def setup_impurity_solver(self,
mesh_param={},
sp={},
nrgp={},
verbose_nrg=False):
self.cp.update(
mesh_param
) # dictionary cp is set up by model-specific constructor of the derived class, but we need to add mesh_parameters
self.S = Solver(**self.cp)
self.S.set_verbosity(verbose_nrg)
self.sp.update(sp) # add remaining solve parameters
self.nrgp.update(nrgp) # optionally add low-level NRG parameters
self.S.set_nrg_params(**self.nrgp)
# Now we initialize the physical quantities
Sigma, mu = self.initial_Sigma_mu(
) # Get initial self-energy and chemical potential
Gloc, Delta = self_consistency(
Sigma, mu, self.ht
) # Initialize local GF Gloc and hybridization function Delta
Gloc, Delta, mu = self.adjust_mu(
Delta, Sigma, mu
) # Adjust mu toward satisfying occupancy goal (and return updated Glocal and Delta as well)
self.Gloc = Gloc.copy() # Initial approximation for local lattice GF
self.Delta = Delta.copy(
) # Initial approximation for hybridization function
self.set_mu(mu) # Sets mu and updates the impurity level
class test_2orb(unittest.TestCase):
# Construct Parameters
cp = {}
cp["model"] = "2orb-UJ"
cp["symtype"] = "QS"
cp["mesh_max"] = 1.0
cp["mesh_min"] = 1e-1
cp["mesh_ratio"] = 1.1
# Set up the Solver
S = Solver(**cp)
# Solve Parameters
sp = {}
sp["T"] = 1e-1
sp["Lambda"] = 4.0
sp["Nz"] = 1
sp["Tmin"] = 0.5
sp["keep"] = 2000
sp["keepenergy"] = 10.0
# Model Parameters
mp = {}
mp["U1"] = 1.0
mp["U2"] = 0.9
mp["eps1"] = -0.5
mp["eps2"] = -0.4
mp["U12"] = 0.1
mp["J12"] = 0.05
sp["model_parameters"] = mp
# Low-level NRG Parameters
np = {}
np["bins"] = 50
S.set_nrg_params(**np)
# # Initialize hybridization function
S.Delta_w['imp'][0,0] << 0.5 * SemiCircular(1.0)
S.Delta_w['imp'][1,1] << 0.4 * SemiCircular(1.0)
# Out-of-diagonal Delta is zero
# Solve the impurity model
S.solve(**sp)
# # Store the Result
with HDFArchive("3_2orb-UJ_QS.out.h5", 'w') as arch:
arch["A_w"] = S.A_w
arch["G_w"] = S.G_w
arch["F_w"] = S.F_w
arch["Sigma_w"] = S.Sigma_w
# Compare against reference result
h5diff("3_2orb-UJ_QS.out.h5", "3_2orb-UJ_QS.ref.h5")
class test_SIAM(unittest.TestCase):
# Construct Parameters
cp = {}
cp["model"] = "SIAM"
cp["symtype"] = "QS"
cp["mesh_max"] = 1.0
cp["mesh_min"] = 1e-3
cp["mesh_ratio"] = 1.1
# Set up the Solver
S = Solver(**cp)
# Solve Parameters
sp = {}
sp["T"] = 1e-3
sp["Lambda"] = 4.0
sp["Nz"] = 4
sp["Tmin"] = 1e-4
sp["keep"] = 50
sp["keepenergy"] = 6.0
# Model Parameters
mp = {}
mp["U1"] = 0.5
mp["eps1"] = -0.24
sp["model_parameters"] = mp
# Low-level NRG Parameters
np = {}
np["bins"] = 50
S.set_nrg_params(**np)
# # Initialize hybridization function
S.Delta_w['imp'] << 0.1 * SemiCircular(1.0)
# Solve the impurity model
S.solve(**sp)
if mpi.is_master_node():
# Store the Result
fnout = "MPI_SIAM_QS_np%i.out.h5" % mpi.size
with HDFArchive(fnout, 'w') as arch:
arch["A_w"] = S.A_w
arch["G_w"] = S.G_w
arch["F_w"] = S.F_w
arch["Sigma_w"] = S.Sigma_w
# Compare against reference result
fnref = "MPI_SIAM_QS.ref.h5" # the same for all cases!
