mirror of
https://github.com/triqs/dft_tools
synced 2024-09-12 05:38:31 +02:00
Corrections for new calc_dc and calc_mu
* typos and subbed check in spin polarized calculations for quantum espresso with a warning when computing the deltaN * fixed typos in comments * removed legacy mode maintaining only compatibility layer and switched to old (<3.10) python syntax * added target density output in mu finder for brent and newton, refactored tunit test for DC, changed some comments
This commit is contained in:
parent
d4f3c48784
commit
0d25aefc73
1
.gitignore
vendored
1
.gitignore
vendored
@ -1,3 +1,2 @@
|
||||
compile_commands.json
|
||||
doc/cpp2rst_generated
|
||||
build/
|
||||
|
@ -38,10 +38,11 @@ from warnings import warn
|
||||
from scipy import compress
|
||||
from scipy.optimize import minimize, newton, brenth
|
||||
|
||||
def compute_DC_from_density(N_tot, U, J, N_spin = None, n_orbitals=5, method='cFLL'):
|
||||
def compute_DC_from_density(N_tot, U, J, N_spin = None, n_orbitals=5, method='sFLL'):
|
||||
"""
|
||||
Computes the double counting correction in terms using various methods
|
||||
|
||||
Computes the double counting correction using various methods.
|
||||
For FLL and AMF DC the notations and equations from doi.org/10.1038/s41598-018-27731-4
|
||||
are used, whereas for the Held DC the definitions from doi.org/10.1080/00018730701619647 are used.
|
||||
|
||||
Parameters
|
||||
----------
|
||||
@ -69,45 +70,48 @@ def compute_DC_from_density(N_tot, U, J, N_spin = None, n_orbitals=5, method='
|
||||
List of floats:
|
||||
- DC_val: double counting potential
|
||||
- E_val: double counting energy
|
||||
|
||||
|
||||
todo: See whether to move this to TRIQS directly instead of dft_tools
|
||||
"""
|
||||
if N_spin is not None:
|
||||
N_spin2 = N_tot-N_spin
|
||||
Mag = N_spin - N_spin2
|
||||
L_orbit = (n_orbitals-1)/2
|
||||
|
||||
match method:
|
||||
case 'cFLL':
|
||||
E_val = 0.5 * U * N_tot * (N_tot-1) - 0.5 * J * N_tot * (N_tot*0.5-1)
|
||||
DC_val = U * (N_tot-0.5) - J *(N_tot*0.5-0.5)
|
||||
if method == 'cFLL':
|
||||
E_val = 0.5 * U * N_tot * (N_tot-1) - 0.5 * J * N_tot * (N_tot*0.5-1)
|
||||
DC_val = U * (N_tot-0.5) - J *(N_tot*0.5-0.5)
|
||||
|
||||
case 'sFLL':
|
||||
assert N_spin is not None, "Spin density not given"
|
||||
E_val = 0.5 * U * N_tot * (N_tot-1) - 0.5 * J * N_tot * (N_tot*0.5-1) - 0.25 * J * Mag**2
|
||||
DC_val = U * (N_tot-0.5) - J *(N_spin-0.5)
|
||||
elif method == 'sFLL':
|
||||
assert N_spin is not None, "Spin density not given"
|
||||
E_val = 0.5 * U * N_tot * (N_tot-1) - 0.5 * J * N_tot * (N_tot*0.5-1) - 0.25 * J * Mag**2
|
||||
DC_val = U * (N_tot-0.5) - J *(N_spin-0.5)
|
||||
|
||||
case 'cAMF':
|
||||
E_val = +0.5 * U * N_tot **2
|
||||
E_val -= 0.25*(U+2*L_orbit*J)/(2*L_orbit+1)*N_tot**2
|
||||
DC_val = U * N_tot - 0.5*(U+2*L_orbit*J)/(2*L_orbit+1)*N_tot
|
||||
elif method == 'cAMF':
|
||||
E_val = +0.5 * U * N_tot **2
|
||||
