CONDENSED_DECAY_INFO_FILE=CONDENSED_DECAY_INFO_FILE,
FULL_DECAY_INFO_FILE=FULL_DECAY_INFO_FILE,
MAX_XS_FILE=MAX_XS_FILE)
PARAMS_DICT.update({sys.argv[0] + " argv": sys.argv[1:]})
save_parameters_as_json(sys.argv[-1], PARAMS_DICT)
tprint("Stage 1: Data reading from", *sys.argv[1:], "complete!")
else:
tprint(
f"Assuming that Stage 1 is complete. Reading {MICROSCOPIC_XS_CSV} as sigma_df and {CONDENSED_DECAY_INFO_FILE} as decay_dict..."
)
from misc_library import unserialize_dict
sigma_df = pd.read_csv(os.path.join(sys.argv[-1], MICROSCOPIC_XS_CSV),
index_col=[0])
with open(os.path.join(sys.argv[-1], CONDENSED_DECAY_INFO_FILE)) as j:
decay_dict = json.load(j)
decay_dict = unserialize_dict(decay_dict)
with open(os.path.join(sys.argv[-1], MAX_XS_FILE)) as j:
max_xs = MaxSigma(json.load(j))
##################################### Calculate count info of about each reactions #####################
IRRADIATION_DURATION = 3600 # spread the irradiation power over the entire course of this length
TRANSIT_DURATION = 86400 * 3
MEASUREMENT_DURATION = 3600 * 3
PRE_MEASUREMENT_POPULATION_FILE = "pre-measurement_population.json"
POST_MEASUREMENT_POPULATION_FILE = "post-measurement_population.json"
if __name__ == "__main__":
from misc_library import BARN, MM_CM, get_apriori, decay_mat_exp_num_decays, decay_mat_exp_population_convolved, build_decay_chain_tree, linearize_decay_chain, EncoderOpenMC
tprint("Stage 2: Calculating information about each reaction:")
PLOT_CONTR = False
PLOT_MACRO = False
PLOT_INDIVIDUAL_SPEC = False
# if False:
if __name__ == '__main__':
"""
with open(os.path.join(sys.argv[-1], "parameters_used.json")) as J:
PARAMS_DICT = json.load(J)
# get the user-defined foil selection, and their thicknesses
"""
# reading data
with open(os.path.join(sys.argv[-1], "final_selection.json")) as j:
selected_foils = json.load(j)
with open(os.path.join(sys.argv[-1], "decay_radiation.json")) as j:
decay_dict = unserialize_dict(json.load(j))
with open(os.path.join(sys.argv[-1], "decay_info.json")) as j:
decay_info = unserialize_dict(
json.load(j)
) # the decay counts given the stated starting and ending measurement times.
with open(os.path.join(sys.argv[-1],
"post-measurement_population.json")) as j:
post_measurement_population = json.load(j)
abs_efficieny_curve = HPGe_efficiency_curve_generator()
PARAMS_DICT = get_parameters_json(sys.argv[-1])
IRRADIATION_DURATION = PARAMS_DICT["IRRADIATION_DURATION"]
b, c = IRRADIATION_DURATION + PARAMS_DICT[
"TRANSIT_DURATION"], IRRADIATION_DURATION + PARAMS_DICT[
"TRANSIT_DURATION"] + PARAMS_DICT["MEASUREMENT_DURATION"]
APRIORI_FLUX, APRIORI_FLUENCE = get_apriori(sys.argv[-1],
IRRADIATION_DURATION)
def run_():
from .read_data import *
def tprint(*msg):
print("\n[t=+{:2.2f}s]".format(time.time() - prog_start_time), *msg)
prog_start_time = time.time()
stage1_outputs_exist = all(
os.path.exists(os.path.join(sys.argv[-1], FULL_DECAY_INFO_FILE)),
os.path.exists(os.path.join(sys.argv[-1], CONDENSED_DECAY_INFO_FILE)),
os.path.exists(os.path.join(sys.argv[-1], MICROSCOPIC_XS_CSV)),
os.path.exists(os.path.join(sys.argv[-1], MAX_XS_FILE)))
if not stage1_outputs_exist:
from misc_library import EncoderOpenMC, MT_to_nuc_num, load_endf_directories, FISSION_MTS, AMBIGUOUS_MT
prog_start_time = time.time()
assert os.path.exists(os.path.join(
sys.argv[-1],
'gs.csv')), "Output directory must already have gs.csv"
gs = pd.read_csv(os.path.join(sys.argv[-1], 'gs.csv')).values
if SORT_BY_REACTION_RATE:
_msg = f"Output directory must already have integrated_apriori.csv in order to sort the {MICROSCOPIC_XS_CSV} in descending order of expected-radionuclide-population later on."