h5diff(fnout, fnref)
class test_SIAM(unittest.TestCase):
# Construct Parameters
cp = {}
cp["model"] = "SIAM"
cp["symtype"] = "QSZ"
cp["mesh_max"] = 1.0
cp["mesh_min"] = 1e-3
cp["mesh_ratio"] = 1.1
# Set up the Solver
S = Solver(**cp)
# Solve Parameters
sp = {}
sp["T"] = 1e-3
sp["Lambda"] = 4.0
sp["Nz"] = 2
sp["Tmin"] = 1e-4
sp["keep"] = 50
sp["keepenergy"] = 6.0
# Model Parameters
mp = {}
mp["U1"] = 0.5
mp["eps1"] = -0.24
mp["B1"] = -0.1
sp["model_parameters"] = mp
# Low-level NRG Parameters
np = {}
np["bins"] = 50
S.set_nrg_params(**np)
# # Initialize hybridization function
S.Delta_w['up'] << 0.05 * SemiCircular(1.0)
S.Delta_w['dn'] << 0.1 * SemiCircular(1.0)
# Solve the impurity model
S.solve(**sp)
# # Store the Result
with HDFArchive("2_SIAM_QSZ.out.h5", 'w') as arch:
arch["A_w"] = S.A_w
arch["G_w"] = S.G_w
arch["F_w"] = S.F_w
arch["Sigma_w"] = S.Sigma_w
# Compare against reference result
h5diff("2_SIAM_QSZ.out.h5", "2_SIAM_QSZ.ref.h5")
class test_SIAM(unittest.TestCase):
# Construct Parameters
cp = {}
cp["model"] = "SIAM"
cp["symtype"] = "QS"
cp["mesh_max"] = 1.0
cp["mesh_min"] = 1e-3
cp["mesh_ratio"] = 1.1
# Set up the Solver
S = Solver(**cp)
# Solve Parameters
sp = {}
sp["T"] = 1e-3
sp["Lambda"] = 4.0
sp["Nz"] = 2
sp["Tmin"] = 1e-4
sp["keep"] = 50
sp["keepenergy"] = 6.0
# Model Parameters
mp = {}
mp["U1"] = 0.5
mp["eps1"] = -0.24
sp["model_parameters"] = mp
# Low-level NRG Parameters
np = {}
np["bins"] = 50
S.set_nrg_params(**np)
# # Initialize hybridization function
S.Delta_w['imp'] << 0.1 * SemiCircular(1.0)
# Solve the impurity model
S.solve(**sp)
if mpi.is_master_node(): HDFArchive('Solver.h5', 'w')['S'] = S
# Rerun the Solver and Compare
S_old = HDFArchive('Solver.h5', 'r')['S']
S_old.solve(**S_old.last_solve_params)
assert_block_gfs_are_close(S_old.G_w, S.G_w, 1e-12)
class test_SIAM(unittest.TestCase):
# Construct Parameters
cp = {}
cp["model"] = "SIAM"
cp["symtype"] = "QS"
cp["mesh_max"] = 1.0
cp["mesh_min"] = 1e-3
cp["mesh_ratio"] = 1.1
# Set up the Solver
S = Solver(**cp)
# Solve Parameters
sp = {}
sp["T"] = 1e-3
sp["Lambda"] = 4.0
sp["Nz"] = 2
sp["Tmin"] = 1e-4
sp["keep"] = 50
sp["keepenergy"] = 6.0
# Model Parameters
mp = {}
mp["U1"] = 0.5
mp["eps1"] = -0.24
sp["model_parameters"] = mp
# Low-level NRG Parameters
np = {}
np["bins"] = 50
S.set_nrg_params(**np)
# # Initialize hybridization function
S.Delta_w['imp'] << 0.1 * SemiCircular(1.0)
# Solve the impurity model
S.solve(**sp)
G_w_1 = S.G_w.copy()
S.solve(**sp)
G_w_2 = S.G_w.copy()
assert_block_gfs_are_close(G_w_1, G_w_2, 1e-12)
from nrgljubljana_interface import Solver, Flat
from h5 import *
# Parameters
D, V, U = 1.0, 0.25, 1.0
e_f = -U / 2.0 # particle-hole symmetric case
T = 1e-5
# Set up the Solver
S = Solver(model="SIAM",
symtype="QS",
mesh_max=2.0,
mesh_min=1e-5,
mesh_ratio=1.01)
# Solve Parameters
sp = {
"T": T,
"Lambda": 2.0,
"Nz": 4,
"Tmin": 1e-6,
"keep": 2000,
"keepenergy": 10.0,
"bandrescale": 1.0
}
# Model Parameters
mp = {"U1": U, "eps1": e_f}
