def update_params(self, d):
allparams = [
('QMC_N_cycles_MAX', 'N_Cycles'),
('NCycles', 'N_Cycles'),
('Hloc', 'H_Local'),
('QuantumNumbers', 'Quantum_Numbers'),
('Length_One_QMC_Cycle', 'Length_Cycle'),
('Number_Warming_Iteration', 'N_Warmup_Cycles'),
('Number_Frequencies_Accumulated', 'N_Frequencies_Accumulated'),
('Global_Move', 'Global_Moves'),
('UseSegmentPicture', 'Use_Segment_Picture'),
('Proba_Move_Insert_Remove_Kink', 'Proba_Insert_Remove'),
('Proba_Move_Move_Kink', 'Proba_Move'),
('OperatorsToAverage', 'Measured_Operators'),
('OpCorrToAverage', 'Measured_Time_Correlators'),
('KeepGF_MC_series', 'Keep_Full_MC_Series'),
('DecorrelationAnalysisG_NFreq', 'Decorrelation_Analysis_G_NFreq'),
('RecordStatisticConfigurations', 'Record_Statistics_Configurations')
]
issue_warning = False
for (old, new) in allparams:
if old in d:
val = d.pop(old)
d.update({new:val})
issue_warning = True
msg = """
**********************************************************************************
Warning: some parameters you used have a different name now and will be
deprecated in future versions. Please check the documentation.
**********************************************************************************
"""
if issue_warning: MPI.report(msg)
def update_params(self, d):
allparams = [
('QMC_N_cycles_MAX', 'N_Cycles'),
('NCycles', 'N_Cycles'),
('Hloc', 'H_Local'),
('QuantumNumbers', 'Quantum_Numbers'),
('Length_One_QMC_Cycle', 'Length_Cycle'),
('Number_Warming_Iteration', 'N_Warmup_Cycles'),
('Number_Frequencies_Accumulated', 'N_Frequencies_Accumulated'),
('Global_Move', 'Global_Moves'),
('UseSegmentPicture', 'Use_Segment_Picture'),
('Proba_Move_Insert_Remove_Kink', 'Proba_Insert_Remove'),
('Proba_Move_Move_Kink', 'Proba_Move'),
('OperatorsToAverage', 'Measured_Operators'),
('OpCorrToAverage', 'Measured_Time_Correlators'),
('KeepGF_MC_series', 'Keep_Full_MC_Series'),
('DecorrelationAnalysisG_NFreq', 'Decorrelation_Analysis_G_NFreq'),
('RecordStatisticConfigurations', 'Record_Statistics_Configurations')
]
issue_warning = False
for (old, new) in allparams:
if old in d:
val = d.pop(old)
d.update({new:val})
issue_warning = True
msg = """
**********************************************************************************
Warning: some parameters you used have a different name now and will be
deprecated in future versions. Please check the documentation.
**********************************************************************************
"""
if issue_warning: MPI.report(msg)
def fitTails(self):
"""Fits the tails using the constant value for the Re Sigma calculated from F=Sigma*G.
Works only for blocks of size one."""
#if (len(self.GFStruct)==2*self.Norb):
if (self.blocssizeone):
spinblocs = [v for v in self.map]
MPI.report("Fitting tails manually")
known_coeff = numpy.zeros([1, 1, 2], numpy.float_)
msh = [x.imag for x in self.G[self.map[spinblocs[0]][0]].mesh]
fit_start = msh[self.Fitting_Frequency_Start]
fit_stop = msh[self.N_Frequencies_Accumulated]
# Fit the tail of G just to get the density
for n, g in self.G:
g.fitTail([[[0, 0, 1]]], 7, fit_start, 2 * fit_stop)
densmat = self.G.density()
for sig1 in spinblocs:
for i in range(self.Norb):
coeff = 0.0
for sig2 in spinblocs:
for j in range(self.Norb):
if (sig1 == sig2):
coeff += self.U[self.offset + i, self.offset +
j] * densmat[self.map[sig1]
[j]][0, 0].real
else:
coeff += self.Up[self.offset + i, self.offset +
j] * densmat[self.map[sig2]
[j]][0, 0].real
known_coeff[0, 0, 1] = coeff
self.Sigma[self.map[sig1][i]].fitTail(
fixed_coef=known_coeff,
order_max=3,
fit_start=fit_start,
fit_stop=fit_stop)
else:
for n, sig in self.Sigma:
known_coeff = numpy.zeros([sig.N1, sig.N2, 1], numpy.float_)
msh = [x.imag for x in sig.mesh]
fit_start = msh[self.Fitting_Frequency_Start]
fit_stop = msh[self.N_Frequencies_Accumulated]
sig.fitTail(fixed_coef=known_coeff,
order_max=3,
fit_start=fit_start,
fit_stop=fit_stop)
def __repack(self):
"""Calls the h5repack routine, in order to reduce the file size of the hdf5 archive.
Should only be used BEFORE the first invokation of HDF_Archive in the program, otherwise
the hdf5 linking is broken!!!"""
import subprocess
if not (MPI.IS_MASTER_NODE()): return
MPI.report("Repacking the file %s"%self.HDFfile)
retcode = subprocess.call(["h5repack","-i%s"%self.HDFfile, "-otemphgfrt.h5"])
if (retcode!=0):
MPI.report("h5repack failed!")
else:
subprocess.call(["mv","-f","temphgfrt.h5","%s"%self.HDFfile])
def read_input_from_HDF(self, SubGrp, thingstoread, optionalthings=[]):
"""
Reads data from the HDF file
"""
retval = True
# init variables on all nodes:
for it in thingstoread:
exec "self.%s = 0" % it
for it in optionalthings:
exec "self.%s = 0" % it
if MPI.IS_MASTER_NODE():
ar = HDF_Archive(self.HDFfile, "a")
if SubGrp in ar:
# first read the necessary things:
for it in thingstoread:
if it in ar[SubGrp]:
exec "self.%s = ar['%s']['%s']" % (it, SubGrp, it)
else:
MPI.report("Loading %s failed!" % it)
retval = False
if (retval) and (len(optionalthings) > 0):
# if necessary things worked, now read optional things:
retval = {}
for it in optionalthings:
if it in ar[SubGrp]:
exec "self.%s = ar['%s']['%s']" % (it, SubGrp, it)
retval["%s" % it] = True
else:
retval["%s" % it] = False
else:
MPI.report("Loading failed: No %s subgroup in HDF5!" % SubGrp)
retval = False
del ar
# now do the broadcasting:
for it in thingstoread:
exec "self.%s = MPI.bcast(self.%s)" % (it, it)
for it in optionalthings:
exec "self.%s = MPI.bcast(self.%s)" % (it, it)
retval = MPI.bcast(retval)
return retval
def __repack(self):
"""Calls the h5repack routine, in order to reduce the file size of the hdf5 archive.
Should only be used BEFORE the first invokation of HDF_Archive in the program, otherwise
the hdf5 linking is broken!!!"""
import subprocess
if not (MPI.IS_MASTER_NODE()): return
MPI.report("Repacking the file %s" % self.HDFfile)
retcode = subprocess.call(
["h5repack", "-i%s" % self.HDFfile, "-otemphgfrt.h5"])
if (retcode != 0):
MPI.report("h5repack failed!")
else:
subprocess.call(["mv", "-f", "temphgfrt.h5", "%s" % self.HDFfile])
def Self_Consistency(self) :
S.Transform_SymmetryBasis_toRealSpace (IN= S.Sigma, OUT = Sigma) # Embedding
# Computes sum over BZ and returns density
F = lambda mu : SK(mu = mu,Sigma = Sigma, Field = None ,Res = G).total_density()/4
if Density_Required :
self.Chemical_potential = Dichotomy.Dichotomy(Function = F,
xinit = self.Chemical_potential, yvalue =Density_Required,
Precision_on_y = 0.01, Delta_x=0.5, MaxNbreLoop = 100,
xname="Chemical_Potential", yname= "Total Density",
verbosity = 3)[0]
else:
MPI.report("Total density = %.3f"%F(self.Chemical_potential))
S.Transform_RealSpace_to_SymmetryBasis (IN = G, OUT = S.G) # Extraction
S.G0 = inverse(S.Sigma + inverse(S.G)) # Finally get S.G0
def run(self,N_Loops, Mixing_Coefficient = 0.5, MaxTime = 0 ):
r"""
Run the DMFT Loop with the following algorithm ::
while STOP_CONDITION :
self.Self_Consistency()
for solver in Solver_List : S.solve()
self.PostSolver() # defaults : does nothing
where STOP_CONDITION is determined by the number of iterations.
:param N_Loops: Maximum number of iteration of the loop
:param Mixing_Coefficient:
:param MaxTime: Maximum time of the loop.
"""
# Set up the signal
# MPI.report("DMFTlab Job PID = %s"%os.getpid())
# Set the signal handler and a 5-second alarm
signal.signal(signal.SIGALRM, self.handler)
signal.alarm(MaxTime)
should_continue = True
while (should_continue):
MPI.report("------ Node : %d -------- Iteration Number = %d"%(MPI.rank,self.Iteration_Number))
self.Self_Consistency()
# call all solvers
for n,sol in enumerate(self.SolverList) :
if hasattr(self,"Chemical_potential") : sol.Chemical_potential=self.Chemical_potential
sol.Iteration_Number=self.Iteration_Number
sol.Solve()
sol.Sigma = sol.Sigma * Mixing_Coefficient + sol.Sigma_Old * (1-Mixing_Coefficient)
# post-solver processing
self.PostSolver()
self.Iteration_Number +=1
should_continue = self.__should_continue(N_Loops)
# end of the while loop
MPI.report("----------- END of DMFT_Loop ----------------")
MPI.barrier()
def fitTails(self):
"""Fits the tails using the constant value for the Re Sigma calculated from F=Sigma*G.
Works only for blocks of size one."""
#if (len(self.GFStruct)==2*self.Norb):
if (self.blocssizeone):
spinblocs = [v for v in self.map]
MPI.report("Fitting tails manually")
known_coeff = numpy.zeros([1,1,2],numpy.float_)
msh = [x.imag for x in self.G[self.map[spinblocs[0]][0]].mesh ]
fit_start = msh[self.Fitting_Frequency_Start]
fit_stop = msh[self.N_Frequencies_Accumulated]
# Fit the tail of G just to get the density
for n,g in self.G:
g.fitTail([[[0,0,1]]],7,fit_start,2*fit_stop)
densmat = self.G.density()
for sig1 in spinblocs:
for i in range(self.Norb):
coeff = 0.0
for sig2 in spinblocs:
for j in range(self.Norb):
if (sig1==sig2):
coeff += self.U[self.offset+i,self.offset+j] * densmat[self.map[sig1][j]][0,0].real
else:
coeff += self.Up[self.offset+i,self.offset+j] * densmat[self.map[sig2][j]][0,0].real
known_coeff[0,0,1] = coeff
self.Sigma[self.map[sig1][i]].fitTail(fixed_coef = known_coeff, order_max = 3, fit_start = fit_start, fit_stop = fit_stop)
else:
for n,sig in self.Sigma:
known_coeff = numpy.zeros([sig.N1,sig.N2,1],numpy.float_)
msh = [x.imag for x in sig.mesh]
fit_start = msh[self.Fitting_Frequency_Start]
fit_stop = msh[self.N_Frequencies_Accumulated]
sig.fitTail(fixed_coef = known_coeff, order_max = 3, fit_start = fit_start, fit_stop = fit_stop)
def Self_Consistency(self):
S.Transform_SymmetryBasis_toRealSpace(IN=S.Sigma,
OUT=Sigma) # Embedding
# Computes sum over BZ and returns density
F = lambda mu: SK(mu=mu, Sigma=Sigma, Field=None, Res=G).total_density(
) / 4
if Density_Required:
self.Chemical_potential = Dichotomy.Dichotomy(
Function=F,
xinit=self.Chemical_potential,
yvalue=Density_Required,
Precision_on_y=0.01,
Delta_x=0.5,
MaxNbreLoop=100,
xname="Chemical_Potential",
yname="Total Density",
verbosity=3)[0]
else:
MPI.report("Total density = %.3f" % F(self.Chemical_potential))
S.Transform_RealSpace_to_SymmetryBasis(IN=G, OUT=S.G) # Extraction
S.G0 = inverse(S.Sigma + inverse(S.G)) # Finally get S.G0
def __init__(self, HDFfile, mu = 0.0, hfield = 0.0, UseLDABlocs = False, LDAdata = 'SumK_LDA', Symmcorrdata = 'SymmCorr',
ParProjdata = 'SumK_LDA_ParProj', Symmpardata = 'SymmPar', Bandsdata = 'SumK_LDA_Bands'):
"""
Initialises the class from data previously stored into an HDF5
"""
if not (type(HDFfile)==StringType):
MPI.report("Give a string for the HDF5 filename to read the input!")