E_val -= 0.25*(U+2*L_orbit*J)/(2*L_orbit+1)*N_tot**2
|
||||
DC_val = U * N_tot - 0.5*(U+2*L_orbit*J)/(2*L_orbit+1)*N_tot
|
||||
|
||||
|
||||
case 'sAMF':
|
||||
assert N_spin is not None, "Spin density not given"
|
||||
E_val = 0.5 * U * N_tot **2
|
||||
E_val -= 0.25*(U+2*L_orbit*J)/(2*L_orbit+1)*N_tot**2
|
||||
E_val -= 0.25*(U+2*L_orbit*J)/(2*L_orbit+1)*Mag**2
|
||||
DC_val = U * N_tot - (U+2*L_orbit*J)/(2*L_orbit+1)*N_spin
|
||||
elif method == 'sAMF':
|
||||
assert N_spin is not None, "Spin density not given"
|
||||
E_val = 0.5 * U * N_tot **2
|
||||
E_val -= 0.25*(U+2*L_orbit*J)/(2*L_orbit+1)*N_tot**2
|
||||
E_val -= 0.25*(U+2*L_orbit*J)/(2*L_orbit+1)*Mag**2
|
||||
DC_val = U * N_tot - (U+2*L_orbit*J)/(2*L_orbit+1)*N_spin
|
||||
|
||||
case 'cHeld':
|
||||
U_mean = (U + (n_orbitals-1)*(U-2*J)+(n_orbitals-1)*(U-3*J))/(2*n_orbitals-1)
|
||||
E_val = 0.5 * U_mean * N_tot * (N_tot - 1)
|
||||
DC_val = U_mean * (N_tot-0.5)
|
||||
elif method == 'cHeld':
|
||||
# Valid for a Kanamori-type Hamiltonian where U'=U-2J
|
||||
U_mean = (U + (n_orbitals-1)*(U-2*J)+(n_orbitals-1)*(U-3*J))/(2*n_orbitals-1)
|
||||
E_val = 0.5 * U_mean * N_tot * (N_tot - 1)
|
||||
DC_val = U_mean * (N_tot-0.5)
|
||||
|
||||
case 'sHeld':
|
||||
raise ValueError(f"Method sHeld not yet implemented")
|
||||
elif method == 'sHeld':
|
||||
raise ValueError(f"Method sHeld not yet implemented")
|
||||
|
||||
case _:
|
||||
raise ValueError(f"DC type {method} not supported")
|
||||
else:
|
||||
raise ValueError(f"DC type {method} not supported")
|
||||
|
||||
mpi.report(f"DC potential computed using the {method} method, V_DC = {DC_val:.6f} eV")
|
||||
mpi.report(f"E_DC using the {method} method, E_DC = {E_val:.6f} eV")
|
||||
@ -1735,7 +1739,7 @@ class SumkDFT(object):
|
||||
self.dc_energ = dc_energ
|
||||
|
||||
def calc_dc(self, dens_mat, orb=0, U_interact=None, J_hund=None,
|
||||
use_dc_formula=0, use_dc_value=None, transform=True, legacy=True):
|
||||
use_dc_formula=0, use_dc_value=None, transform=True):
|
||||
r"""
|
||||
Calculate and set the double counting corrections.
|
||||
|
||||
@ -1767,8 +1771,13 @@ class SumkDFT(object):
|
||||
Value of interaction parameter `U`.
|
||||
J_hund : float, optional
|
||||
Value of interaction parameter `J`.
|
||||
use_dc_formula : int, optional
|
||||
Type of double-counting correction (see description).
|
||||
use_dc_formula : int or string, optional
|
||||
Type of double-counting correction (see description of `compute_DC_from_density` above).
|
||||
There is an interface with the legacy implementation which allows for the old convention:
|
||||
* 0 -> 'sFLL' spin dependent fully localized limit
|
||||
* 1 -> 'cHeld' spin independent Held formula
|
||||
* 2 -> 'sAMF' spin dependent around-mean field approximation
|
||||
|
||||
use_dc_value : float, optional
|
||||
Value of the double-counting correction. If specified
|
||||
`U_interact`, `J_hund` and `use_dc_formula` are ignored.