assert os.path.exists(
os.path.join(sys.argv[-1], 'integrated_apriori.csv')), _msg
apriori = pd.read_csv(
os.path.join(sys.argv[-1],
'integrated_apriori.csv'))['value'].values
endf_file_list = load_endf_directories(sys.argv[1:-1])
print(f"Loaded {len(endf_file_list)} different material files,\n")
# First compile the decay records
tprint(
"Stage 1: Compiling the decay information as decay_dict, and recording the excited-state to isomeric-state information:"
)
decay_dict = OrderedDict() # dictionary of decay data
isomeric_to_excited_state = OrderedDict(
) # a dictionary that translates all
with warnings.catch_warnings(record=True) as w_list:
for file in tqdm(endf_file_list):
name = str(file.target["atomic_number"]).zfill(
3) + ATOMIC_SYMBOL[file.target["atomic_number"]] + str(
file.target["mass_number"])
isomeric_name = name # make a copy
if file.target[
"isomeric_state"] > 0: # if it is not at the lowest isomeric state: add the _e behind it too.
isomeric_name += "_m" + str(file.target["isomeric_state"])
name += "_e" + str(file.target["state"])
isomeric_to_excited_state[isomeric_name] = name[
3:] # trim the excited state name
if file.info[
'sublibrary'] == "Radioactive decay data": # applicable to materials with (mf, mt) = (8, 457) file section
dec_f = Decay.from_endf(file)
decay_dict[name] = extract_decay(dec_f)
if w_list:
print(w_list[0].filename + ", line {}, {}'s:".format(
w_list[0].lineno, w_list[0].category.__name__))
for w in w_list:
print(" " + str(w.message))
decay_dict = sort_and_trim_ordered_dict(
decay_dict) # reorder it so that it conforms to the
isomeric_to_excited_state = sort_and_trim_ordered_dict(
isomeric_to_excited_state)
tprint(
"Renaming the decay products from isomeric state names to excited state names:"
)
decay_dict = rename_branching_ratio(decay_dict,
isomeric_to_excited_state)
# Save said decay records
with open(os.path.join(sys.argv[-1], FULL_DECAY_INFO_FILE), 'w') as j:
tprint("Saving the decay spectra as {} ...".format(
FULL_DECAY_INFO_FILE))
json.dump(decay_dict, j, cls=EncoderOpenMC)
# turn decay records into number of counts
tprint("Condensing each decay spectrum...")
for name, dec_file in tqdm(decay_dict.items()):
condense_spectrum(dec_file)
with open(os.path.join(sys.argv[-1], CONDENSED_DECAY_INFO_FILE),
'w') as j:
tprint("Saving the condensed decay information as {} ...".format(
CONDENSED_DECAY_INFO_FILE))
json.dump(decay_dict, j, cls=EncoderOpenMC)
# Then compile the Incident-neutron records
tprint("Compiling the raw cross-section dictionary.")
xs_dict = OrderedDict()
for file in tqdm(endf_file_list):
# mf10 = {}
if file.info['sublibrary'] == "Incident-neutron data":
inc_f = IncidentNeutron.from_endf(file)
nuc_sort_name = str(inc_f.atomic_number).zfill(3) + inc_f.name
# get the higher-energy range values of xs as well if available.
mf10_mt5 = MF10(file.section.get(
(10, 5),
None)) # default value = None if (10, 5 doesn't exist.)
for (izap, isomeric_state), xs in mf10_mt5.items():
atomic_number, mass_number = divmod(izap, 1000)
if atomic_number > 0 and mass_number > 0: # ignore the weird products that means nothing meaningful
isomeric_name = ATOMIC_SYMBOL[atomic_number] + str(
mass_number)
if isomeric_state > 0:
isomeric_name += "_m" + str(isomeric_state)
e_name = isomeric_to_excited_state.get(
isomeric_name,
isomeric_name.split("_")[0]
) # return the ground state name if there is no corresponding excited state name for such isomer.
long_name = nuc_sort_name + "-" + e_name + "-MT=5"
xs_dict[long_name] = xs
# get the normal reactions, found in mf=3
for mt, rx in inc_f.reactions.items():
if any([(mt in AMBIGUOUS_MT), (mt in FISSION_MTS),
(301 <= mt <= 459)]):
continue # skip the cases of AMBIGUOUS_MT, fission mt, and heating information. They don't give us useful information about radionuclides produced.
append_name_list, xs_list = extract_xs(inc_f.atomic_number,
inc_f.mass_number,
rx,
tabulated=True)
# add each product into the dictionary one by one.
for name, xs in zip(append_name_list, xs_list):
xs_dict[nuc_sort_name + '-' + name] = xs
# memory management
print(
"Deleting endf_file_list since it will no longer be used in this script, in an attempt to reduce memory usage"
)
del endf_file_list
gc.collect()
# del decay_dict
xs_dict = sort_and_trim_ordered_dict(xs_dict)
tprint(
"Collapsing the cross-section to the group structure specified by 'gs.csv' and then saving it as '{}' ..."