else:
self.HDFfile = HDFfile
self.LDAdata = LDAdata
self.ParProjdata = ParProjdata
self.Bandsdata = Bandsdata
self.Symmpardata = Symmpardata
self.Symmcorrdata = Symmcorrdata
self.blocnames= [ ['up','down'], ['ud'] ]
self.NspinblocsGF = [2,1]
self.Gupf = None
self.hfield = hfield
# read input from HDF:
thingstoread = ['EnergyUnit','Nk','k_dep_projection','SP','SO','charge_below','Density_Required',
'symm_op','N_shells','shells','N_corr_shells','corr_shells','use_rotations','rotmat','rotmat_timeinv','Nreps',
'dim_reps','T','N_Orbitals','Proj_Mat','BZ_weights','Hopping']
optionalthings = ['GFStruct_Solver','mapinv','map','Chemical_Potential','dc_imp','DCenerg','deg_shells']
#ar=HDF_Archive(self.HDFfile,'a')
#del ar
self.retval = self.read_input_from_HDF(SubGrp=self.LDAdata,thingstoread=thingstoread,optionalthings=optionalthings)
#ar=HDF_Archive(self.HDFfile,'a')
#del ar
if (self.SO) and (abs(self.hfield)>0.000001):
self.hfield=0.0
MPI.report("For SO, the external magnetic field is not implemented, setting it to 0!!")
self.inequiv_shells(self.corr_shells) # determine the number of inequivalent correlated shells
# field to convert blocnames to indices
self.names_to_ind = [{}, {}]
for ibl in range(2):
for inm in range(self.NspinblocsGF[ibl]):
self.names_to_ind[ibl][self.blocnames[ibl][inm]] = inm * self.SP #(self.Nspinblocs-1)
# GF structure used for the local things in the k sums
self.GFStruct_corr = [ [ (al, range( self.corr_shells[i][3])) for al in self.blocnames[self.corr_shells[i][4]] ]
for i in xrange(self.N_corr_shells) ]
if not (self.retval['GFStruct_Solver']):
# No GFStruct was stored in HDF, so first set a standard one:
self.GFStruct_Solver = [ [ (al, range( self.corr_shells[self.invshellmap[i]][3]) )
for al in self.blocnames[self.corr_shells[self.invshellmap[i]][4]] ]
for i in xrange(self.N_inequiv_corr_shells) ]
self.map = [ {} for i in xrange(self.N_inequiv_corr_shells) ]
self.mapinv = [ {} for i in xrange(self.N_inequiv_corr_shells) ]
for i in xrange(self.N_inequiv_corr_shells):
for al in self.blocnames[self.corr_shells[self.invshellmap[i]][4]]:
self.map[i][al] = [al for j in range( self.corr_shells[self.invshellmap[i]][3] ) ]
self.mapinv[i][al] = al
if not (self.retval['dc_imp']):
# init the double counting:
self.__initDC()
if not (self.retval['Chemical_Potential']):
self.Chemical_Potential = mu
if not (self.retval['deg_shells']):
self.deg_shells = [ [] for i in range(self.N_inequiv_corr_shells)]
if self.symm_op:
#MPI.report("Do the init for symm:")
self.Symm_corr = Symmetry(HDFfile,subgroup=self.Symmcorrdata)
# determine the smallest blocs, if wanted:
if (UseLDABlocs): dm=self.analyse_BS()
# now save things again to HDF5:
if (MPI.IS_MASTER_NODE()):
ar=HDF_Archive(self.HDFfile,'a')
ar[self.LDAdata]['hfield'] = self.hfield
del ar
self.save()
def Solve(self):
""" Solve the impurity problem """
# Find if an operator is in oplist
def mysearch(op):
l = [ k for (k,v) in OPdict.items() if (v-op).is_zero()]
assert len(l) <=1
return l[0] if l else None
# Same but raises an error if pb
def myfind(op):
r = mysearch(op)
if r==None : raise "Operator %s can not be found by myfind !"%r
return r
# For backward compatibility
self.update_params(self.__dict__)
# Test all a parameters before solutions
MPI.report(Parameters.check(self.__dict__,self.Required,self.Optional))
# We have to add the Hamiltonian the epsilon part of G0
if type(self.H_Local) != type(Operator()) : raise "H_Local is not an operator"
H = self.H_Local
for a,alpha_list in self.GFStruct :
for mu in alpha_list :
for nu in alpha_list :
H += real(self.G0[a]._tail[2][mu,nu]) * Cdag(a,mu)*C(a,nu)
OPdict = {"Hamiltonian": H}
MPI.report("Hamiltonian with Eps0 term : ",H)
# First separate the quantum Numbers that are operators and those which are symmetries.
QuantumNumberOperators = dict( (n,op) for (n,op) in self.Quantum_Numbers.items() if type(op) == type(Operator()))
QuantumNumberSymmetries = dict( (n,op) for (n,op) in self.Quantum_Numbers.items() if type(op) != type(Operator()))
# Check that the quantum numbers commutes with the Hamiltonian
for name,op in QuantumNumberOperators.items():
assert Commutator(self.H_Local ,op).is_zero(), "One quantum number is not commuting with Hamiltonian"
OPdict[name]=op
# Complete the OPdict with the fundamental operators
OPdict, nf, nb, SymChar, NameOpFundamentalList = Operators.Complete_OperatorsList_with_Fundamentals(OPdict)
# Add the operators to be averaged in OPdict and prepare the list for the C-code
self.Measured_Operators_Results = {}
self.twice_defined_Ops = {}
self.Operators_To_Average_List = []
for name, op in self.Measured_Operators.items():
opn = mysearch(op)
if opn == None :
OPdict[name] = op
self.Measured_Operators_Results[name] = 0.0
self.Operators_To_Average_List.append(name)
else:
MPI.report("Operator %s already defined as %s, using this instead for measuring"%(name,opn))
self.twice_defined_Ops[name] = opn
self.Measured_Operators_Results[opn] = 0.0
if opn not in self.Operators_To_Average_List: self.Operators_To_Average_List.append(opn)
# Time correlation functions are added
self.OpCorr_To_Average_List = []
for name, op in self.Measured_Time_Correlators.items():
opn = mysearch(op[0])
if opn == None :
OPdict[name] = op[0]
self.OpCorr_To_Average_List.append(name)
else:
MPI.report("Operator %s already defined as %s, using this instead for measuring"%(name,opn))
if opn not in self.OpCorr_To_Average_List: self.OpCorr_To_Average_List.append(opn)
# Create storage for data:
Nops = len(self.OpCorr_To_Average_List)
f = lambda L : GFBloc_ImTime(Indices= [0], Beta = self.Beta, NTimeSlices=L )
if (Nops>0):
self.Measured_Time_Correlators_Results = GF(Name_Block_Generator = [ ( n,f(self.Measured_Time_Correlators[n][1]) ) for n in self.Measured_Time_Correlators], Copy=False)
else:
self.Measured_Time_Correlators_Results = GF(Name_Block_Generator = [ ( 'OpCorr',f(2) ) ], Copy=False)
# Take care of the global moves
# First, given a function (a,alpha,dagger) -> (a', alpha', dagger')
# I construct a function on fundamental operators
def Map_GM_to_Fund_Ops( GM ) :
def f(fop) :
a,alpha, dagger = fop.name + (fop.dag,)
ap,alphap,daggerp = GM((a,alpha,dagger))
return Cdag(ap,alphap) if daggerp else C(ap,alphap)
return f
# Complete the OpList so that it is closed under the global moves
while 1:
added_something = False
for n,(proba,GM) in enumerate(self.Global_Moves):
# F is a function that map all operators according to the global move
F = Extend_Function_on_Fundamentals(Map_GM_to_Fund_Ops(GM))
# Make sure that OPdict is complete, i.e. all images of OPdict operators are in OPdict
for name,op in OPdict.items() :
op_im = F(op)
if mysearch(op_im)==None :
# find the key and put in in the dictionnary
i=0
while 1:
new_name = name + 'GM' + i*'_' + "%s"%n
if new_name not in OPdict : break
added_something = True
OPdict[new_name] = op_im
# break the while loop
if not added_something: break
# Now I have all operators, I make the transcription of the global moves
self.Global_Moves_Mapping_List = []
for n,(proba,GM) in enumerate(self.Global_Moves):
F = Extend_Function_on_Fundamentals(Map_GM_to_Fund_Ops(GM))
m = {}
for name,op in OPdict.items() :
op_im = F(op)
n1,n2 = myfind(op),myfind(op_im)
m[n1] = n2
name = "%s"%n
self.Global_Moves_Mapping_List.append((proba,m,name))
#MPI.report ("Global_Moves_Mapping_List", self.Global_Moves_Mapping_List)
# Now add the operator for F calculation if needed
if self.Use_F :
Hloc_WithoutQuadratic = self.H_Local.RemoveQuadraticTerms()
for n,op in OPdict.items() :
if op.is_Fundamental():
op2 = Commutator(Hloc_WithoutQuadratic,op)
if not mysearch(op2) : OPdict["%s_Comm_Hloc"%n] = op2
# All operators have real coefficients. Check this and remove the 0j term
# since the C++ expects operators with real numbers
for n,op in OPdict.items(): op.make_coef_real_and_check()
# Transcription of operators for C++
Oplist2 = Operators.Transcribe_OpList_for_C(OPdict)
SymList = [sym for (n,sym) in SymChar.items() if n in QuantumNumberSymmetries]
self.H_diag = C_Module.Hloc(nf,nb,Oplist2,QuantumNumberOperators,SymList,self.Quantum_Numbers_Selection,0)
# Create the C_Cag_Ops array which describes the grouping of (C,Cdagger) operator
# for the MonteCarlo moves : (a, alpha) block structure [ [ (C_name, Cdag_name)]]
self.C_Cdag_Ops = [ [ (myfind(C(a,alpha)), myfind(Cdag(a,alpha))) for alpha in al ] for a,al in self.GFStruct]
# Define G0_inv and correct it to have G0 to have perfect 1/omega behavior
self.G0_inv = inverse(self.G0)
Delta = self.G0_inv.Delta()
for n,g in self.G0_inv:
assert(g.N1==g.N2)
identity=numpy.identity(g.N1)
self.G0[n] <<= GF_Initializers.A_Omega_Plus_B(identity, g._tail[0])
self.G0[n] -= Delta[n]
#self.G0[n] <<= iOmega_n + g._tail[0] - Delta[n]
self.G0_inv <<= self.G0
self.G0.invert()
# Construct the function in tau
f = lambda g,L : GFBloc_ImTime(Indices= g.Indices, Beta = g.Beta, NTimeSlices=L )
self.Delta_tau = GF(Name_Block_Generator = [ (n,f(g,self.N_Time_Slices_Delta) ) for n,g in self.G], Copy=False, Name='D')
self.G_tau = GF(Name_Block_Generator = [ (n,f(g,self.N_Time_Slices_Gtau) ) for n,g in self.G], Copy=False, Name='G')
self.F_tau = GF(Name_Block_Generator = self.G_tau, Copy=True, Name='F')
for (i,gt) in self.Delta_tau : gt.setFromInverseFourierOf(Delta[i])
MPI.report("Inv Fourier done")
if (self.Legendre_Accumulation):
self.G_Legendre = GF(Name_Block_Generator = [ (n,GFBloc_ImLegendre(Indices=g.Indices, Beta=g.Beta, NLegendreCoeffs=self.N_Legendre_Coeffs) ) for n,g in self.G], Copy=False, Name='Gl')
else:
self.G_Legendre = GF(Name_Block_Generator = [ (n,GFBloc_ImLegendre(Indices=[1], Beta=g.Beta, NLegendreCoeffs=1) ) for n,g in self.G], Copy=False, Name='Gl') # G_Legendre must not be empty but is not needed in this case. So I make it as small as possible.