|
||||
@ -1807,68 +1816,21 @@ class SumkDFT(object):
|
||||
dim //= 2
|
||||
|
||||
if use_dc_value is None:
|
||||
if legacy:
|
||||
#For legacy compatibility
|
||||
if use_dc_formula == 0:
|
||||
mpi.report(f"Detected {use_dc_formula=}, changing to sFLL")
|
||||
use_dc_formula = "sFLL"
|
||||
if use_dc_formula == 1:
|
||||
mpi.report(f"Detected {use_dc_formula=}, changing to cHeld")
|
||||
use_dc_formula = "cHeld"
|
||||
if use_dc_formula == 2:
|
||||
mpi.report(f"Detected {use_dc_formula=}, changing to sAMF")
|
||||
use_dc_formula = "sAMF"
|
||||
|
||||
if U_interact is None and J_hund is None:
|
||||
raise ValueError("set_dc: either provide U_interact and J_hund or set use_dc_value to dc value.")
|
||||
|
||||
if use_dc_formula == 0: # FLL
|
||||
|
||||
self.dc_energ[icrsh] = U_interact / \
|
||||
2.0 * Ncrtot * (Ncrtot - 1.0)
|
||||
for sp in spn:
|
||||
Uav = U_interact * (Ncrtot - 0.5) - \
|
||||
J_hund * (Ncr[sp] - 0.5)
|
||||
self.dc_imp[icrsh][sp] *= Uav
|
||||
self.dc_energ[icrsh] -= J_hund / \
|
||||
len(spn) * (Ncr[sp]) * (Ncr[sp] - 1.0)
|
||||
mpi.report(
|
||||
"DC for shell %(icrsh)i and block %(sp)s = %(Uav)f" % locals())
|
||||
|
||||
elif use_dc_formula == 1: # Held's formula, with U_interact the interorbital onsite interaction
|
||||
|
||||
self.dc_energ[icrsh] = (U_interact + (dim - 1) * (U_interact - 2.0 * J_hund) + (
|
||||
dim - 1) * (U_interact - 3.0 * J_hund)) / (2 * dim - 1) / 2.0 * Ncrtot * (Ncrtot - 1.0)
|
||||
for sp in spn:
|
||||
Uav = (U_interact + (dim - 1) * (U_interact - 2.0 * J_hund) + (dim - 1)
|
||||
* (U_interact - 3.0 * J_hund)) / (2 * dim - 1) * (Ncrtot - 0.5)
|
||||
self.dc_imp[icrsh][sp] *= Uav
|
||||
mpi.report(
|
||||
"DC for shell %(icrsh)i and block %(sp)s = %(Uav)f" % locals())
|
||||
|
||||
elif use_dc_formula == 2: # AMF
|
||||
|
||||
self.dc_energ[icrsh] = 0.5 * U_interact * Ncrtot * Ncrtot
|
||||
for sp in spn:
|
||||
Uav = U_interact * \
|
||||
(Ncrtot - Ncr[sp] / dim) - \
|
||||
J_hund * (Ncr[sp] - Ncr[sp] / dim)
|
||||
self.dc_imp[icrsh][sp] *= Uav
|
||||
self.dc_energ[
|
||||
icrsh] -= (U_interact + (dim - 1) * J_hund) / dim / len(spn) * Ncr[sp] * Ncr[sp]
|
||||
mpi.report(
|
||||
"DC for shell %(icrsh)i and block %(sp)s = %(Uav)f" % locals())
|
||||
|
||||
mpi.report("DC energy for shell %s = %s" %
|
||||
(icrsh, self.dc_energ[icrsh]))
|
||||
|
||||
else:
|
||||
#For legacy compatibility
|
||||
match use_dc_formula:
|
||||
case 0:
|
||||
mpi.report(f"Detected {use_dc_formula=}, changing to sFLL")
|
||||
use_dc_formula = "sFLL"
|
||||
case 1:
|
||||
mpi.report(f"Detected {use_dc_formula=}, changing to cHeld")
|
||||
use_dc_formula = "cHeld"
|
||||
case 2:
|
||||
mpi.report(f"Detected {use_dc_formula=}, changing to sAMF")
|
||||
use_dc_formula = "sAMF"
|
||||
|
||||
for sp in spn:
|
||||
DC_val, E_val = compute_DC_from_density(N_tot=Ncrtot,U=U_interact, J=J_hund, n_orbitals=dim, N_spin=Ncr[sp], method=use_dc_formula)
|
||||
self.dc_imp[icrsh][sp] *= DC_val
|
||||
self.dc_energ[icrsh] -= E_val
|
||||
for sp in spn:
|
||||
DC_val, E_val = compute_DC_from_density(N_tot=Ncrtot,U=U_interact, J=J_hund, n_orbitals=dim, N_spin=Ncr[sp], method=use_dc_formula)
|
||||
self.dc_imp[icrsh][sp] *= DC_val
|
||||
self.dc_energ[icrsh] = E_val
|
||||
|
||||
|
||||
|
||||
@ -2048,7 +2010,6 @@ class SumkDFT(object):
|
||||
def calc_mu(self, precision=0.01, broadening=None, delta=0.5, max_loops=100, method="dichotomy"):
|
||||
r"""
|
||||
Searches for the chemical potential that gives the DFT total charge.
