_weights[ik]
|
||||
|
||||
# non-projected DOS
|
||||
for iom in range(n_om):
|
||||
for bname,gf in S: DOS[bname][iom] += gf.data[iom,:,:].imag.trace()/(-3.1415926535)
|
||||
for bname,gf in G_latt_w: DOS[bname][iom] += gf.data[iom,:,:].imag.trace()/(-3.1415926535)
|
||||
|
||||
#projected DOS:
|
||||
for ish in range(self.n_shells):
|
||||
tmp = Gproj[ish].copy()
|
||||
for ir in range(self.n_parproj[ish]):
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold_pc(ik,ir,ish,bname,S[bname],gf)
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold_pc(ik,ir,ish,bname,G_latt_w[bname],gf)
|
||||
Gproj[ish] += tmp
|
||||
|
||||
# collect data from mpi:
|
||||
|
|
@ -307,22 +243,22 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
if mpi.is_master_node():
|
||||
# output to files
|
||||
for bn in self.spin_block_names[self.SO]:
|
||||
f=open('./DOScorr%s.dat'%bn, 'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(Msh[i],DOS[bn][i]))
|
||||
for sp in self.spin_block_names[self.SO]:
|
||||
f=open('./DOScorr%s.dat'%sp, 'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(mesh[i],DOS[sp][i]))
|
||||
f.close()
|
||||
|
||||
# partial
|
||||
for ish in range(self.n_shells):
|
||||
f=open('DOScorr%s_proj%s.dat'%(bn,ish),'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(Msh[i],DOSproj[ish][bn][i]))
|
||||
f=open('DOScorr%s_proj%s.dat'%(sp,ish),'w')
|
||||
for i in range(n_om): f.write("%s %s\n"%(mesh[i],DOSproj[ish][sp][i]))
|
||||
f.close()
|
||||
|
||||
for i in range(self.shells[ish]['dim']):
|
||||
for j in range(i,self.shells[ish]['dim']):
|
||||
Fname = './DOScorr'+bn+'_proj'+str(ish)+'_'+str(i)+'_'+str(j)+'.dat'
|
||||
Fname = './DOScorr'+sp+'_proj'+str(ish)+'_'+str(i)+'_'+str(j)+'.dat'
|
||||
f=open(Fname,'w')
|
||||
for iom in range(n_om): f.write("%s %s\n"%(Msh[iom],DOSproj_orb[ish][bn][iom,i,j]))
|
||||
for iom in range(n_om): f.write("%s %s\n"%(mesh[iom],DOSproj_orb[ish][sp][iom,i,j]))
|
||||
f.close()
|
||||
|
||||
|
||||
|
|
@ -332,7 +268,7 @@ class SumkDFTTools(SumkDFT):
|
|||
""" Calculates the correlated band structure with a real-frequency self energy.
|
||||
ATTENTION: Many things from the original input file are overwritten!!!"""
|
||||
|
||||
assert hasattr(self,"Sigma_imp"), "Set Sigma First!!"
|
||||
assert hasattr(self,"Sigma_imp_w"), "spaghettis: Set Sigma_imp_w first."
|
||||
things_to_read = ['n_k','n_orbitals','proj_mat','hopping','n_parproj','proj_mat_pc']
|
||||
value_read = self.read_input_from_hdf(subgrp=self.bands_data,things_to_read=things_to_read)
|
||||
if not value_read: return value_read
|
||||
|
|
@ -370,12 +306,12 @@ class SumkDFTTools(SumkDFT):
|
|||
spn = self.spin_block_names[self.SO]
|
||||
|
||||
# init DOS:
|
||||
M = [x.real for x in self.Sigma_imp[0].mesh]
|
||||
n_om = len(M)
|
||||
mesh = [x.real for x in self.Sigma_imp_w[0].mesh]
|
||||
n_om = len(mesh)
|
||||
|
||||
if plot_range is None:
|
||||
om_minplot = M[0]-0.001
|
||||
om_maxplot = M[n_om-1] + 0.001
|
||||
om_minplot = mesh[0]-0.001
|
||||
om_maxplot = mesh[n_om-1] + 0.001
|
||||
else:
|
||||
om_minplot = plot_range[0]
|
||||
om_maxplot = plot_range[1]
|
||||
|
|
@ -395,20 +331,20 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
if not ishell is None:
|
||||
GFStruct_proj = [ (sp, range(self.shells[ishell]['dim'])) for sp in spn ]
|
||||