sp["model_parameters"] = mp
# Initialize hybridization function
from pytriqs.archive import *
import math
# Parameters
D = 1.0 # bandwidth
U = 1.0
Gamma = 0.1
e_f = -0.4
U12 = 1.0
J12 = 0.0
T = 1e-3
# Set up the Solver
S = Solver(model="2orb-UJ",
symtype="QS",
mesh_max=2.00676,
mesh_min=1e-5,
mesh_ratio=1.01)
# Solve Parameters
sp = {
"T": T,
"Lambda": 4.0,
"Nz": 4,
"Tmin": 1e-5,
"keep": 4000,
"keepenergy": 10.0,
"bandrescale": 1.0
}
# Model Parameters
from nrgljubljana_interface import Solver, Flat
from pytriqs.archive import *
# Parameters
D, V, U = 1.0, 0.2, 0 # Zero e-e interaction
e_f = -U / 2.0 # particle-hole symmetric case
T = 1e-5
omega = 0.2 # phonon frequency
g1 = 0.2 # electron-phonon coupling strength
n1 = 1 # n1 in g1*(a+a^dag)*(n-n1)
# Set up the Solver
S = Solver(model="Holstein/Nph=10",
symtype="QS",
mesh_max=2.0,
mesh_min=1e-5,
mesh_ratio=1.01)
# Solve Parameters
sp = {
"T": T,
"Lambda": 2.0,
"Nz": 4,
"Tmin": 1e-6,
"keep": 1000,
"keepenergy": 10.0,
"bandrescale": 1.0
}
# Model Parameters
mp = {"U1": U, "eps1": e_f, "omega": omega, "g1": g1, "n1": n1}
class DMFT_solver(object):
itern = 0 # iteration counter
okn = 0 # number of iterations in which convergent criteria were satisfied
solution_filename = "solution.h5" # converged solution (all convergence criteria satisfied)
checkpoint_filename = "checkpoint.h5" # current solution (for checkpoint/restart functionality)
stats_filename = "stats.dat" # some statistics about the DMFT iteration
stop_flag_file = "STOP" # the calculation can be aborted by creating this file
converged_flag_file = "CONVERGED" # the script touches this file upon reaching convergence
# Provides the initial Sigma and mu
def initial_Sigma_mu(self):
if os.path.isfile(self.checkpoint_filename
): # continue DMFT iteration after interruption
return restart_calculation(self.checkpoint_filename)
elif os.path.isfile(
self.solution_filename
): # continue DMFT iteration after failed convergence
return restart_calculation(self.solution_filename)
else: # start from scratch
return self.new_calculation()
def __init__(self, param, dmft_param):
self.param = param
self.dmft_param = dmft_param
self.occupancy_goal = param["occupancy"]
self.T = param["T"]
self.observables = [] # List of expectation values to compute
self.cp = {} # Dictinary with creator parameters
self.sp = {
"T": self.T,
"model_parameters": {}
} # Dictionary with solver parameters
self.mp = {} # Dictionary with model parameters
self.nrgp = {
} # Dictionary with low-level NRG Parameters (optional tweaks)
# Open file with basic information (convergence criteria, occupancy, expectation values of operators) for monitoring the iteration process
if mpi.is_master_node():
self.stats_file = open(self.stats_filename, "w",
buffering=1) # line buffered
# Initialize a function ht0 for calculating the Hilbert transform of the DOS
if (param["dos"] == "Bethe"):
self.ht1 = lambda z: 2 * (
z - 1j * np.sign(z.imag) * np.sqrt(1 - z**2)
) # Analytical expression for Hilbert transform of Bethe lattice DOS