|
||||
A simple bisection method is used.
|
||||
|
||||
Parameters
|
||||
----------
|
||||
@ -2061,7 +2022,7 @@ class SumkDFT(object):
|
||||
max_loops : int, optional
|
||||
Number of dichotomy loops maximally performed.
|
||||
|
||||
max_loops : string, optional
|
||||
method : string, optional
|
||||
Type of optimization used:
|
||||
* dichotomy: usual bisection algorithm from the TRIQS library
|
||||
* newton: newton method, faster convergence but more unstable
|
||||
@ -2116,52 +2077,50 @@ class SumkDFT(object):
|
||||
|
||||
mpi.report("Trying out mu = {}".format(str(mu)))
|
||||
calc_dens = self.total_density(mu=mu, broadening=broadening).real - density
|
||||
mpi.report("Delta to target density = {}".format(str(calc_dens)))
|
||||
mpi.report(f"Target density = {density}; Delta to target = {calc_dens}")
|
||||
return calc_dens
|
||||
|
||||
#check for lowercase matching for the method variable
|
||||
match method.lower():
|
||||
if method.lower()=="dichotomy":
|
||||
mpi.report("\nSUMK calc_mu: Using dichtomy adjustment to find chemical potential\n")
|
||||
self.chemical_potential = dichotomy.dichotomy(function=F_bisection,
|
||||
x_init=self.chemical_potential, y_value=density,
|
||||
precision_on_y=precision, delta_x=delta, max_loops=max_loops,
|
||||
x_name="Chemical Potential", y_name="Total Density",
|
||||
verbosity=3)[0]
|
||||
elif method.lower()=="newton":
|
||||
mpi.report("\nSUMK calc_mu: Using Newton method to find chemical potential\n")
|
||||
self.chemical_potential = newton(func=F_optimize,
|
||||
x0=self.chemical_potential,
|
||||
tol=precision, maxiter=max_loops,
|
||||
)
|
||||
|
||||
case "dichotomy":
|
||||
mpi.report("\nSUMK calc_mu: Using dichtomy adjustment to find chemical potential\n")
|
||||
self.chemical_potential = dichotomy.dichotomy(function=F_bisection,
|
||||
x_init=self.chemical_potential, y_value=density,
|
||||
precision_on_y=precision, delta_x=delta, max_loops=max_loops,
|
||||
x_name="Chemical Potential", y_name="Total Density",
|
||||
verbosity=3)[0]
|
||||
case 'newton':
|
||||
mpi.report("\nSUMK calc_mu: Using Newton method to find chemical potential\n")
|
||||
self.chemical_potential = newton(func=F_optimize,
|
||||
x0=self.chemical_potential,
|
||||
tol=precision, maxiter=max_loops,
|
||||
)
|
||||
elif method.lower()=="brent":
|
||||
mpi.report("\nSUMK calc_mu: Using Brent method to find chemical potential")
|
||||
mpi.report("SUMK calc_mu: Finding bounds \n")
|
||||
|
||||
case 'brent':
|
||||
mpi.report("\nSUMK calc_mu: Using Brent method to find chemical potential")
|
||||
mpi.report("SUMK calc_mu: Finding bounds \n")
|
||||
mu_guess_0, mu_guess_1 = find_bounds(function=F_optimize,
|
||||