# Starting the C++ code
self.Sigma_Old <<= self.Sigma
C_Module.MC_solve(self.__dict__ ) # C++ solver
# Compute G on Matsubara axis possibly fitting the tail
if self.Legendre_Accumulation:
for s,g in self.G:
identity=numpy.zeros([g.N1,g.N2],numpy.float)
for i,m in enumerate (g._IndicesL):
for j,n in enumerate (g._IndicesR):
if m==n: identity[i,j]=1
self.G_Legendre[s].enforce_discontinuity(identity) # set the known tail
g <<= LegendreToMatsubara(self.G_Legendre[s])
else:
if (self.Time_Accumulation):
for name, g in self.G_tau:
identity=numpy.zeros([g.N1,g.N2],numpy.float)
for i,m in enumerate (g._IndicesL):
for j,n in enumerate (g._IndicesR):
if m==n: identity[i,j]=1
g._tail.zero()
g._tail[1] = identity
self.G[name].setFromFourierOf(g)
# This is very sick... but what can we do???
self.Sigma <<= self.G0_inv - inverse(self.G)
self.fitTails()
self.G <<= inverse(self.G0_inv - self.Sigma)
# Now find the self-energy
self.Sigma <<= self.G0_inv - inverse(self.G)
MPI.report("Solver %(Name)s has ended."%self.__dict__)
# for operator averages: if twice defined operator, rename output:
for op1,op2 in self.twice_defined_Ops.items():
self.Measured_Operators_Results[op1] = self.Measured_Operators_Results[op2]
for op1,op2 in self.twice_defined_Ops.items():
if op2 in self.Measured_Operators_Results.keys(): del self.Measured_Operators_Results[op2]
if self.Use_F :
for (n,f) in self.F: f.setFromFourierOf(self.F_tau[n])
self.G2 = self.G0 + self.G0 * self.F
self.Sigma2 = self.F * inverse(self.G2)
def convert_DMFT_input(self):
"""
Reads the input files, and stores the data in the HDFfile
"""
if not (MPI.IS_MASTER_NODE()): return # do it only on master:
MPI.report("Reading input from %s..."%self.LDA_file)
# Read and write only on Master!!!
# R is a generator : each R.Next() will return the next number in the file
R = Read_Fortran_File(self.LDA_file)
try:
EnergyUnit = R.next() # read the energy convertion factor
Nk = int(R.next()) # read the number of k points
k_dep_projection = 1
SP = int(R.next()) # flag for spin-polarised calculation
SO = int(R.next()) # flag for spin-orbit calculation
charge_below = R.next() # total charge below energy window
Density_Required = R.next() # total density required, for setting the chemical potential
symm_op = 1 # Use symmetry groups for the k-sum
# the information on the non-correlated shells is not important here, maybe skip:
N_shells = int(R.next()) # number of shells (e.g. Fe d, As p, O p) in the unit cell,
# corresponds to index R in formulas
# now read the information about the shells:
shells = [ [ int(R.next()) for i in range(4) ] for icrsh in range(N_shells) ] # reads iatom, sort, l, dim
N_corr_shells = int(R.next()) # number of corr. shells (e.g. Fe d, Ce f) in the unit cell,
# corresponds to index R in formulas
# now read the information about the shells:
corr_shells = [ [ int(R.next()) for i in range(6) ] for icrsh in range(N_corr_shells) ] # reads iatom, sort, l, dim, SO flag, irep
self.inequiv_shells(corr_shells) # determine the number of inequivalent correlated shells, has to be known for further reading...
use_rotations = 1
rotmat = [numpy.identity(corr_shells[icrsh][3],numpy.complex_) for icrsh in xrange(N_corr_shells)]
# read the matrices
rotmat_timeinv = [0 for i in range(N_corr_shells)]
for icrsh in xrange(N_corr_shells):
for i in xrange(corr_shells[icrsh][3]): # read real part:
for j in xrange(corr_shells[icrsh][3]):
rotmat[icrsh][i,j] = R.next()
for i in xrange(corr_shells[icrsh][3]): # read imaginary part:
for j in xrange(corr_shells[icrsh][3]):
rotmat[icrsh][i,j] += 1j * R.next()
if (SP==1): # read time inversion flag:
rotmat_timeinv[icrsh] = int(R.next())
# Read here the infos for the transformation of the basis:
Nreps = [1 for i in range(self.N_inequiv_corr_shells)]
dim_reps = [0 for i in range(self.N_inequiv_corr_shells)]
T = []
for icrsh in range(self.N_inequiv_corr_shells):
Nreps[icrsh] = int(R.next()) # number of representatives ("subsets"), e.g. t2g and eg
dim_reps[icrsh] = [int(R.next()) for i in range(Nreps[icrsh])] # dimensions of the subsets
# The transformation matrix:
# it is of dimension 2l+1, if no SO, and 2*(2l+1) with SO!!
#T = []
#for ish in xrange(self.N_inequiv_corr_shells):
ll = 2*corr_shells[self.invshellmap[icrsh]][2]+1
lmax = ll * (corr_shells[self.invshellmap[icrsh]][4] + 1)
T.append(numpy.zeros([lmax,lmax],numpy.complex_))
# now read it from file:
for i in xrange(lmax):
for j in xrange(lmax):
T[icrsh][i,j] = R.next()
for i in xrange(lmax):
for j in xrange(lmax):
T[icrsh][i,j] += 1j * R.next()
# Spin blocks to be read:
Nspinblocs = SP + 1 - SO # number of spins to read for Norbs and Ham, NOT Projectors
# read the list of N_Orbitals for all k points
N_Orbitals = [ [0 for isp in range(Nspinblocs)] for ik in xrange(Nk)]
for isp in range(Nspinblocs):
for ik in xrange(Nk):
N_Orbitals[ik][isp] = int(R.next())
#print N_Orbitals
# Initialise the projectors:
Proj_Mat = [ [ [numpy.zeros([corr_shells[icrsh][3], N_Orbitals[ik][isp]], numpy.complex_)
for icrsh in range (N_corr_shells)]
for isp in range(Nspinblocs)]
for ik in range(Nk) ]
# Read the projectors from the file:
for ik in xrange(Nk):
for icrsh in range(N_corr_shells):
no = corr_shells[icrsh][3]
# first Real part for BOTH spins, due to conventions in dmftproj:
for isp in range(Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i,j] = R.next()
# now Imag part:
for isp in range(Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i,j] += 1j * R.next()
# now define the arrays for weights and hopping ...
BZ_weights = numpy.ones([Nk],numpy.float_)/ float(Nk) # w(k_index), default normalisation
Hopping = [ [numpy.zeros([N_Orbitals[ik][isp],N_Orbitals[ik][isp]],numpy.complex_)
for isp in range(Nspinblocs)] for ik in xrange(Nk) ]
# weights in the file
for ik in xrange(Nk) : BZ_weights[ik] = R.next()
# if the sum over spins is in the weights, take it out again!!
sm = sum(BZ_weights)
BZ_weights[:] /= sm
# Grab the H
# we use now the convention of a DIAGONAL Hamiltonian!!!!
for isp in range(Nspinblocs):
for ik in xrange(Nk) :
no = N_Orbitals[ik][isp]
for i in xrange(no):
Hopping[ik][isp][i,i] = R.next() * EnergyUnit
#keep some things that we need for reading parproj:
self.N_shells = N_shells
self.shells = shells
self.N_corr_shells = N_corr_shells
self.corr_shells = corr_shells
self.Nspinblocs = Nspinblocs
self.N_Orbitals = N_Orbitals
self.Nk = Nk
self.SO = SO
self.SP = SP
self.EnergyUnit = EnergyUnit
except StopIteration : # a more explicit error if the file is corrupted.
raise "SumK_LDA : reading file HMLT_file failed!"
R.close()
#print Proj_Mat[0]
#-----------------------------------------
# Store the input into HDF5:
ar = HDF_Archive(self.HDFfile,'a')
if not (self.LDASubGrp in ar): ar.create_group(self.LDASubGrp)
# The subgroup containing the data. If it does not exist, it is created.
# If it exists, the data is overwritten!!!
ar[self.LDASubGrp]['EnergyUnit'] = EnergyUnit
ar[self.LDASubGrp]['Nk'] = Nk
ar[self.LDASubGrp]['k_dep_projection'] = k_dep_projection
ar[self.LDASubGrp]['SP'] = SP
ar[self.LDASubGrp]['SO'] = SO
ar[self.LDASubGrp]['charge_below'] = charge_below
ar[self.LDASubGrp]['Density_Required'] = Density_Required
ar[self.LDASubGrp]['symm_op'] = symm_op
ar[self.LDASubGrp]['N_shells'] = N_shells
ar[self.LDASubGrp]['shells'] = shells
ar[self.LDASubGrp]['N_corr_shells'] = N_corr_shells
ar[self.LDASubGrp]['corr_shells'] = corr_shells
ar[self.LDASubGrp]['use_rotations'] = use_rotations
ar[self.LDASubGrp]['rotmat'] = rotmat
ar[self.LDASubGrp]['rotmat_timeinv'] = rotmat_timeinv
ar[self.LDASubGrp]['Nreps'] = Nreps
ar[self.LDASubGrp]['dim_reps'] = dim_reps
ar[self.LDASubGrp]['T'] = T
ar[self.LDASubGrp]['N_Orbitals'] = N_Orbitals
ar[self.LDASubGrp]['Proj_Mat'] = Proj_Mat
ar[self.LDASubGrp]['BZ_weights'] = BZ_weights
ar[self.LDASubGrp]['Hopping'] = Hopping
del ar
# Symmetries are used,
# Now do the symmetries for correlated orbitals:
self.read_Symmetry_input(orbits=corr_shells,symmfile=self.Symm_file,SymmSubGrp=self.SymmSubGrp,SO=SO,SP=SP)
def Solve(self,Iteration_Number=1,Test_Convergence=0.0001):
"""Calculation of the impurity Greens function using Hubbard-I"""
# Test all a parameters before solutions
print Parameters.check(self.__dict__,self.Required,self.Optional)
#Solver_Base.Solve(self,is_last_iteration,Iteration_Number,Test_Convergence)
if self.Converged :
MPI.report("Solver %(Name)s has already converted: SKIPPING"%self.__dict__)
return
self.__save_eal('eal.dat',Iteration_Number)
MPI.report( "Starting Fortran solver %(Name)s"%self.__dict__)
self.Sigma_Old <<= self.Sigma
self.G_Old <<= self.G
# call the fortran solver:
temp = 1.0/self.Beta
gf,tail,self.atocc,self.atmag = gf_hi_fullu(e0f=self.ealmat, ur=self.ur, umn=self.umn, ujmn=self.ujmn,
zmsb=self.zmsb, nmom=self.Nmoments, ns=self.Nspin, temp=temp, verbosity = self.Verbosity)
#self.sig = sigma_atomic_fullu(gf=self.gf,e0f=self.eal,zmsb=self.zmsb,ns=self.Nspin,nlm=self.Nlm)
if (self.Verbosity==0):
# No fortran output, so give basic results here
MPI.report("Atomic occupancy in Hubbard I Solver : %s"%self.atocc)
MPI.report("Atomic magn. mom. in Hubbard I Solver : %s"%self.atmag)
# transfer the data to the GF class:
if (self.UseSpinOrbit):
nlmtot = self.Nlm*2 # only one block in this case!
else:
nlmtot = self.Nlm
M={}
isp=-1
for a,al in self.GFStruct:
isp+=1
#M[a] = gf[isp*self.Nlm:(isp+1)*self.Nlm,isp*self.Nlm:(isp+1)*self.Nlm,:]
M[a] = gf[isp*nlmtot:(isp+1)*nlmtot,isp*nlmtot:(isp+1)*nlmtot,:]
for i in range(min(self.Nmoments,10)):
self.tailtempl[a][i+1].array[:] = tail[i][isp*nlmtot:(isp+1)*nlmtot,isp*nlmtot:(isp+1)*nlmtot]
glist = lambda : [ GFBloc_ImFreq(Indices = al, Beta = self.Beta, NFreqMatsubara = self.Nmsb, Data=M[a], Tail=self.tailtempl[a])
for a,al in self.GFStruct]
self.G = GF(NameList = self.a_list, BlockList = glist(),Copy=False)
# Self energy:
self.G0 <<= GF_Initializers.A_Omega_Plus_B(A=1,B=0.0)
M = [ self.ealmat[isp*nlmtot:(isp+1)*nlmtot,isp*nlmtot:(isp+1)*nlmtot] for isp in range((2*self.Nlm)/nlmtot) ]
self.G0 -= M
self.Sigma <<= self.G0 - inverse(self.G)
# invert G0
self.G0.invert()
def test_distance(G1,G2, dist) :
def f(G1,G2) :
print abs(G1._data.array - G2._data.array)
dS = max(abs(G1._data.array - G2._data.array).flatten())
aS = max(abs(G1._data.array).flatten())
return dS <= aS*dist
return reduce(lambda x,y : x and y, [f(g1,g2) for (i1,g1),(i2,g2) in izip(G1,G2)])
MPI.report("\nChecking Sigma for convergence...\nUsing tolerance %s"%Test_Convergence)
self.Converged = test_distance(self.Sigma,self.Sigma_Old,Test_Convergence)
if self.Converged :
MPI.report("Solver HAS CONVERGED")
else :
MPI.report("Solver has not yet converged")
def read_Symmetry_input(self,orbits,symmfile,SymmSubGrp,SO,SP):
"""
Reads input for the symmetrisations from symmfile, which is case.sympar or case.symqmc.