Gproj = BlockGf(name_block_generator = [ (block,GfReFreq(indices = inner, mesh = self.Sigma_imp[0].mesh)) for block,inner in GFStruct_proj ], make_copies = False)
|
||||
Gproj = BlockGf(name_block_generator = [ (block,GfReFreq(indices = inner, mesh = self.Sigma_imp_w[0].mesh)) for block,inner in GFStruct_proj ], make_copies = False)
|
||||
Gproj.zero()
|
||||
|
||||
for ik in range(self.n_k):
|
||||
|
||||
S = self.lattice_gf_realfreq(ik=ik,mu=mu,broadening=broadening)
|
||||
G_latt_w = self.lattice_gf(ik=ik,mu=mu,iw_or_w="w",broadening=broadening)
|
||||
if ishell is None:
|
||||
# non-projected A(k,w)
|
||||
for iom in range(n_om):
|
||||
if (M[iom] > om_minplot) and (M[iom] < om_maxplot):
|
||||
if (mesh[iom] > om_minplot) and (mesh[iom] < om_maxplot):
|
||||
if fermi_surface:
|
||||
for bname,gf in S: Akw[bname][ik,0] += gf.data[iom,:,:].imag.trace()/(-3.1415926535) * (M[1]-M[0])
|
||||
for bname,gf in G_latt_w: Akw[bname][ik,0] += gf.data[iom,:,:].imag.trace()/(-3.1415926535) * (mesh[1]-mesh[0])
|
||||
else:
|
||||
for bname,gf in S: Akw[bname][ik,iom] += gf.data[iom,:,:].imag.trace()/(-3.1415926535)
|
||||
for bname,gf in G_latt_w: Akw[bname][ik,iom] += gf.data[iom,:,:].imag.trace()/(-3.1415926535)
|
||||
Akw[bname][ik,iom] += ik*shift # shift Akw for plotting in xmgrace -- REMOVE
|
||||
|
||||
|
||||
|
|
@ -417,7 +353,7 @@ class SumkDFTTools(SumkDFT):
|
|||
Gproj.zero()
|
||||
tmp = Gproj.copy()
|
||||
for ir in range(self.n_parproj[ishell]):
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold_pc(ik,ir,ishell,bname,S[bname],gf)
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold_pc(ik,ir,ishell,bname,G_latt_w[bname],gf)
|
||||
Gproj += tmp
|
||||
|
||||
# FIXME NEED TO READ IN ROTMAT_ALL FROM PARPROJ SUBGROUP, REPLACE ROTLOC WITH ROTLOC_ALL
|
||||
|
|
@ -427,7 +363,7 @@ class SumkDFTTools(SumkDFT):
|
|||
# for bname,gf in Gproj: Gproj[bname] << self.rotloc(0,gf,direction='toLocal')
|
||||
|
||||
for iom in range(n_om):
|
||||
if (M[iom] > om_minplot) and (M[iom] < om_maxplot):
|
||||
if (mesh[iom] > om_minplot) and (mesh[iom] < om_maxplot):
|
||||
for ish in range(self.shells[ishell]['dim']):
|
||||
for ibn in spn:
|
||||
Akw[ibn][ish,ik,iom] = Gproj[ibn].data[iom,ish,ish].imag/(-3.1415926535)
|
||||
|
|
@ -458,13 +394,13 @@ class SumkDFTTools(SumkDFT):
|
|||
f.write('%s %s\n'%(ik,Akw[ibn][ik,0]))
|
||||
else:
|
||||
for iom in range(n_om):
|
||||
if (M[iom] > om_minplot) and (M[iom] < om_maxplot):
|
||||
if (mesh[iom] > om_minplot) and (mesh[iom] < om_maxplot):
|
||||
if invert_Akw:
|
||||
Akw[ibn][ik,iom] = 1.0/(minAkw-maxAkw)*(Akw[ibn][ik,iom] - maxAkw)
|
||||
if shift > 0.0001:
|
||||
f.write('%s %s\n'%(M[iom],Akw[ibn][ik,iom]))
|
||||
f.write('%s %s\n'%(mesh[iom],Akw[ibn][ik,iom]))
|
||||
else:
|
||||
f.write('%s %s %s\n'%(ik,M[iom],Akw[ibn][ik,iom]))
|
||||
f.write('%s %s %s\n'%(ik,mesh[iom],Akw[ibn][ik,iom]))
|
||||
|
||||
f.write('\n')
|
||||
|
||||
|
|
@ -482,13 +418,13 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
for ik in range(self.n_k):
|
||||
for iom in range(n_om):
|
||||
if (M[iom] > om_minplot) and (M[iom] < om_maxplot):
|
||||
if (mesh[iom] > om_minplot) and (mesh[iom] < om_maxplot):
|
||||
if invert_Akw:
|
||||
Akw[ibn][ish,ik,iom] = 1.0/(minAkw-maxAkw)*(Akw[ibn][ish,ik,iom] - maxAkw)
|
||||
if shift > 0.0001:
|
||||
f.write('%s %s\n'%(M[iom],Akw[ibn][ish,ik,iom]))
|
||||
f.write('%s %s\n'%(mesh[iom],Akw[ibn][ish,ik,iom]))
|
||||
else:
|
||||
f.write('%s %s %s\n'%(ik,M[iom],Akw[ibn][ish,ik,iom]))
|
||||
f.write('%s %s %s\n'%(ik,mesh[iom],Akw[ibn][ish,ik,iom]))
|
||||
|
||||
f.write('\n')
|
||||
|
||||
|
|
@ -511,10 +447,10 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
mu = self.chemical_potential
|
||||
GFStruct_proj = [ [ (sp, range(self.shells[i]['dim'])) for sp in spn ] for i in range(self.n_shells) ]
|
||||
if hasattr(self,"Sigma_imp"):
|
||||
Gproj = [BlockGf(name_block_generator = [ (block,GfImFreq(indices = inner, mesh = self.Sigma_imp[0].mesh)) for block,inner in GFStruct_proj[ish] ], make_copies = False)
|
||||
if hasattr(self,"Sigma_imp_iw"):
|
||||
Gproj = [BlockGf(name_block_generator = [ (block,GfImFreq(indices = inner, mesh = self.Sigma_imp_iw[0].mesh)) for block,inner in GFStruct_proj[ish] ], make_copies = False)
|
||||
for ish in range(self.n_shells)]
|
||||
beta = self.Sigma_imp[0].mesh.beta
|
||||
beta = self.Sigma_imp_iw[0].mesh.beta
|
||||
else:
|
||||
Gproj = [BlockGf(name_block_generator = [ (block,GfImFreq(indices = inner, beta = beta)) for block,inner in GFStruct_proj[ish] ], make_copies = False)
|
||||
for ish in range(self.n_shells)]
|
||||
|
|
@ -524,13 +460,13 @@ class SumkDFTTools(SumkDFT):
|
|||
ikarray=numpy.array(range(self.n_k))
|
||||
|
||||
for ik in mpi.slice_array(ikarray):
|
||||
S = self.lattice_gf_matsubara(ik=ik,mu=mu,beta=beta)
|
||||
S *= self.bz_weights[ik]
|
||||
G_latt_iw = self.lattice_gf(ik=ik,mu=mu,iw_or_w="iw",beta=beta)
|
||||
G_latt_iw *= self.bz_weights[ik]
|
||||
|
||||
for ish in range(self.n_shells):
|
||||
tmp = Gproj[ish].copy()
|
||||
for ir in range(self.n_parproj[ish]):
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold_pc(ik,ir,ish,bname,S[bname],gf)
|
||||
for bname,gf in tmp: tmp[bname] << self.downfold_pc(ik,ir,ish,bname,G_latt_iw[bname],gf)
|
||||
Gproj[ish] += tmp
|
||||
|
||||
#collect data from mpi:
|
||||
|
|
@ -619,7 +555,7 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
# Define mesh for Greens function and the used energy range
|
||||
if (with_Sigma == False):
|
||||
self.omega = numpy.array([round(x.real,12) for x in self.Sigma_imp[0].mesh])
|
||||
self.omega = numpy.array([round(x.real,12) for x in self.Sigma_imp_w[0].mesh])
|
||||
mu = self.chemical_potential
|
||||
n_om = len(self.omega)
|
||||
print "Using omega mesh provided by Sigma."
|
||||
|
|
@ -632,15 +568,15 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
# Truncate Sigma to given omega window
|
||||
for icrsh in range(self.n_corr_shells):
|
||||
Sigma_save = self.Sigma_imp[icrsh].copy()
|
||||
Sigma_save = self.Sigma_imp_w[icrsh].copy()
|
||||
spn = self.spin_block_names[self.corr_shells[icrsh]['SO']]
|
||||
glist = lambda : [ GfReFreq(indices = inner, window=(self.omega[0], self.omega[-1]),n_points=n_om) for block, inner in self.gf_struct_sumk[icrsh]]
|
||||
self.Sigma_imp[icrsh] = BlockGf(name_list = spn, block_list = glist(),make_copies=False)
|
||||
for i,g in self.Sigma_imp[icrsh]:
|
||||
self.Sigma_imp_w[icrsh] = BlockGf(name_list = spn, block_list = glist(),make_copies=False)
|
||||
for i,g in self.Sigma_imp_w[icrsh]:
|
||||
for iL in g.indices:
|
||||
for iR in g.indices:
|
||||
for iom in xrange(n_om):
|
||||
g.data[iom,iL,iR]= Sigma_save[i].data[ioffset+iom,iL,iR]
|
||||
g.data[iom,iL,iR] = Sigma_save[i].data[ioffset+iom,iL,iR] # FIXME IS THIS CLEAN? MANIPULATING data DIRECTLY?