x_init=self.chemical_potential,
|
||||
delta_x=delta, max_loops=max_loops,
|
||||
)
|
||||
mu_guess_1 += 0.01 #scrambles higher lying interval to avoid getting stuck
|
||||
mpi.report("\nSUMK calc_mu: Searching root with Brent method\n")
|
||||
self.chemical_potential = brenth(f=F_optimize,
|
||||
a=mu_guess_0,
|
||||
b=mu_guess_1,
|
||||
xtol=precision, maxiter=max_loops,
|
||||
)
|
||||
|
||||
mu_guess_0, mu_guess_1 = find_bounds(function=F_optimize,
|
||||
x_init=self.chemical_potential,
|
||||
delta_x=delta, max_loops=max_loops,
|
||||
)
|
||||
mu_guess_1 += 0.01 #scrambles higher lying interval to avoid getting stuck
|
||||
mpi.report("\nSUMK calc_mu: Searching root with Brent method\n")
|
||||
self.chemical_potential = brenth(f=F_optimize,
|
||||
a=mu_guess_0,
|
||||
b=mu_guess_1,
|
||||
xtol=precision, maxiter=max_loops,
|
||||
)
|
||||
|
||||
case _:
|
||||
raise ValueError(
|
||||
f"SUMK calc_mu: The method selected: {method}, is not implemented\n",
|
||||
"""
|
||||
Please check for typos or select one of the following:
|
||||
* dichotomy: usual bisection algorithm from the TRIQS library
|
||||
* newton: newton method, fastest convergence but more unstable
|
||||
* brent: finds bounds and proceeds with hyperbolic brent method, a compromise between speed and ensuring convergence
|
||||
"""
|
||||
)
|
||||
else:
|
||||
raise ValueError(
|
||||
f"SUMK calc_mu: The selected method: {method}, is not implemented\n",
|
||||
"""
|
||||
Please check for typos or select one of the following:
|
||||
* dichotomy: usual bisection algorithm from the TRIQS library
|
||||
* newton: newton method, fastest convergence but more unstable
|
||||
* brent: finds bounds and proceeds with hyperbolic brent method, a compromise between speed and ensuring convergence
|
||||
"""
|
||||
)
|
||||
|
||||
return self.chemical_potential
|
||||
|
||||
@ -2414,7 +2373,8 @@ class SumkDFT(object):
|
||||
f.write("\n")
|
||||
|
||||
elif dm_type == 'qe':
|
||||
assert self.SP == 0, "Spin-polarized density matrix is not implemented"
|
||||
if self.SP == 0:
|
||||
mpi.report("SUMK calc_density_correction: WARNING! Averaging out spin-polarized correction in the density channel")
|
||||
|
||||
subgrp = 'dft_update'
|
||||
delta_N = np.zeros([self.n_k, max(self.n_orbitals[:,0]), max(self.n_orbitals[:,0])], dtype=complex)
|
||||
|
BIN
test/python/NiO.ref.h5
Executable file
BIN
test/python/NiO.ref.h5
Executable file
Binary file not shown.
BIN
test/python/NiO.ref.h5_copy
Executable file
BIN
test/python/NiO.ref.h5_copy
Executable file
Binary file not shown.
Binary file not shown.
BIN
test/python/SrVO3.ref.h5_copy
Normal file
BIN
test/python/SrVO3.ref.h5_copy
Normal file
Binary file not shown.