"""
if not (MPI.IS_MASTER_NODE()): return
MPI.report("Reading symmetry input from %s..."%symmfile)
N_orbits = len(orbits)
R=Read_Fortran_File(symmfile)
try:
Ns = int(R.next()) # Number of symmetry operations
Natoms = int(R.next()) # number of atoms involved
perm = [ [int(R.next()) for i in xrange(Natoms)] for j in xrange(Ns) ] # list of permutations of the atoms
if SP:
timeinv = [ int(R.next()) for j in xrange(Ns) ] # timeinversion for SO xoupling
else:
timeinv = [ 0 for j in xrange(Ns) ]
# Now read matrices:
mat = []
for iNs in xrange(Ns):
mat.append( [ numpy.zeros([orbits[orb][3], orbits[orb][3]],numpy.complex_) for orb in xrange(N_orbits) ] )
for orb in range(N_orbits):
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat[iNs][orb][i,j] = R.next() # real part
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat[iNs][orb][i,j] += 1j * R.next() # imaginary part
# determine the inequivalent shells:
#SHOULD BE FINALLY REMOVED, PUT IT FOR ALL ORBITALS!!!!!
#self.inequiv_shells(orbits)
mat_tinv = [numpy.identity(orbits[orb][3],numpy.complex_)
for orb in range(N_orbits)]
if ((SO==0) and (SP==0)):
# here we need an additional time inversion operation, so read it:
for orb in range(N_orbits):
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat_tinv[orb][i,j] = R.next() # real part
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat_tinv[orb][i,j] += 1j * R.next() # imaginary part
except StopIteration : # a more explicit error if the file is corrupted.
raise "Symmetry : reading file failed!"
R.close()
# Save it to the HDF:
ar=HDF_Archive(self.HDFfile,'a')
if not (SymmSubGrp in ar): ar.create_group(SymmSubGrp)
thingstowrite = ['Ns','Natoms','perm','orbits','SO','SP','timeinv','mat','mat_tinv']
for it in thingstowrite: exec "ar['%s']['%s'] = %s"%(SymmSubGrp,it,it)
del ar
def convert_Parproj_input(self,
ParProjSubGrp='SumK_LDA_ParProj',
SymmParSubGrp='SymmPar'):
"""
Reads the input for the partial charges projectors from case.parproj, and stores it in the SymmParSubGrp
group in the HDF5.
"""
if not (MPI.IS_MASTER_NODE()): return
self.ParProjSubGrp = ParProjSubGrp
self.SymmParSubGrp = SymmParSubGrp
MPI.report("Reading parproj input from %s..." % self.Parproj_file)
Dens_Mat_below = [[
numpy.zeros([self.shells[ish][3], self.shells[ish][3]],
numpy.complex_) for ish in range(self.N_shells)
] for isp in range(self.Nspinblocs)]
R = Read_Fortran_File(self.Parproj_file)
#try:
N_parproj = [int(R.next()) for i in range(self.N_shells)]
# Initialise P, here a double list of matrices:
Proj_Mat_pc = [[[[
numpy.zeros([self.shells[ish][3], self.N_Orbitals[ik][isp]],
numpy.complex_) for ir in range(N_parproj[ish])
] for ish in range(self.N_shells)] for isp in range(self.Nspinblocs)]
for ik in range(self.Nk)]
rotmat_all = [
numpy.identity(self.shells[ish][3], numpy.complex_)
for ish in xrange(self.N_shells)
]
rotmat_all_timeinv = [0 for i in range(self.N_shells)]
for ish in range(self.N_shells):
#print ish
# read first the projectors for this orbital:
for ik in xrange(self.Nk):
for ir in range(N_parproj[ish]):
for isp in range(self.Nspinblocs):
for i in xrange(
self.shells[ish][3]): # read real part:
for j in xrange(self.N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][i, j] = R.next()
for isp in range(self.Nspinblocs):
for i in xrange(
self.shells[ish][3]): # read imaginary part:
for j in xrange(self.N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][
i, j] += 1j * R.next()
# now read the Density Matrix for this orbital below the energy window:
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read real part:
for j in xrange(self.shells[ish][3]):
Dens_Mat_below[isp][ish][i, j] = R.next()
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read imaginary part:
for j in xrange(self.shells[ish][3]):
Dens_Mat_below[isp][ish][i, j] += 1j * R.next()
if (self.SP == 0): Dens_Mat_below[isp][ish] /= 2.0
# Global -> local rotation matrix for this shell:
for i in xrange(self.shells[ish][3]): # read real part:
for j in xrange(self.shells[ish][3]):
rotmat_all[ish][i, j] = R.next()
for i in xrange(self.shells[ish][3]): # read imaginary part:
for j in xrange(self.shells[ish][3]):
rotmat_all[ish][i, j] += 1j * R.next()
#print Dens_Mat_below[0][ish],Dens_Mat_below[1][ish]
if (self.SP):
rotmat_all_timeinv[ish] = int(R.next())
#except StopIteration : # a more explicit error if the file is corrupted.
# raise "SumK_LDA_Wien2k_input: reading file for Projectors failed!"
R.close()
#-----------------------------------------
# Store the input into HDF5:
ar = HDF_Archive(self.HDFfile, 'a')
if not (self.ParProjSubGrp in ar): ar.create_group(self.ParProjSubGrp)
# The subgroup containing the data. If it does not exist, it is created.
# If it exists, the data is overwritten!!!
thingstowrite = [
'Dens_Mat_below', 'N_parproj', 'Proj_Mat_pc', 'rotmat_all',
'rotmat_all_timeinv'
]
for it in thingstowrite:
exec "ar['%s']['%s'] = %s" % (self.ParProjSubGrp, it, it)
del ar
# Symmetries are used,
# Now do the symmetries for all orbitals:
self.read_Symmetry_input(orbits=self.shells,
symmfile=self.Symmpar_file,
SymmSubGrp=self.SymmParSubGrp,
SO=self.SO,
SP=self.SP)
def __init__(self,
Beta,
Norb,
U_interact=None,
J_Hund=None,
GFStruct=False,
map=False,
use_spinflip=False,
useMatrix=True,
l=2,
T=None,
dimreps=None,
irep=None,
deg_orbs=[],
Sl_Int=None):
self.offset = 0
self.use_spinflip = use_spinflip
self.Norb = Norb
if (useMatrix):
if not (Sl_Int is None):
Umat = Umatrix(l=l)
assert len(Sl_Int) == (l + 1), "Sl_Int has the wrong length"
if (type(Sl_Int) == ListType):
Rcl = numpy.array(Sl_Int)
else:
Rcl = Sl_Int
Umat(T=T, Rcl=Rcl)
else:
if ((U_interact == None) and (J_Hund == None)):
MPI.report("Give U,J or Slater integrals!!!")
assert 0
Umat = Umatrix(U_interact=U_interact, J_Hund=J_Hund, l=l)
Umat(T=T)
Umat.ReduceMatrix()
if (Umat.N == Umat.Nmat):
# Transformation T is of size 2l+1
self.U = Umat.U
self.Up = Umat.Up
else:
# Transformation is of size 2(2l+1)
self.U = Umat.U
# now we have the reduced matrices U and Up, we need it for tail fitting anyways
if (use_spinflip):
#Take the 4index Umatrix
# check for imaginary matrix elements:
if (abs(Umat.Ufull.imag) > 0.0001).any():
MPI.report(
"WARNING: complex interaction matrix!! Ignoring imaginary part for the moment!"
)
MPI.report(
"If you want to change this, look into Wien2k/Solver_MultiBand.py"
)
self.U4ind = Umat.Ufull.real
# this will be changed for arbitrary irep:
# use only one subgroup of orbitals?
if not (irep is None):
#print irep, dimreps
assert not (dimreps is None
), "Dimensions of the representatives are missing!"
assert Norb == dimreps[
irep - 1], "Dimensions of dimrep and Norb do not fit!"
for ii in range(irep - 1):
self.offset += dimreps[ii]
else:
if ((U_interact == None) and (J_Hund == None)):
MPI.report("For Kanamori representation, give U and J!!")
assert 0
self.U = numpy.zeros([Norb, Norb], numpy.float_)
self.Up = numpy.zeros([Norb, Norb], numpy.float_)
for i in range(Norb):
for j in range(Norb):
if (i == j):
self.Up[i, i] = U_interact + 2.0 * J_Hund
else:
self.Up[i, j] = U_interact
self.U[i, j] = U_interact - J_Hund
if (GFStruct):
assert map, "give also the mapping!"
self.map = map
else:
# standard GFStruct and map
GFStruct = [('%s' % (ud), [n for n in range(Norb)])
for ud in ['up', 'down']]
self.map = {
'up': ['up' for v in range(self.Norb)],
'down': ['down' for v in range(self.Norb)]
}
#print GFStruct,self.map
if (use_spinflip == False):
Hamiltonian = self.__setHamiltonian_density()
else:
if (useMatrix):
Hamiltonian = self.__setfullHamiltonian_Slater()
else:
Hamiltonian = self.__setfullHamiltonian_Kanamori(J_Hund=J_Hund)
Quantum_Numbers = self.__setQuantumNumbers(GFStruct)
# Determine if there are only blocs of size 1:
self.blocssizeone = True
for ib in GFStruct:
if (len(ib[1]) > 1): self.blocssizeone = False
# now initialize the solver with the stuff given above:
Solver.__init__(self,
Beta=Beta,
GFstruct=GFStruct,
H_Local=Hamiltonian,
Quantum_Numbers=Quantum_Numbers)
#self.SetGlobalMoves(deg_orbs)
self.N_Cycles = 10000
self.Nmax_Matrix = 100
self.N_Time_Slices_Delta = 10000
#if ((len(GFStruct)==2*Norb) and (use_spinflip==False)):
if ((self.blocssizeone) and (use_spinflip == False)):
self.Use_Segment_Picture = True
else:
self.Use_Segment_Picture = False
def __init__(
self,
HDFfile,
mu=0.0,
hfield=0.0,
UseLDABlocs=False,
LDAdata="SumK_LDA",
Symmcorrdata="SymmCorr",
ParProjdata="SumK_LDA_ParProj",
Symmpardata="SymmPar",
Bandsdata="SumK_LDA_Bands",
):
"""
Initialises the class from data previously stored into an HDF5
"""
if not (type(HDFfile) == StringType):
MPI.report("Give a string for the HDF5 filename to read the input!")
else:
self.HDFfile = HDFfile
self.LDAdata = LDAdata
self.ParProjdata = ParProjdata
self.Bandsdata = Bandsdata
self.Symmpardata = Symmpardata
self.Symmcorrdata = Symmcorrdata
self.blocnames = [["up", "down"], ["ud"]]
self.NspinblocsGF = [2, 1]
self.Gupf = None
self.hfield = hfield
# read input from HDF:
thingstoread = [
"EnergyUnit",
"Nk",
"k_dep_projection",
"SP",
"SO",
"charge_below",
"Density_Required",
"symm_op",
"N_shells",
"shells",
"N_corr_shells",
"corr_shells",
"use_rotations",
"rotmat",
"rotmat_timeinv",
"Nreps",
"dim_reps",
"T",
"N_Orbitals",
"Proj_Mat",
"BZ_weights",
"Hopping",
]
optionalthings = [
"GFStruct_Solver",
"mapinv",
"map",
"Chemical_Potential",
"dc_imp",
"DCenerg",
"deg_shells",
]
# ar=HDF_Archive(self.HDFfile,'a')
# del ar
self.retval = self.read_input_from_HDF(
SubGrp=self.LDAdata, thingstoread=thingstoread, optionalthings=optionalthings
)
# ar=HDF_Archive(self.HDFfile,'a')
# del ar
if (self.SO) and (abs(self.hfield) > 0.000001):
self.hfield = 0.0
MPI.report("For SO, the external magnetic field is not implemented, setting it to 0!!")