|
||||
|
||||
else:
|
||||
assert n_om is not None, "Number of omega points (n_om) needed!"
|
||||
|
|
@ -684,8 +620,8 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
ikarray = numpy.array(range(self.n_k))
|
||||
for ik in mpi.slice_array(ikarray):
|
||||
unchangesize = all([ self.n_orbitals[ik][isp] == mupat[isp].shape[0] for isp in range(n_inequiv_spin_blocks)])
|
||||
if (not unchangesize):
|
||||
unchangedsize = all([ self.n_orbitals[ik][isp] == mupat[isp].shape[0] for isp in range(n_inequiv_spin_blocks)])
|
||||
if not unchangedsize:
|
||||
# recontruct green functions.
|
||||
S = BlockGf(name_block_generator=[(bln[isp], GfReFreq(indices=range(self.n_orbitals[ik][isp]), window = (self.omega[0], self.omega[-1]), n_points = n_om))
|
||||
for isp in range(n_inequiv_spin_blocks) ], make_copies=False)
|
||||
|
|
@ -707,10 +643,10 @@ class SumkDFTTools(SumkDFT):
|
|||
if (with_Sigma == False):
|
||||
tmp = S.copy() # init temporary storage
|
||||
# form self energy from impurity self energy and double counting term.
|
||||
stmp = self.add_dc()
|
||||
## substract self energy
|
||||
sigma_minus_dc = self.add_dc(iw_or_w="w")
|
||||
# substract self energy
|
||||
for icrsh in xrange(self.n_corr_shells):
|
||||
for sig, gf in tmp: tmp[sig] << self.upfold(ik, icrsh, sig, stmp[icrsh][sig], gf)
|
||||
for sig, gf in tmp: tmp[sig] << self.upfold(ik, icrsh, sig, sigma_minus_dc[icrsh][sig], gf)
|
||||
S -= tmp
|
||||
|
||||
S.invert()
|
||||
|
|
@ -786,7 +722,7 @@ class SumkDFTTools(SumkDFT):
|
|||
|
||||
volcc, volpc = self.cellvolume(self.latticetype, self.latticeconstants, self.latticeangles)
|
||||
|
||||
n_direction,n_q,n_w= self.Pw_optic.shape
|
||||
n_direction, n_q, n_w= self.Pw_optic.shape
|
||||
omegaT = self.omega * beta
|
||||
A0 = numpy.empty((n_direction,n_q), dtype=numpy.float_)
|
||||
q_0 = False
|
||||
|
|
|
|||
|
|
@ -39,7 +39,7 @@ class Symmetry:
|
|||
SP: Flag for spin polarisation.
|
||||
"""
|
||||
|
||||
assert type(hdf_file) == StringType, "hdf_file must be a filename"
|
||||
assert type(hdf_file) == StringType, "Symmetry: hdf_file must be a filename."
|
||||
self.hdf_file = hdf_file
|
||||
things_to_read = ['n_symm','n_atoms','perm','orbits','SO','SP','time_inv','mat','mat_tinv']
|
||||
for it in things_to_read: setattr(self,it,0)
|
||||
|
|
@ -73,8 +73,8 @@ class Symmetry:
|
|||
|
||||
def symmetrize(self,obj):
|
||||
|
||||
assert isinstance(obj,list), "symmetry: obj has to be a list of objects."
|
||||
assert len(obj) == self.n_orbits, "symmetry: obj has to be a list of the same length as defined in the init."
|
||||
assert isinstance(obj,list), "symmetrize: obj has to be a list of objects."
|
||||
assert len(obj) == self.n_orbits, "symmetrize: obj has to be a list of the same length as defined in the init."
|
||||
|
||||
if isinstance(obj[0],BlockGf):
|
||||
symm_obj = [ obj[i].copy() for i in range(len(obj)) ] # here the result is stored, it is a BlockGf!
|
||||
|
|
|
|||
Loading…
Reference in New Issue
Block a user