168
test/python/dc_test.py
Executable file
168
test/python/dc_test.py
Executable file
@ -0,0 +1,168 @@
|
||||
##########################################################################
|
||||
#
|
||||
# TRIQS: a Toolbox for Research in Interacting Quantum Systems
|
||||
#
|
||||
# Copyright (C) 2023 by A. Carta
|
||||
#
|
||||
# TRIQS is free software: you can redistribute it and/or modify it under the
|
||||
# terms of the GNU General Public License as published by the Free Software
|
||||
# Foundation, either version 3 of the License, or (at your option) any later
|
||||
# version.
|
||||
#
|
||||
# TRIQS is distributed in the hope that it will be useful, but WITHOUT ANY
|
||||
# WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
|
||||
# FOR A PARTICULAR PURPOSE. See the GNU General Public License for more
|
||||
# details.
|
||||
#
|
||||
# You should have received a copy of the GNU General Public License along with
|
||||
# TRIQS. If not, see <http://www.gnu.org/licenses/>.
|
||||
#
|
||||
##########################################################################
|
||||
|
||||
|
||||
|
||||
import numpy as np
|
||||
from triqs_dft_tools.sumk_dft import *
|
||||
from triqs.gf import *
|
||||
from h5 import HDFArchive
|
||||
from triqs.operators.util import *
|
||||
import triqs.utility.mpi as mpi
|
||||
|
||||
|
||||
Uval = 5
|
||||
Jval = 0.3
|
||||
|
||||
method_dict = {
|
||||
"FLL":{
|
||||
"numbering_convention":0,
|
||||
"new_convention":"cFLL"
|
||||
},
|
||||
"AMF":{
|
||||
"numbering_convention":2,
|
||||
"new_convention":"cAMF"
|
||||
},
|
||||
"Held":{
|
||||
"numbering_convention":1,
|
||||
"new_convention":"cHeld"
|
||||
},
|
||||
}
|
||||
|
||||
|
||||
|
||||
|
||||
def test_dc(method, method_dict, dens, Uval, Jval, filename):
|
||||
|
||||
dc_no = method_dict[method]["numbering_convention"]
|
||||
dc_string = method_dict[method]["new_convention"]
|
||||
|
||||
mpi.report("XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX")
|
||||
mpi.report(f"\n Testing interface {method} \n")
|
||||
mpi.report("XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX")
|
||||
|
||||
mpi.report("\nTesting legacy compatibility layer:\n")
|
||||
SK_compat.calc_dc(dens_mat=dens[0], U_interact=Uval, J_hund=Jval, use_dc_formula=dc_no )
|
||||
mpi.report("Up DC matrix:")
|
||||
mpi.report(SK_compat.dc_imp[0]['up'])
|
||||
mpi.report(f"Double counting energy = {SK_compat.dc_energ} ")
|
||||
|
||||
mpi.report("\nTesting new dc interface:\n")
|
||||
SK_new.calc_dc(dens_mat=dens[0], U_interact=Uval, J_hund=Jval, use_dc_formula=dc_string)
|
||||
mpi.report("Up DC matrix:")
|
||||
mpi.report(SK_new.dc_imp[0]['up'])
|
||||
mpi.report(f"Double counting energy = {SK_new.dc_energ} ")
|
||||
|
||||
# Load previously computed DC values from h5 archive
|
||||
R = HDFArchive(f'./{filename}', 'r')
|
||||
dc_comp = R[f'DC_{method}_benchmark']['dc_imp']
|
||||
en_comp = R[f'DC_{method}_benchmark']['dc_energ']
|
||||
del R
|
||||
|
||||
mpi.report(f"\nAsserting comparison for method: {method}")
|
||||
assert np.allclose(SK_compat.dc_imp[0]['up'], dc_comp, atol=1e-12), f"Assertion failed comparing legacy Vdc to reference, method: {method} "
|
||||
assert np.allclose(SK_compat.dc_energ, en_comp, atol=1e-12), f"Assertion failed comparing legacy energy to reference, method {method} "
|
||||