self.inequiv_shells(self.corr_shells) # determine the number of inequivalent correlated shells
# field to convert blocnames to indices
self.names_to_ind = [{}, {}]
for ibl in range(2):
for inm in range(self.NspinblocsGF[ibl]):
self.names_to_ind[ibl][self.blocnames[ibl][inm]] = inm * self.SP # (self.Nspinblocs-1)
# GF structure used for the local things in the k sums
self.GFStruct_corr = [
[(al, range(self.corr_shells[i][3])) for al in self.blocnames[self.corr_shells[i][4]]]
for i in xrange(self.N_corr_shells)
]
if not (self.retval["GFStruct_Solver"]):
# No GFStruct was stored in HDF, so first set a standard one:
self.GFStruct_Solver = [
[
(al, range(self.corr_shells[self.invshellmap[i]][3]))
for al in self.blocnames[self.corr_shells[self.invshellmap[i]][4]]
]
for i in xrange(self.N_inequiv_corr_shells)
]
self.map = [{} for i in xrange(self.N_inequiv_corr_shells)]
self.mapinv = [{} for i in xrange(self.N_inequiv_corr_shells)]
for i in xrange(self.N_inequiv_corr_shells):
for al in self.blocnames[self.corr_shells[self.invshellmap[i]][4]]:
self.map[i][al] = [al for j in range(self.corr_shells[self.invshellmap[i]][3])]
self.mapinv[i][al] = al
if not (self.retval["dc_imp"]):
# init the double counting:
self.__initDC()
if not (self.retval["Chemical_Potential"]):
self.Chemical_Potential = mu
if not (self.retval["deg_shells"]):
self.deg_shells = [[] for i in range(self.N_inequiv_corr_shells)]
if self.symm_op:
# MPI.report("Do the init for symm:")
self.Symm_corr = Symmetry(HDFfile, subgroup=self.Symmcorrdata)
# determine the smallest blocs, if wanted:
if UseLDABlocs:
dm = self.analyse_BS()
# now save things again to HDF5:
if MPI.IS_MASTER_NODE():
ar = HDF_Archive(self.HDFfile, "a")
ar[self.LDAdata]["hfield"] = self.hfield
del ar
self.save()
def convert_DMFT_input(self):
"""
Reads the input files, and stores the data in the HDFfile
"""
if not (MPI.IS_MASTER_NODE()): return # do it only on master:
MPI.report("Reading input from %s..." % self.LDA_file)
# Read and write only on Master!!!
# R is a generator : each R.Next() will return the next number in the file
R = Read_Fortran_File(self.LDA_file)
try:
EnergyUnit = R.next() # read the energy convertion factor
Nk = int(R.next()) # read the number of k points
k_dep_projection = 1
SP = int(R.next()) # flag for spin-polarised calculation
SO = int(R.next()) # flag for spin-orbit calculation
charge_below = R.next() # total charge below energy window
Density_Required = R.next(
) # total density required, for setting the chemical potential
symm_op = 1 # Use symmetry groups for the k-sum
# the information on the non-correlated shells is not important here, maybe skip:
N_shells = int(R.next(
)) # number of shells (e.g. Fe d, As p, O p) in the unit cell,
# corresponds to index R in formulas
# now read the information about the shells:
shells = [[int(R.next()) for i in range(4)]
for icrsh in range(N_shells)
] # reads iatom, sort, l, dim
N_corr_shells = int(R.next(
)) # number of corr. shells (e.g. Fe d, Ce f) in the unit cell,
# corresponds to index R in formulas
# now read the information about the shells:
corr_shells = [[int(R.next()) for i in range(6)]
for icrsh in range(N_corr_shells)
] # reads iatom, sort, l, dim, SO flag, irep
self.inequiv_shells(
corr_shells
) # determine the number of inequivalent correlated shells, has to be known for further reading...
use_rotations = 1
rotmat = [
numpy.identity(corr_shells[icrsh][3], numpy.complex_)
for icrsh in xrange(N_corr_shells)
]
# read the matrices
rotmat_timeinv = [0 for i in range(N_corr_shells)]
for icrsh in xrange(N_corr_shells):
for i in xrange(corr_shells[icrsh][3]): # read real part:
for j in xrange(corr_shells[icrsh][3]):
rotmat[icrsh][i, j] = R.next()
for i in xrange(corr_shells[icrsh][3]): # read imaginary part:
for j in xrange(corr_shells[icrsh][3]):
rotmat[icrsh][i, j] += 1j * R.next()
if (SP == 1): # read time inversion flag:
rotmat_timeinv[icrsh] = int(R.next())
# Read here the infos for the transformation of the basis:
Nreps = [1 for i in range(self.N_inequiv_corr_shells)]
dim_reps = [0 for i in range(self.N_inequiv_corr_shells)]
T = []
for icrsh in range(self.N_inequiv_corr_shells):
Nreps[icrsh] = int(R.next(
)) # number of representatives ("subsets"), e.g. t2g and eg
dim_reps[icrsh] = [int(R.next()) for i in range(Nreps[icrsh])
] # dimensions of the subsets
# The transformation matrix:
# it is of dimension 2l+1, if no SO, and 2*(2l+1) with SO!!
#T = []
#for ish in xrange(self.N_inequiv_corr_shells):
ll = 2 * corr_shells[self.invshellmap[icrsh]][2] + 1
lmax = ll * (corr_shells[self.invshellmap[icrsh]][4] + 1)
T.append(numpy.zeros([lmax, lmax], numpy.complex_))
# now read it from file:
for i in xrange(lmax):
for j in xrange(lmax):
T[icrsh][i, j] = R.next()
for i in xrange(lmax):
for j in xrange(lmax):
T[icrsh][i, j] += 1j * R.next()
# Spin blocks to be read:
Nspinblocs = SP + 1 - SO # number of spins to read for Norbs and Ham, NOT Projectors
# read the list of N_Orbitals for all k points
N_Orbitals = [[0 for isp in range(Nspinblocs)]
for ik in xrange(Nk)]
for isp in range(Nspinblocs):
for ik in xrange(Nk):
N_Orbitals[ik][isp] = int(R.next())
#print N_Orbitals
# Initialise the projectors:
Proj_Mat = [[[
numpy.zeros([corr_shells[icrsh][3], N_Orbitals[ik][isp]],
numpy.complex_) for icrsh in range(N_corr_shells)
] for isp in range(Nspinblocs)] for ik in range(Nk)]
# Read the projectors from the file:
for ik in xrange(Nk):
for icrsh in range(N_corr_shells):
no = corr_shells[icrsh][3]
# first Real part for BOTH spins, due to conventions in dmftproj:
for isp in range(Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i, j] = R.next()
# now Imag part:
for isp in range(Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i, j] += 1j * R.next()
# now define the arrays for weights and hopping ...
BZ_weights = numpy.ones([Nk], numpy.float_) / float(
Nk) # w(k_index), default normalisation
Hopping = [[
numpy.zeros([N_Orbitals[ik][isp], N_Orbitals[ik][isp]],
numpy.complex_) for isp in range(Nspinblocs)
] for ik in xrange(Nk)]
# weights in the file
for ik in xrange(Nk):
BZ_weights[ik] = R.next()
# if the sum over spins is in the weights, take it out again!!
sm = sum(BZ_weights)
BZ_weights[:] /= sm
# Grab the H
# we use now the convention of a DIAGONAL Hamiltonian!!!!
for isp in range(Nspinblocs):
for ik in xrange(Nk):
no = N_Orbitals[ik][isp]
for i in xrange(no):
Hopping[ik][isp][i, i] = R.next() * EnergyUnit
#keep some things that we need for reading parproj:
self.N_shells = N_shells
self.shells = shells
self.N_corr_shells = N_corr_shells
self.corr_shells = corr_shells
self.Nspinblocs = Nspinblocs
self.N_Orbitals = N_Orbitals
self.Nk = Nk
self.SO = SO
self.SP = SP
self.EnergyUnit = EnergyUnit
except StopIteration: # a more explicit error if the file is corrupted.
raise "SumK_LDA : reading file HMLT_file failed!"
R.close()
#print Proj_Mat[0]
#-----------------------------------------
# Store the input into HDF5:
ar = HDF_Archive(self.HDFfile, 'a')
if not (self.LDASubGrp in ar): ar.create_group(self.LDASubGrp)
# The subgroup containing the data. If it does not exist, it is created.
# If it exists, the data is overwritten!!!
ar[self.LDASubGrp]['EnergyUnit'] = EnergyUnit
ar[self.LDASubGrp]['Nk'] = Nk
ar[self.LDASubGrp]['k_dep_projection'] = k_dep_projection
ar[self.LDASubGrp]['SP'] = SP
ar[self.LDASubGrp]['SO'] = SO
ar[self.LDASubGrp]['charge_below'] = charge_below
ar[self.LDASubGrp]['Density_Required'] = Density_Required
ar[self.LDASubGrp]['symm_op'] = symm_op
ar[self.LDASubGrp]['N_shells'] = N_shells
ar[self.LDASubGrp]['shells'] = shells
ar[self.LDASubGrp]['N_corr_shells'] = N_corr_shells
ar[self.LDASubGrp]['corr_shells'] = corr_shells
ar[self.LDASubGrp]['use_rotations'] = use_rotations
ar[self.LDASubGrp]['rotmat'] = rotmat
ar[self.LDASubGrp]['rotmat_timeinv'] = rotmat_timeinv
ar[self.LDASubGrp]['Nreps'] = Nreps
ar[self.LDASubGrp]['dim_reps'] = dim_reps
ar[self.LDASubGrp]['T'] = T
ar[self.LDASubGrp]['N_Orbitals'] = N_Orbitals
ar[self.LDASubGrp]['Proj_Mat'] = Proj_Mat
ar[self.LDASubGrp]['BZ_weights'] = BZ_weights
ar[self.LDASubGrp]['Hopping'] = Hopping
del ar
# Symmetries are used,
# Now do the symmetries for correlated orbitals:
self.read_Symmetry_input(orbits=corr_shells,
symmfile=self.Symm_file,
SymmSubGrp=self.SymmSubGrp,
SO=SO,
SP=SP)
def analyse_BS(self, threshold=0.00001, includeshells=None):
""" Determines the Greens function block structure from the simple point integration"""
dm = self.simplepointdensmat()
densmat = [dm[self.invshellmap[ish]] for ish in xrange(self.N_inequiv_corr_shells)]
if includeshells is None:
includeshells = range(self.N_inequiv_corr_shells)
for ish in includeshells:
# self.GFStruct_Solver.append([])
self.GFStruct_Solver[ish] = []
a_list = [a for a, al in self.GFStruct_corr[self.invshellmap[ish]]]
for a in a_list:
dm = densmat[ish][a]
dmbool = abs(dm) > threshold # gives an index list of entries larger that threshold
offdiag = []
for i in xrange(len(dmbool)):
for j in xrange(i, len(dmbool)):
if (dmbool[i, j]) & (i != j):
offdiag.append([i, j])
NBlocs = len(dmbool)
blocs = [[i] for i in range(NBlocs)]
for i in range(len(offdiag)):
if offdiag[i][0] != offdiag[i][1]:
for j in range(len(blocs[offdiag[i][1]])):
blocs[offdiag[i][0]].append(blocs[offdiag[i][1]][j])
del blocs[offdiag[i][1]]
for j in range(i + 1, len(offdiag)):
if offdiag[j][0] == offdiag[i][1]:
offdiag[j][0] = offdiag[i][0]
if offdiag[j][1] == offdiag[i][1]:
offdiag[j][1] = offdiag[i][0]
if offdiag[j][0] > offdiag[i][1]:
offdiag[j][0] -= 1
if offdiag[j][1] > offdiag[i][1]:
offdiag[j][1] -= 1
offdiag[j].sort()
NBlocs -= 1
for i in range(NBlocs):
blocs[i].sort()
self.GFStruct_Solver[ish].append(("%s%s" % (a, i), blocs[i]))
# map is the mapping of the blocs from the SK blocs to the CTQMC blocs:
self.map[ish][a] = range(len(dmbool))
for ibl in range(NBlocs):
for j in range(len(blocs[ibl])):
self.map[ish][a][blocs[ibl][j]] = "%s%s" % (a, ibl)
self.mapinv[ish]["%s%s" % (a, ibl)] = a
# now calculate degeneracies of orbitals:
dm = {}
for bl in self.GFStruct_Solver[ish]:
bln = bl[0]
ind = bl[1]
# get dm for the blocks:
dm[bln] = numpy.zeros([len(ind), len(ind)], numpy.complex_)
for i in range(len(ind)):
for j in range(len(ind)):
dm[bln][i, j] = densmat[ish][self.mapinv[ish][bln]][ind[i], ind[j]]
for bl in self.GFStruct_Solver[ish]:
for bl2 in self.GFStruct_Solver[ish]:
if dm[bl[0]].shape == dm[bl2[0]].shape:
if ((abs(dm[bl[0]] - dm[bl2[0]]) < threshold).all()) and (bl[0] != bl2[0]):
# check if it was already there:
ind1 = -1
ind2 = -2
for n, ind in enumerate(self.deg_shells[ish]):
if bl[0] in ind:
ind1 = n
if bl2[0] in ind:
ind2 = n
if (ind1 < 0) and (ind2 >= 0):
self.deg_shells[ish][ind2].append(bl[0])
elif (ind1 >= 0) and (ind2 < 0):
self.deg_shells[ish][ind1].append(bl2[0])
elif (ind1 < 0) and (ind2 < 0):
self.deg_shells[ish].append([bl[0], bl2[0]])
if MPI.IS_MASTER_NODE():
ar = HDF_Archive(self.HDFfile, "a")
ar[self.LDAdata]["GFStruct_Solver"] = self.GFStruct_Solver
ar[self.LDAdata]["map"] = self.map
ar[self.LDAdata]["mapinv"] = self.mapinv
try:
ar[self.LDAdata]["deg_shells"] = self.deg_shells
except:
MPI.report("deg_shells not stored, degeneracies not found")
del ar
return densmat
def read_Symmetry_input(self, orbits, symmfile, SymmSubGrp, SO, SP):
"""
Reads input for the symmetrisations from symmfile, which is case.sympar or case.symqmc.