self.ht0 = lambda z: self.ht1(z / param["Bethe_unit"])
else:
table = np.loadtxt(param["dos"])
self.dosA = Gf(mesh=MeshReFreqPts(table[:, 0]), target_shape=[])
for i, w in enumerate(self.dosA.mesh):
self.dosA[w] = np.array([[table[i, 1]]])
self.ht0 = lambda z: hilbert_transform_refreq(self.dosA, z)
# Performs the Hilbert transform with argument z, ensuring that the imaginary part is positive (to produce retarded GFs)
def ht(self, z, EPS=1e-20):
return self.ht0(z.real + 1j * (z.imag if z.imag > 0.0 else EPS)
) # Fix problems due to causality violation
# Model specific changes to the impurity model parameters need to be defined in derived classes
def set_mu(self, mu):
self.mu = mu
# This may be called after all constructors (base and all derived classes) have done their job
def setup_impurity_solver(self,
mesh_param={},
sp={},
nrgp={},
verbose_nrg=False):
self.cp.update(
mesh_param
) # dictionary cp is set up by model-specific constructor of the derived class, but we need to add mesh_parameters
self.S = Solver(**self.cp)
self.S.set_verbosity(verbose_nrg)
self.sp.update(sp) # add remaining solve parameters
self.nrgp.update(nrgp) # optionally add low-level NRG parameters
self.S.set_nrg_params(**self.nrgp)
# Now we initialize the physical quantities
Sigma, mu = self.initial_Sigma_mu(
) # Get initial self-energy and chemical potential
Gloc, Delta = self_consistency(
Sigma, mu, self.ht
) # Initialize local GF Gloc and hybridization function Delta
Gloc, Delta, mu = self.adjust_mu(
Delta, Sigma, mu
) # Adjust mu toward satisfying occupancy goal (and return updated Glocal and Delta as well)
self.Gloc = Gloc.copy() # Initial approximation for local lattice GF
self.Delta = Delta.copy(
) # Initial approximation for hybridization function
self.set_mu(mu) # Sets mu and updates the impurity level
# Iteratively adjust mu, taking into account the self-consistency equation.
# Returns an improved estimate for the hybridisation function.
def adjust_mu(self, Delta_in, Sigma, old_mu):
Delta = Delta_in.copy()
mu = old_mu
max_mu_adjust = self.dmft_param.get(
"max_mu_adjust", 10
) # number of cycles for adjusting the value of the chemical potential
for _ in range(max_mu_adjust):
mu = update_mu(Delta, Sigma, self.occupancy_goal, self.T, mu)
Gloc, Delta = self_consistency(Sigma, mu, self.ht)
new_mu = mu
max_mu_diff = self.dmft_param.get(
"max_mu_diff", None) # maximum change in mu that is allowed
if max_mu_diff is not None:
new_mu = clamp(old_mu - max_mu_diff, new_mu, old_mu + max_mu_diff)
mu_alpha = self.dmft_param.get(
"mu_alpha",
1.0) # mixing parameter for the chemical potential adjustment
new_mu = mu_alpha * new_mu + (1.0 - mu_alpha) * old_mu
if verbose():
print("Adjusted mu from %.10f to %.10f" % (old_mu, new_mu))
return Gloc, Delta, new_mu
def set_model_parameters(self, mp):
for k, v in mp.items():
if v is None:
del mp[k] # Remove undefined parameters from the dictionary
self.sp["model_parameters"].update(mp) # Update, not an assignment!