assert np.allclose(SK_new.dc_imp[0]['up'], dc_comp, atol=1e-12), f"Assertion failed comparing Vdc to reference, method: {method} "
|
||||
assert np.allclose(SK_new.dc_energ, en_comp, atol=1e-12), f"Assertion failed comparing energy to reference, method: {method} "
|
||||
mpi.report("Comparison with stored DC values successfull!\n")
|
||||
|
||||
|
||||
|
||||
|
||||
# %% 5 orbitals testing
|
||||
|
||||
mpi.report("\n############################################")
|
||||
mpi.report("############################################")
|
||||
mpi.report(f"\n \n Starting tests for 5 orbitals \n \n")
|
||||
mpi.report("############################################")
|
||||
mpi.report("############################################")
|
||||
dft_filename = "./NiO.ref"
|
||||
use_blocks = False
|
||||
SK_compat = SumkDFT(hdf_file=dft_filename+'.h5',use_dft_blocks=use_blocks)
|
||||
SK_compat.set_mu(13.9)
|
||||
SK_new = SumkDFT(hdf_file=dft_filename+'.h5',use_dft_blocks=use_blocks)
|
||||
SK_new.set_mu(13.9)
|
||||
|
||||
|
||||
icrsh = 0
|
||||
dens = SK_compat.density_matrix()
|
||||
|
||||
with np.printoptions(precision=5):
|
||||
for key in dens[0].keys():
|
||||
mpi.report(f"{key} channel")
|
||||
mpi.report(dens[0][key].real)
|
||||
|
||||
N_up = np.trace(dens[0]['up'].real)
|
||||
N_down = np.trace(dens[0]['down'].real)
|
||||
N_tot = N_up + N_down
|
||||
|
||||
mpi.report(f"{N_up=} ,{N_down=}, {N_tot=}\n")
|
||||
|
||||
for method in ["FLL", "AMF", "Held"]:
|
||||
test_dc(method, method_dict, dens, Uval, Jval, filename = f"{dft_filename}.h5")
|
||||
|
||||
#in case implementation changes, to write new testing data into archive
|
||||
#R = HDFArchive('./NiO.ref.h5', 'a')
|
||||
#R.create_group(f'DC_{method}_benchmark')
|
||||
#R[f'DC_{method}_benchmark']['dc_imp']= SK_new.dc_imp[0]['up']
|
||||
#R[f'DC_{method}_benchmark']['dc_energ']= SK_new.dc_energ
|
||||
#del R
|
||||
|
||||
|
||||
# 3 orbital testing
|
||||
|
||||
mpi.report("############################################")
|
||||
mpi.report("############################################")
|
||||
mpi.report(f"\n \n Starting tests for 3 orbitals \n \n")
|
||||
mpi.report("############################################")
|
||||
mpi.report("############################################")
|
||||
dft_filename = "./SrVO3.ref"
|
||||
use_blocks = False
|
||||
SK_compat = SumkDFT(hdf_file=dft_filename+'.h5',use_dft_blocks=use_blocks)
|
||||
SK_new = SumkDFT(hdf_file=dft_filename+'.h5',use_dft_blocks=use_blocks)
|
||||
|
||||
icrsh = 0
|
||||
dens = SK_compat.density_matrix()
|
||||
|
||||
|
||||
with np.printoptions(precision=5):
|
||||
for key in dens[0].keys():
|
||||
mpi.report(f"{key} channel")
|
||||
mpi.report(dens[0][key].real)
|
||||
|
||||
N_up = np.trace(dens[0]['up'].real)
|
||||
N_down = np.trace(dens[0]['down'].real)
|
||||
N_tot = N_up + N_down
|
||||
|
||||
mpi.report(f"{N_up=} ,{N_down=}, {N_tot=}\n")
|
||||
|
||||
Uval = 5
|
||||
Jval = 0.3
|
||||
|
||||
for method in ["FLL", "AMF", "Held"]:
|
||||
test_dc(method, method_dict, dens, Uval, Jval, filename = f"{dft_filename}.h5" )
|
||||
|
||||
#in case implementation changes, to write new testing data into archive
|
||||
#R = HDFArchive(f'./{dft_filename}.h5', 'a')
|
||||
#R.create_group(f'DC_{method}_benchmark')
|
||||
#R[f'DC_{method}_benchmark']['dc_imp']= SK_new.dc_imp[0]['up']
|
||||
#R[f'DC_{method}_benchmark']['dc_energ']= SK_new.dc_energ
|
||||
#del R
|
Loading…
Reference in New Issue
Block a user