"""
if not (MPI.IS_MASTER_NODE()): return
MPI.report("Reading symmetry input from %s..." % symmfile)
N_orbits = len(orbits)
R = Read_Fortran_File(symmfile)
try:
Ns = int(R.next()) # Number of symmetry operations
Natoms = int(R.next()) # number of atoms involved
perm = [[int(R.next()) for i in xrange(Natoms)]
for j in xrange(Ns)] # list of permutations of the atoms
if SP:
timeinv = [int(R.next()) for j in xrange(Ns)
] # timeinversion for SO xoupling
else:
timeinv = [0 for j in xrange(Ns)]
# Now read matrices:
mat = []
for iNs in xrange(Ns):
mat.append([
numpy.zeros([orbits[orb][3], orbits[orb][3]],
numpy.complex_) for orb in xrange(N_orbits)
])
for orb in range(N_orbits):
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat[iNs][orb][i, j] = R.next() # real part
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat[iNs][orb][i,
j] += 1j * R.next() # imaginary part
# determine the inequivalent shells:
#SHOULD BE FINALLY REMOVED, PUT IT FOR ALL ORBITALS!!!!!
#self.inequiv_shells(orbits)
mat_tinv = [
numpy.identity(orbits[orb][3], numpy.complex_)
for orb in range(N_orbits)
]
if ((SO == 0) and (SP == 0)):
# here we need an additional time inversion operation, so read it:
for orb in range(N_orbits):
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat_tinv[orb][i, j] = R.next() # real part
for i in xrange(orbits[orb][3]):
for j in xrange(orbits[orb][3]):
mat_tinv[orb][i,
j] += 1j * R.next() # imaginary part
except StopIteration: # a more explicit error if the file is corrupted.
raise "Symmetry : reading file failed!"
R.close()
# Save it to the HDF:
ar = HDF_Archive(self.HDFfile, 'a')
if not (SymmSubGrp in ar): ar.create_group(SymmSubGrp)
thingstowrite = [
'Ns', 'Natoms', 'perm', 'orbits', 'SO', 'SP', 'timeinv', 'mat',
'mat_tinv'
]
for it in thingstowrite:
exec "ar['%s']['%s'] = %s" % (SymmSubGrp, it, it)
del ar
def convert_bands_input(self, BandsSubGrp='SumK_LDA_Bands'):
"""
Converts the input for momentum resolved spectral functions, and stores it in BandsSubGrp in the
HDF5.
"""
if not (MPI.IS_MASTER_NODE()): return
self.BandsSubGrp = BandsSubGrp
MPI.report("Reading bands input from %s..." % self.Band_file)
R = Read_Fortran_File(self.Band_file)
try:
Nk = int(R.next())
# read the list of N_Orbitals for all k points
N_Orbitals = [[0 for isp in range(self.Nspinblocs)]
for ik in xrange(Nk)]
for isp in range(self.Nspinblocs):
for ik in xrange(Nk):
N_Orbitals[ik][isp] = int(R.next())
# Initialise the projectors:
Proj_Mat = [[[
numpy.zeros([self.corr_shells[icrsh][3], N_Orbitals[ik][isp]],
numpy.complex_)
for icrsh in range(self.N_corr_shells)
] for isp in range(self.Nspinblocs)] for ik in range(Nk)]
# Read the projectors from the file:
for ik in xrange(Nk):
for icrsh in range(self.N_corr_shells):
no = self.corr_shells[icrsh][3]
# first Real part for BOTH spins, due to conventions in dmftproj:
for isp in range(self.Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i, j] = R.next()
# now Imag part:
for isp in range(self.Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i, j] += 1j * R.next()
Hopping = [[
numpy.zeros([N_Orbitals[ik][isp], N_Orbitals[ik][isp]],
numpy.complex_) for isp in range(self.Nspinblocs)
] for ik in xrange(Nk)]
# Grab the H
# we use now the convention of a DIAGONAL Hamiltonian!!!!
for isp in range(self.Nspinblocs):
for ik in xrange(Nk):
no = N_Orbitals[ik][isp]
for i in xrange(no):
Hopping[ik][isp][i, i] = R.next() * self.EnergyUnit
# now read the partial projectors:
N_parproj = [int(R.next()) for i in range(self.N_shells)]
# Initialise P, here a double list of matrices:
Proj_Mat_pc = [[[[
numpy.zeros([self.shells[ish][3], N_Orbitals[ik][isp]],
numpy.complex_) for ir in range(N_parproj[ish])
] for ish in range(self.N_shells)]
for isp in range(self.Nspinblocs)]
for ik in range(Nk)]
for ish in range(self.N_shells):
for ik in xrange(Nk):
for ir in range(N_parproj[ish]):
for isp in range(self.Nspinblocs):
for i in xrange(
self.shells[ish][3]): # read real part:
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][
i, j] = R.next()
for i in xrange(self.shells[ish]
[3]): # read imaginary part:
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][
i, j] += 1j * R.next()
except StopIteration: # a more explicit error if the file is corrupted.
raise "SumK_LDA : reading file HMLT_file failed!"
R.close()
# reading done!
#-----------------------------------------
# Store the input into HDF5:
ar = HDF_Archive(self.HDFfile, 'a')
if not (self.BandsSubGrp in ar): ar.create_group(self.BandsSubGrp)
# The subgroup containing the data. If it does not exist, it is created.
# If it exists, the data is overwritten!!!
thingstowrite = [
'Nk', 'N_Orbitals', 'Proj_Mat', 'Hopping', 'N_parproj',
'Proj_Mat_pc'
]
for it in thingstowrite:
exec "ar['%s']['%s'] = %s" % (self.BandsSubGrp, it, it)
#ar[self.BandsSubGrp]['Nk'] = Nk
#ar[self.BandsSubGrp]['N_Orbitals'] = N_Orbitals
#ar[self.BandsSubGrp]['Proj_Mat'] = Proj_Mat
#self.Proj_Mat = Proj_Mat
#self.N_Orbitals = N_Orbitals
#self.Nk = Nk
#self.Hopping = Hopping
del ar
def Solve(self):
""" Solve the impurity problem """
# Find if an operator is in oplist
def mysearch(op):
l = [ k for (k,v) in OPdict.items() if (v-op).is_zero()]
assert len(l) <=1
return l[0] if l else None
# Same but raises an error if pb
def myfind(op):
r = mysearch(op)
if r==None : raise "Operator %s can not be found by myfind !"%r
return r
# For backward compatibility
self.update_params(self.__dict__)
# Test all a parameters before solutions
MPI.report(Parameters.check(self.__dict__,self.Required,self.Optional))
# We have to add the Hamiltonian the epsilon part of G0
if type(self.H_Local) != type(Operator()) : raise "H_Local is not an operator"
H = self.H_Local
for a,alpha_list in self.GFStruct :
for mu in alpha_list :
for nu in alpha_list :
H += real(self.G0[a]._tail[2][mu,nu]) * Cdag(a,mu)*C(a,nu)
OPdict = {"Hamiltonian": H}
MPI.report("Hamiltonian with Eps0 term : ",H)