# Store the complete set of results
def store_result(self, fn):
with HDFArchive(fn, 'w') as arch:
arch["S"] = self.S
arch["Gloc"] = self.Gloc
arch["Delta"] = self.Delta
arch["mu"] = self.mu
arch["Gself"] = self.Gself
arch["occupancy"] = self.occupancy
# Perform a DMFT step. Input is the hybridization function for solving the effective impurity model,
# output is a new hybridization function resulting from the application of the DMFT self-consistency equation.
def dmft_step(self, Delta_in):
self.itern += 1
if verbose():
print("\nIteration %i min_iter=%i max_iter=%i" %
(self.itern, self.dmft_param["min_iter"],
self.dmft_param["max_iter"]))
Delta_in_fixed = fix_hyb_function(Delta_in,
self.dmft_param["Delta_min"])
self.S.Delta_w << Delta_in_fixed
t0 = timeit.default_timer()
self.S.solve(**self.sp) # Solve the impurity model
t1 = timeit.default_timer()
dt = int(t1 - t0)
solver_time = '{:02}:{:02}:{:02}'.format(dt // 3600, dt % 3600 // 60,
dt % 60) # hh:mm:ss format
self.Gself = calc_G(
Delta_in_fixed, self.S.Sigma_w,
self.mu) # impurity GF ("self-energy-trick" improved)
Gloc_prev = self.Gloc.copy(
) # store copy of previous Gloc for checking convergence
self.Gloc, self.Delta = self_consistency(
self.S.Sigma_w, self.mu,
self.ht) # apply the DMFT self-consistency equation
self.occupancy = calc_occupancy(
self.Delta, self.S.Sigma_w, self.mu,
self.T) # occupancy calculated from the local lattice GF
diff_loc_imp = gf_diff(
self.Gself,
self.Gloc) # difference between impurity and local lattice GF
diff_prev = gf_diff(
self.Gloc, Gloc_prev
) # difference between two consecutively computed local latice GFs
diff_occupancy = abs(
self.occupancy - self.occupancy_goal
) # this difference is used as the measure of deviation
stats = OrderedDict([("itern", self.itern), ("time", solver_time),
("mu", self.mu), ("diff_loc_imp", diff_loc_imp),
("diff_prev", diff_prev),
("diff_occupancy", diff_occupancy),
("occupancy", self.occupancy)])
for i in self.observables:
stats[i] = self.S.expv[i]
header_string = fmt_str_header(
len(stats)).format(*[i for i in stats.keys()])
stats_string = fmt_str(len(stats)).format(*[i for i in stats.values()])
if mpi.is_master_node():
if self.itern == 1:
print(header_string, file=self.stats_file)
print(stats_string, file=self.stats_file)
if verbose():
print(header_string)
print(stats_string)
if self.dmft_param["store_steps"] and mpi.is_master_node():
os.mkdir(str(self.itern)) # one subdirectory per iteration
save_BlockGf(str(self.itern) + "/Delta", Delta_in_fixed)
save_BlockGf(str(self.itern) + "/Sigma",
self.S.Sigma_w) # self-energy
save_BlockGf(str(self.itern) + "/G",
self.Gloc) # local lattice Green's function
save_BlockA(str(self.itern) + "/A",
self.Gloc) # spectral function of local lattice GF
self.store_result(str(self.itern) + "/" + self.solution_filename)
if mpi.is_master_node():
self.store_result(self.checkpoint_filename
) # for checkpoint/restart functionality
# Check for convergence
if (diff_loc_imp < self.dmft_param["eps_loc_imp"]
and diff_prev < self.dmft_param["eps_prev"]
and diff_occupancy < self.dmft_param["eps_occupancy"]):
self.okn += 1
else:
self.okn = 0
# The only way to exit the DMFT loop is by generating exceptions.
if (self.okn >= self.dmft_param.get("conv_iter", 1)
and self.itern >= self.dmft_param["min_iter"]):
if mpi.is_master_node():
self.store_result(self.solution_filename
) # full converged results as an HDF5 file
try:
os.remove(self.checkpoint_filename
) # checkpoint file is no longer needed
except OSError:
pass
if self.converged_flag_file:
touch(self.converged_flag_file
) # signal convergence through a file
raise Converged("%s\n%s" % (header_string, stats_string))
if (self.itern == self.dmft_param["max_iter"]):
raise FailedToConverge("%s\n%s" % (header_string, stats_string))
if self.stop_flag_file and os.path.isfile(self.stop_flag_file):
raise ForcedStop()
if self.dmft_param["occup_method"] == "adjust":
self.Gloc, self.Delta, new_mu = self.adjust_mu(
self.Delta, self.S.Sigma_w,
self.mu) # here we update mu to get closer to target occupancy
self.set_mu(new_mu)
return self.Delta
# DMFT driver routine with linear mixing
def solve_with_linear_mixing(self, alpha, mixer_param):
Delta_in = self.Delta.copy()
while True:
Delta_out = self.dmft_step(Delta_in)
newDelta = alpha * Delta_out + (1 - alpha) * Delta_in
Delta_in << newDelta
# DMFT driver routine with Broyden mixing: the goal is to find a root of the function F(Delta)=dmft_step(Delta)-Delta.
def solve_with_broyden_mixing(self, alpha, broyden_param):
if self.dmft_param["occup_method"] == "broyden":
def F(Delta_in, mu):
if verbose():
print("(Broyden) Setting mu to %.18f" % mu)
self.set_mu(mu)
Delta_out = self.dmft_step(Delta_in)
occup_factor = self.dmft_param.get("occup_factor", 1.0)
return Delta_out - Delta_in, occup_factor * (
self.occupancy_goal - self.occupancy)
npF = lambda x: wrap(*F(*unwrap(x, self.S, scalar=True))
) # unpack the tuples
xin = wrap(self.Delta, self.mu)
else:
def F(Delta):
return self.dmft_step(Delta) - Delta
npF = lambda x: bgf_to_nparray(F(nparray_to_bgf(x, self.S)))
xin = bgf_to_nparray(self.Delta)
bp = {
"reduction_method": "svd",
"max_rank": 20,
"f_tol": 1e-99
} # Loop forever (small f_tol!)
bp.update(broyden_param)
optimize.broyden1(npF, xin, alpha=alpha, verbose=verbose(), **bp)
raise Converged("broyden1() converged")
def solve(self):
alpha = self.dmft_param["alpha"]
if (self.dmft_param["mixing_method"] == "linear"):
self.solve_with_linear_mixing(alpha)
if (self.dmft_param["mixing_method"] == "broyden"):
self.solve_with_broyden_mixing(
alpha, self.dmft_param.get("broyden_param", {}))
# Additional quantities of interest
observables = ["n_d", "n_d^2"]
if B is not None:
observables.extend(["SZd"])
if "Holstein" in model:
observables.extend(["nph", "displ", "displ^2"])
# Run-time global variables
itern = 0 # iteration counter
verbose = verbose and mpi.is_master_node() # output is only produced by the master node
store_steps = store_steps and mpi.is_master_node() # output is only produced by the master node
symtype = ("QS" if B is None else "QSZ")
# Set up the Solver
S = Solver(model=model, symtype=symtype, mesh_max=mesh_max, mesh_min=mesh_min, mesh_ratio=mesh_ratio)
S.set_verbosity(verbose_nrg)
newG = lambda : S.G_w.copy() # Creates a BlockGf object of appropriate structure
nr_blocks = lambda bgf : len([bl for bl in bgf.indices]) # Returns the number of blocks in a BlockGf object
block_size = lambda bl : len(S.G_w[bl].indices[0]) # Matrix size of Green's functions in block 'bl'
identity = lambda bl : np.identity(block_size(bl)) # Returns the identity matrix in block 'bl'
# Solve Parameters
sp = { "T": T, "Lambda": 2.0, "Nz": 4, "Tmin": 1e-5, "keep": 10000, "keepenergy": 10.0 }
# Model Parameters
mp = { "U1": U, "B1": B, "omega": omega, "g1": g1, "n1": n1 }
for k,v in mp.items():
if v is None: del mp[k] # Remove undefined parameters from the dictionary
sp["model_parameters"] = mp