# First separate the quantum Numbers that are operators and those which are symmetries.
QuantumNumberOperators = dict( (n,op) for (n,op) in self.Quantum_Numbers.items() if type(op) == type(Operator()))
QuantumNumberSymmetries = dict( (n,op) for (n,op) in self.Quantum_Numbers.items() if type(op) != type(Operator()))
# Check that the quantum numbers commutes with the Hamiltonian
for name,op in QuantumNumberOperators.items():
assert Commutator(self.H_Local ,op).is_zero(), "One quantum number is not commuting with Hamiltonian"
OPdict[name]=op
# Complete the OPdict with the fundamental operators
OPdict, nf, nb, SymChar, NameOpFundamentalList = Operators.Complete_OperatorsList_with_Fundamentals(OPdict)
# Add the operators to be averaged in OPdict and prepare the list for the C-code
self.Measured_Operators_Results = {}
self.twice_defined_Ops = {}
self.Operators_To_Average_List = []
for name, op in self.Measured_Operators.items():
opn = mysearch(op)
if opn == None :
OPdict[name] = op
self.Measured_Operators_Results[name] = 0.0
self.Operators_To_Average_List.append(name)
else:
MPI.report("Operator %s already defined as %s, using this instead for measuring"%(name,opn))
self.twice_defined_Ops[name] = opn
self.Measured_Operators_Results[opn] = 0.0
if opn not in self.Operators_To_Average_List: self.Operators_To_Average_List.append(opn)
# Time correlation functions are added
self.OpCorr_To_Average_List = []
for name, op in self.Measured_Time_Correlators.items():
opn = mysearch(op[0])
if opn == None :
OPdict[name] = op[0]
self.OpCorr_To_Average_List.append(name)
else:
MPI.report("Operator %s already defined as %s, using this instead for measuring"%(name,opn))
if opn not in self.OpCorr_To_Average_List: self.OpCorr_To_Average_List.append(opn)
# Create storage for data:
Nops = len(self.OpCorr_To_Average_List)
f = lambda L : GFBloc_ImTime(Indices= [0], Beta = self.Beta, NTimeSlices=L )
if (Nops>0):
self.Measured_Time_Correlators_Results = GF(Name_Block_Generator = [ ( n,f(self.Measured_Time_Correlators[n][1]) ) for n in self.Measured_Time_Correlators], Copy=False)
else:
self.Measured_Time_Correlators_Results = GF(Name_Block_Generator = [ ( 'OpCorr',f(2) ) ], Copy=False)
# Take care of the global moves
# First, given a function (a,alpha,dagger) -> (a', alpha', dagger')
# I construct a function on fundamental operators
def Map_GM_to_Fund_Ops( GM ) :
def f(fop) :
a,alpha, dagger = fop.name + (fop.dag,)
ap,alphap,daggerp = GM((a,alpha,dagger))
return Cdag(ap,alphap) if daggerp else C(ap,alphap)
return f
# Complete the OpList so that it is closed under the global moves
while 1:
added_something = False
for n,(proba,GM) in enumerate(self.Global_Moves):
# F is a function that map all operators according to the global move
F = Extend_Function_on_Fundamentals(Map_GM_to_Fund_Ops(GM))
# Make sure that OPdict is complete, i.e. all images of OPdict operators are in OPdict
for name,op in OPdict.items() :
op_im = F(op)
if mysearch(op_im)==None :
# find the key and put in in the dictionnary
i=0
while 1:
new_name = name + 'GM' + i*'_' + "%s"%n
if new_name not in OPdict : break
added_something = True
OPdict[new_name] = op_im
# break the while loop
if not added_something: break
# Now I have all operators, I make the transcription of the global moves
self.Global_Moves_Mapping_List = []
for n,(proba,GM) in enumerate(self.Global_Moves):
F = Extend_Function_on_Fundamentals(Map_GM_to_Fund_Ops(GM))
m = {}
for name,op in OPdict.items() :
op_im = F(op)
n1,n2 = myfind(op),myfind(op_im)
m[n1] = n2
name = "%s"%n
self.Global_Moves_Mapping_List.append((proba,m,name))
#MPI.report ("Global_Moves_Mapping_List", self.Global_Moves_Mapping_List)
# Now add the operator for F calculation if needed
if self.Use_F :
Hloc_WithoutQuadratic = self.H_Local.RemoveQuadraticTerms()
for n,op in OPdict.items() :
if op.is_Fundamental():
op2 = Commutator(Hloc_WithoutQuadratic,op)
if not mysearch(op2) : OPdict["%s_Comm_Hloc"%n] = op2
# All operators have real coefficients. Check this and remove the 0j term
# since the C++ expects operators with real numbers
for n,op in OPdict.items(): op.make_coef_real_and_check()
# Transcription of operators for C++
Oplist2 = Operators.Transcribe_OpList_for_C(OPdict)
SymList = [sym for (n,sym) in SymChar.items() if n in QuantumNumberSymmetries]
self.H_diag = C_Module.Hloc(nf,nb,Oplist2,QuantumNumberOperators,SymList,self.Quantum_Numbers_Selection,0)
# Create the C_Cag_Ops array which describes the grouping of (C,Cdagger) operator
# for the MonteCarlo moves : (a, alpha) block structure [ [ (C_name, Cdag_name)]]
self.C_Cdag_Ops = [ [ (myfind(C(a,alpha)), myfind(Cdag(a,alpha))) for alpha in al ] for a,al in self.GFStruct]
# Define G0_inv and correct it to have G0 to have perfect 1/omega behavior
self.G0_inv = inverse(self.G0)
Delta = self.G0_inv.Delta()
for n,g in self.G0_inv:
assert(g.N1==g.N2)
identity=numpy.identity(g.N1)
self.G0[n] <<= GF_Initializers.A_Omega_Plus_B(identity, g._tail[0])
self.G0[n] -= Delta[n]
#self.G0[n] <<= iOmega_n + g._tail[0] - Delta[n]
self.G0_inv <<= self.G0
self.G0.invert()
# Construct the function in tau
f = lambda g,L : GFBloc_ImTime(Indices= g.Indices, Beta = g.Beta, NTimeSlices=L )
self.Delta_tau = GF(Name_Block_Generator = [ (n,f(g,self.N_Time_Slices_Delta) ) for n,g in self.G], Copy=False, Name='D')
self.G_tau = GF(Name_Block_Generator = [ (n,f(g,self.N_Time_Slices_Gtau) ) for n,g in self.G], Copy=False, Name='G')
self.F_tau = GF(Name_Block_Generator = self.G_tau, Copy=True, Name='F')
for (i,gt) in self.Delta_tau : gt.setFromInverseFourierOf(Delta[i])
MPI.report("Inv Fourier done")
if (self.Legendre_Accumulation):
self.G_Legendre = GF(Name_Block_Generator = [ (n,GFBloc_ImLegendre(Indices=g.Indices, Beta=g.Beta, NLegendreCoeffs=self.N_Legendre_Coeffs) ) for n,g in self.G], Copy=False, Name='Gl')
else:
self.G_Legendre = GF(Name_Block_Generator = [ (n,GFBloc_ImLegendre(Indices=[1], Beta=g.Beta, NLegendreCoeffs=1) ) for n,g in self.G], Copy=False, Name='Gl') # G_Legendre must not be empty but is not needed in this case. So I make it as small as possible.
# Starting the C++ code
self.Sigma_Old <<= self.Sigma
C_Module.MC_solve(self.__dict__ ) # C++ solver
# Compute G on Matsubara axis possibly fitting the tail
if self.Legendre_Accumulation:
for s,g in self.G:
identity=numpy.zeros([g.N1,g.N2],numpy.float)
for i,m in enumerate (g._IndicesL):
for j,n in enumerate (g._IndicesR):
if m==n: identity[i,j]=1
self.G_Legendre[s].enforce_discontinuity(identity) # set the known tail
g <<= LegendreToMatsubara(self.G_Legendre[s])
else:
if (self.Time_Accumulation):
for name, g in self.G_tau:
identity=numpy.zeros([g.N1,g.N2],numpy.float)
for i,m in enumerate (g._IndicesL):
for j,n in enumerate (g._IndicesR):
if m==n: identity[i,j]=1
g._tail.zero()
g._tail[1] = identity
self.G[name].setFromFourierOf(g)
# This is very sick... but what can we do???
self.Sigma <<= self.G0_inv - inverse(self.G)
self.fitTails()
self.G <<= inverse(self.G0_inv - self.Sigma)
# Now find the self-energy
self.Sigma <<= self.G0_inv - inverse(self.G)
MPI.report("Solver %(Name)s has ended."%self.__dict__)
# for operator averages: if twice defined operator, rename output:
for op1,op2 in self.twice_defined_Ops.items():
self.Measured_Operators_Results[op1] = self.Measured_Operators_Results[op2]
for op1,op2 in self.twice_defined_Ops.items():
if op2 in self.Measured_Operators_Results.keys(): del self.Measured_Operators_Results[op2]
if self.Use_F :
for (n,f) in self.F: f.setFromFourierOf(self.F_tau[n])
self.G2 = self.G0 + self.G0 * self.F
self.Sigma2 = self.F * inverse(self.G2)
def convert_Parproj_input(self,ParProjSubGrp='SumK_LDA_ParProj',SymmParSubGrp='SymmPar'):
"""
Reads the input for the partial charges projectors from case.parproj, and stores it in the SymmParSubGrp
group in the HDF5.
"""
if not (MPI.IS_MASTER_NODE()): return
self.ParProjSubGrp = ParProjSubGrp
self.SymmParSubGrp = SymmParSubGrp
MPI.report("Reading parproj input from %s..."%self.Parproj_file)
Dens_Mat_below = [ [numpy.zeros([self.shells[ish][3],self.shells[ish][3]],numpy.complex_) for ish in range(self.N_shells)]
for isp in range(self.Nspinblocs) ]
R = Read_Fortran_File(self.Parproj_file)
#try:
N_parproj = [int(R.next()) for i in range(self.N_shells)]
# Initialise P, here a double list of matrices:
Proj_Mat_pc = [ [ [ [numpy.zeros([self.shells[ish][3], self.N_Orbitals[ik][isp]], numpy.complex_)
for ir in range(N_parproj[ish])]
for ish in range (self.N_shells) ]
for isp in range(self.Nspinblocs) ]
for ik in range(self.Nk) ]
rotmat_all = [numpy.identity(self.shells[ish][3],numpy.complex_) for ish in xrange(self.N_shells)]
rotmat_all_timeinv = [0 for i in range(self.N_shells)]
for ish in range(self.N_shells):
#print ish
# read first the projectors for this orbital:
for ik in xrange(self.Nk):
for ir in range(N_parproj[ish]):
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read real part:
for j in xrange(self.N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][i,j] = R.next()
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read imaginary part:
for j in xrange(self.N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][i,j] += 1j * R.next()
# now read the Density Matrix for this orbital below the energy window:
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read real part:
for j in xrange(self.shells[ish][3]):
Dens_Mat_below[isp][ish][i,j] = R.next()
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read imaginary part:
for j in xrange(self.shells[ish][3]):
Dens_Mat_below[isp][ish][i,j] += 1j * R.next()
if (self.SP==0): Dens_Mat_below[isp][ish] /= 2.0
# Global -> local rotation matrix for this shell:
for i in xrange(self.shells[ish][3]): # read real part:
for j in xrange(self.shells[ish][3]):
rotmat_all[ish][i,j] = R.next()
for i in xrange(self.shells[ish][3]): # read imaginary part:
for j in xrange(self.shells[ish][3]):
rotmat_all[ish][i,j] += 1j * R.next()
#print Dens_Mat_below[0][ish],Dens_Mat_below[1][ish]
if (self.SP):
rotmat_all_timeinv[ish] = int(R.next())
#except StopIteration : # a more explicit error if the file is corrupted.
# raise "SumK_LDA_Wien2k_input: reading file for Projectors failed!"
R.close()
#-----------------------------------------
# Store the input into HDF5:
ar = HDF_Archive(self.HDFfile,'a')
if not (self.ParProjSubGrp in ar): ar.create_group(self.ParProjSubGrp)
# The subgroup containing the data. If it does not exist, it is created.
# If it exists, the data is overwritten!!!
thingstowrite = ['Dens_Mat_below','N_parproj','Proj_Mat_pc','rotmat_all','rotmat_all_timeinv']
for it in thingstowrite: exec "ar['%s']['%s'] = %s"%(self.ParProjSubGrp,it,it)
del ar
# Symmetries are used,
# Now do the symmetries for all orbitals:
self.read_Symmetry_input(orbits=self.shells,symmfile=self.Symmpar_file,SymmSubGrp=self.SymmParSubGrp,SO=self.SO,SP=self.SP)
def __init__(self, Beta, Norb, U_interact=None, J_Hund=None, GFStruct=False, map=False, use_spinflip=False,
useMatrix = True, l=2, T=None, dimreps=None, irep=None, deg_orbs = [], Sl_Int = None):
self.offset = 0
self.use_spinflip = use_spinflip
self.Norb = Norb
if (useMatrix):
if not (Sl_Int is None):
Umat = Umatrix(l=l)
assert len(Sl_Int)==(l+1),"Sl_Int has the wrong length"
if (type(Sl_Int)==ListType):
Rcl = numpy.array(Sl_Int)
else:
Rcl = Sl_Int
Umat(T=T,Rcl=Rcl)
else:
if ((U_interact==None)and(J_Hund==None)):
MPI.report("Give U,J or Slater integrals!!!")
assert 0
Umat = Umatrix(U_interact=U_interact, J_Hund=J_Hund, l=l)
Umat(T=T)
Umat.ReduceMatrix()
if (Umat.N==Umat.Nmat):
# Transformation T is of size 2l+1
self.U = Umat.U
self.Up = Umat.Up
else:
# Transformation is of size 2(2l+1)
self.U = Umat.U
# now we have the reduced matrices U and Up, we need it for tail fitting anyways
if (use_spinflip):
#Take the 4index Umatrix
# check for imaginary matrix elements:
if (abs(Umat.Ufull.imag)>0.0001).any():
MPI.report("WARNING: complex interaction matrix!! Ignoring imaginary part for the moment!")
MPI.report("If you want to change this, look into Wien2k/Solver_MultiBand.py")
self.U4ind = Umat.Ufull.real
# this will be changed for arbitrary irep:
# use only one subgroup of orbitals?
if not (irep is None):
#print irep, dimreps
assert not (dimreps is None), "Dimensions of the representatives are missing!"
assert Norb==dimreps[irep-1],"Dimensions of dimrep and Norb do not fit!"
for ii in range(irep-1):
self.offset += dimreps[ii]
else:
if ((U_interact==None)and(J_Hund==None)):
MPI.report("For Kanamori representation, give U and J!!")
assert 0
self.U = numpy.zeros([Norb,Norb],numpy.float_)
self.Up = numpy.zeros([Norb,Norb],numpy.float_)
for i in range(Norb):
for j in range(Norb):
if (i==j):
self.Up[i,i] = U_interact + 2.0*J_Hund
else:
self.Up[i,j] = U_interact
self.U[i,j] = U_interact - J_Hund
if (GFStruct):
assert map, "give also the mapping!"
self.map = map
else:
# standard GFStruct and map
GFStruct = [ ('%s'%(ud),[n for n in range(Norb)]) for ud in ['up','down'] ]
self.map = {'up' : ['up' for v in range(self.Norb)], 'down' : ['down' for v in range(self.Norb)]}
#print GFStruct,self.map
if (use_spinflip==False):
Hamiltonian = self.__setHamiltonian_density()
else:
if (useMatrix):
Hamiltonian = self.__setfullHamiltonian_Slater()
else:
Hamiltonian = self.__setfullHamiltonian_Kanamori(J_Hund = J_Hund)
Quantum_Numbers = self.__setQuantumNumbers(GFStruct)
# Determine if there are only blocs of size 1:
self.blocssizeone = True
for ib in GFStruct:
if (len(ib[1])>1): self.blocssizeone = False
# now initialize the solver with the stuff given above:
Solver.__init__(self,
Beta = Beta,
GFstruct = GFStruct,
H_Local = Hamiltonian,
Quantum_Numbers = Quantum_Numbers )
#self.SetGlobalMoves(deg_orbs)
self.N_Cycles = 10000
self.Nmax_Matrix = 100
self.N_Time_Slices_Delta= 10000
#if ((len(GFStruct)==2*Norb) and (use_spinflip==False)):
if ((self.blocssizeone) and (use_spinflip==False)):
self.Use_Segment_Picture = True
else:
self.Use_Segment_Picture = False
def convert_bands_input(self,BandsSubGrp = 'SumK_LDA_Bands'):
"""
Converts the input for momentum resolved spectral functions, and stores it in BandsSubGrp in the
HDF5.
"""
if not (MPI.IS_MASTER_NODE()): return
self.BandsSubGrp = BandsSubGrp
MPI.report("Reading bands input from %s..."%self.Band_file)
R = Read_Fortran_File(self.Band_file)
try:
Nk = int(R.next())
# read the list of N_Orbitals for all k points
N_Orbitals = [ [0 for isp in range(self.Nspinblocs)] for ik in xrange(Nk)]
for isp in range(self.Nspinblocs):
for ik in xrange(Nk):
N_Orbitals[ik][isp] = int(R.next())
# Initialise the projectors:
Proj_Mat = [ [ [numpy.zeros([self.corr_shells[icrsh][3], N_Orbitals[ik][isp]], numpy.complex_)
for icrsh in range (self.N_corr_shells)]
for isp in range(self.Nspinblocs)]
for ik in range(Nk) ]
# Read the projectors from the file:
for ik in xrange(Nk):
for icrsh in range(self.N_corr_shells):
no = self.corr_shells[icrsh][3]
# first Real part for BOTH spins, due to conventions in dmftproj:
for isp in range(self.Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i,j] = R.next()
# now Imag part:
for isp in range(self.Nspinblocs):
for i in xrange(no):
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat[ik][isp][icrsh][i,j] += 1j * R.next()
Hopping = [ [numpy.zeros([N_Orbitals[ik][isp],N_Orbitals[ik][isp]],numpy.complex_)
for isp in range(self.Nspinblocs)] for ik in xrange(Nk) ]
# Grab the H
# we use now the convention of a DIAGONAL Hamiltonian!!!!
for isp in range(self.Nspinblocs):
for ik in xrange(Nk) :
no = N_Orbitals[ik][isp]
for i in xrange(no):
Hopping[ik][isp][i,i] = R.next() * self.EnergyUnit
# now read the partial projectors:
N_parproj = [int(R.next()) for i in range(self.N_shells)]
# Initialise P, here a double list of matrices:
Proj_Mat_pc = [ [ [ [numpy.zeros([self.shells[ish][3], N_Orbitals[ik][isp]], numpy.complex_)
for ir in range(N_parproj[ish])]
for ish in range (self.N_shells) ]
for isp in range(self.Nspinblocs) ]
for ik in range(Nk) ]
for ish in range(self.N_shells):
for ik in xrange(Nk):
for ir in range(N_parproj[ish]):
for isp in range(self.Nspinblocs):
for i in xrange(self.shells[ish][3]): # read real part:
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][i,j] = R.next()
for i in xrange(self.shells[ish][3]): # read imaginary part:
for j in xrange(N_Orbitals[ik][isp]):
Proj_Mat_pc[ik][isp][ish][ir][i,j] += 1j * R.next()
except StopIteration : # a more explicit error if the file is corrupted.
raise "SumK_LDA : reading file HMLT_file failed!"
R.close()
# reading done!
#-----------------------------------------
# Store the input into HDF5:
ar = HDF_Archive(self.HDFfile,'a')
if not (self.BandsSubGrp in ar): ar.create_group(self.BandsSubGrp)
# The subgroup containing the data. If it does not exist, it is created.
# If it exists, the data is overwritten!!!
thingstowrite = ['Nk','N_Orbitals','Proj_Mat','Hopping','N_parproj','Proj_Mat_pc']
for it in thingstowrite: exec "ar['%s']['%s'] = %s"%(self.BandsSubGrp,it,it)
#ar[self.BandsSubGrp]['Nk'] = Nk
#ar[self.BandsSubGrp]['N_Orbitals'] = N_Orbitals
#ar[self.BandsSubGrp]['Proj_Mat'] = Proj_Mat
#self.Proj_Mat = Proj_Mat
#self.N_Orbitals = N_Orbitals
#self.Nk = Nk
#self.Hopping = Hopping
del ar
def Dichotomy(Function, xinit,yvalue,Precision_on_y,Delta_x, MaxNbreLoop=1000, xname="", yname="",verbosity=1):
"""
Solver Function(x) = yvalue.
Arguments :
- Function : function (real valued) to be solved by dichotomy
- xinit : Init value for x. On success, returns the new value of x
- yvalue :
- precision : calculation stops for abs(f(x) - yvalue)<precision
- MaxNbreLoop : maximum number of loops before failure. Default is 1000
- xname, yname : name of the variable x, y for the report
- verbosity : verbosity level.
Returns :
- A tuple (x,y). x is the value found, y is f(x).
- (None,None) if the calculation failed.
"""
def sign(x):
if x>0.0 : return 1
if x<0.0 : return -1
return 0
MPI.report("Dichotomy adjustment of %(xname)s to obtain %(yname)s = %(yvalue)f +/- %(Precision_on_y)f"%locals() )
PR = " "
if xname=="" or yname=="" : verbosity = max(verbosity,1)
x=xinit;Delta_x= abs(Delta_x)
# First find the bounds
y1 = Function(x)
eps = sign(y1-yvalue)
x1=x;y2=y1;x2=x1
nbre_loop=0
while (nbre_loop<= MaxNbreLoop) and (y2-yvalue)*eps>0 and abs(y2-yvalue)>Precision_on_y :
nbre_loop +=1
x2 -= eps*Delta_x
y2 = Function(x2)
if xname!="" and verbosity>2:
MPI.report("%(PR)s%(xname)s = %(x2)f \n%(PR)s%(yname)s = %(y2)f"%locals())
MPI.report("%(PR)s%(x1)f < %(xname)s < %(x2)f"%locals())
MPI.report("%(PR)s%(y1)f < %(yname)s < %(y2)f"%locals())
# Now mu is between mu1 and mu2
yfound = y2
# We found bounds. What if the next loop is never run ?
# i.e. x1 or x2 are close to the solution
# we have to know which one is the best ....
if abs(y1-yvalue)< abs(y2-yvalue) :
x=x1
else:
x=x2
#Now let's refine our mu....
while (nbre_loop<= MaxNbreLoop) and (abs(yfound-yvalue)>Precision_on_y) :
nbre_loop +=1
x = x1 + (x2 - x1) * (yvalue - y1)/(y2-y1)
yfound = Function(x)
if (y1-yvalue)*(yfound - yvalue)>0 :
x1 = x; y1=yfound
else :
x2= x;y2=yfound;
if verbosity>2 :
MPI.report("%(PR)s%(x1)f < %(xname)s < %(x2)f"%locals())
MPI.report("%(PR)s%(y1)f < %(yname)s < %(y2)f"%locals())
if abs(yfound - yvalue) < Precision_on_y :
if verbosity>0:
MPI.report("%(PR)s%(xname)s found in %(nbre_loop)d iterations : "%locals())
MPI.report("%(PR)s%(yname)s = %(yfound)f;%(xname)s = %(x)f"%locals())
return (x,yfound)
else :
if verbosity>0:
MPI.report("%(PR)sFAILURE to adjust %(xname)s to the value %(yvalue)f after %(nbre_loop)d iterations."%locals())
return (None,None)
def SetDoubleCounting(self, densmat, U_interact, J_Hund, orb=0, useDCformula=0, useval=None):
"""Sets the double counting term for inequiv orbital orb
useDCformula=0: LDA+U FLL double counting, useDCformula=1: Held's formula.
useDCformula=2: AMF
Be sure that you use the correct interaction Hamiltonian!"""
# if (not hasattr(self,"dc_imp")): self.__initDC()
dm = [{} for i in xrange(self.N_corr_shells)]
for i in xrange(self.N_corr_shells):
l = self.corr_shells[i][3] # *(1+self.corr_shells[i][4])
for j in xrange(len(self.GFStruct_corr[i])):
dm[i]["%s" % self.GFStruct_corr[i][j][0]] = numpy.zeros([l, l], numpy.float_)
for icrsh in xrange(self.N_corr_shells):
iorb = self.shellmap[icrsh] # iorb is the index of the inequivalent shell corresponding to icrsh
if iorb == orb:
# do this orbital
l = self.corr_shells[icrsh][3] # *(1+self.corr_shells[icrsh][4])
for j in xrange(len(self.GFStruct_corr[icrsh])):
self.dc_imp[icrsh]["%s" % self.GFStruct_corr[icrsh][j][0]] = numpy.identity(l, numpy.float_)
# transform the CTQMC blocks to the full matrix:
for ibl in range(len(self.GFStruct_Solver[iorb])):
for i in range(len(self.GFStruct_Solver[iorb][ibl][1])):
for j in range(len(self.GFStruct_Solver[iorb][ibl][1])):
bl = self.GFStruct_Solver[iorb][ibl][0]
ind1 = self.GFStruct_Solver[iorb][ibl][1][i]
ind2 = self.GFStruct_Solver[iorb][ibl][1][j]
dm[icrsh][self.mapinv[iorb][bl]][ind1, ind2] = densmat[bl][
i, j
].real # only real part relevant for trace
M = self.corr_shells[icrsh][3]
Ncr = {}
Ncrtot = 0.0
a_list = [a for a, al in self.GFStruct_corr[icrsh]]
for bl in a_list:
Ncr[bl] = dm[icrsh][bl].trace()
Ncrtot += Ncr[bl]
# average the densities if there is no SP:
if self.SP == 0:
for bl in a_list:
Ncr[bl] = Ncrtot / len(a_list)
# correction for SO: we have only one block in this case, but in DC we need N/2
elif self.SP == 1 and self.SO == 1:
for bl in a_list:
Ncr[bl] = Ncrtot / 2.0
if useval is None:
if useDCformula == 0:
self.DCenerg[icrsh] = U_interact / 2.0 * Ncrtot * (Ncrtot - 1.0)
for bl in a_list:
Uav = U_interact * (Ncrtot - 0.5) - J_Hund * (Ncr[bl] - 0.5)
self.dc_imp[icrsh][bl] *= Uav
self.DCenerg[icrsh] -= J_Hund / 2.0 * (Ncr[bl]) * (Ncr[bl] - 1.0)
MPI.report("DC for shell %(icrsh)i and block %(bl)s = %(Uav)f" % locals())
elif useDCformula == 1:
self.DCenerg[icrsh] = (
(U_interact + J_Hund * (2.0 - (M - 1)) / (2 * M - 1)) / 2.0 * Ncrtot * (Ncrtot - 1.0)
)
for bl in a_list:
# Held's formula, with U_interact the interorbital onsite interaction
Uav = (U_interact + J_Hund * (2.0 - (M - 1)) / (2 * M - 1)) * (Ncrtot - 0.5)
self.dc_imp[icrsh][bl] *= Uav
MPI.report("DC for shell %(icrsh)i and block %(bl)s = %(Uav)f" % locals())
elif useDCformula == 2:
self.DCenerg[icrsh] = 0.5 * U_interact * Ncrtot * Ncrtot
for bl in a_list:
# AMF
Uav = U_interact * (Ncrtot - Ncr[bl] / M) - J_Hund * (Ncr[bl] - Ncr[bl] / M)
self.dc_imp[icrsh][bl] *= Uav
self.DCenerg[icrsh] -= (U_interact + (M - 1) * J_Hund) / M * 0.5 * Ncr[bl] * Ncr[bl]
MPI.report("DC for shell %(icrsh)i and block %(bl)s = %(Uav)f" % locals())
# output:
MPI.report("DC energy for shell %s = %s" % (icrsh, self.DCenerg[icrsh]))
else:
a_list = [a for a, al in self.GFStruct_corr[icrsh]]
for bl in a_list:
self.dc_imp[icrsh][bl] *= useval
self.DCenerg[icrsh] = useval * Ncrtot
# output:
MPI.report("DC for shell %(icrsh)i = %(useval)f" % locals())
MPI.report("DC energy = %s" % self.DCenerg[icrsh])