.format(MICROSCOPIC_XS_CSV))
sigma_df, max_xs = collapse_xs(xs_dict, gs)
with open(os.path.join(sys.argv[-1], MAX_XS_FILE), "w") as j:
json.dump(max_xs, j)
del xs_dict
gc.collect()
if not SHOW_SEPARATE_MT_REACTION_RATES:
sigma_df = merge_identical_parent_products(sigma_df)
# Need to make merge_identical_parent_products to work with max_xs as well.
if SORT_BY_REACTION_RATE:
sigma_df = sigma_df.loc[ary(sigma_df.index)[np.argsort(
sigma_df.values @ apriori)[::-1]]]
print(
f"Saving the cross-sections in the required group structure to file as '{MICROSCOPIC_XS_CSV}'..."
)
sigma_df.to_csv(os.path.join(sys.argv[-1], MICROSCOPIC_XS_CSV))
# saves the number of radionuclide produced per (neutron cm^-2) of fluence flash-irradiated in that given bin.
# save parameters at the end.
PARAMS_DICT = dict(
HPGe_eff_file=HPGe_eff_file,
gamma_E=gamma_E,
FISSION_MTS=FISSION_MTS,
AMBIGUOUS_MT=AMBIGUOUS_MT,
SORT_BY_REACTION_RATE=SORT_BY_REACTION_RATE,
SHOW_SEPARATE_MT_REACTION_RATES=SHOW_SEPARATE_MT_REACTION_RATES,
CONDENSED_DECAY_INFO_FILE=CONDENSED_DECAY_INFO_FILE,
FULL_DECAY_INFO_FILE=FULL_DECAY_INFO_FILE,
MAX_XS_FILE=MAX_XS_FILE)
PARAMS_DICT.update({sys.argv[0] + " argv": sys.argv[1:]})
save_parameters_as_json(sys.argv[-1], PARAMS_DICT)
tprint("Stage 1: Data reading from", *sys.argv[1:], "complete!")
else:
tprint(
f"Assuming that Stage 1 is complete. Reading {MICROSCOPIC_XS_CSV} as sigma_df and {CONDENSED_DECAY_INFO_FILE} as decay_dict..."
)
from misc_library import unserialize_dict
sigma_df = pd.read_csv(os.path.join(sys.argv[-1], MICROSCOPIC_XS_CSV),
index_col=[0])
with open(os.path.join(sys.argv[-1], CONDENSED_DECAY_INFO_FILE)) as j:
decay_dict = json.load(j)
decay_dict = unserialize_dict(decay_dict)
with open(os.path.join(sys.argv[-1], MAX_XS_FILE)) as j:
max_xs = MaxSigma(json.load(j))
from misc_library import BARN, MM_CM, get_apriori, decay_mat_exp_num_decays, decay_mat_exp_population_convolved, build_decay_chain_tree, linearize_decay_chain, EncoderOpenMC
tprint("Stage 2: Calculating information about each reaction:")
apriori_flux, apriori_fluence = get_apriori(sys.argv[-1],
IRRADIATION_DURATION)
# get the production rate for each reaction, and build that into a dataframe (which will be expanded upon)
population = pd.DataFrame(
{
'production of primary product per reactant atom':
(sigma_df.values * BARN) @ apriori_fluence
},
index=sigma_df.index)
del sigma_df
gc.collect(
) # sigma_df is now used and will not be called again; remove it from memory to reduce memory usage/ stop stuffing up RAM.
# create containers to contain the calculated activities
# detected_counts_per_primary_product = {}
population_pre, population_post = defaultdict(dict), defaultdict(
dict) # key = the name of the subchain
total_counts, total_counts_post_meas, activity_pre, activity_post, cnt_rate_pre, cnt_rate_post = {}, {}, {}, {}, {}, {}
tprint(
"Calculating the expected number of photopeak counts for each type of product created:"
)
product_set = set([
parent_product_mt.split("-")[1]
for parent_product_mt in population.index
])
PRE_MEASUREMENT = IRRADIATION_DURATION + TRANSIT_DURATION
POST_MEASUREMENT = IRRADIATION_DURATION + TRANSIT_DURATION + MEASUREMENT_DURATION
for product in tqdm(product_set):
detected_counts_per_primary_product = []
for subchain in linearize_decay_chain(
build_decay_chain_tree(product, decay_dict)):
new_pathway = {
"pathway":
"-".join(subchain.names),
"counts during measurement":
decay_mat_exp_num_decays(
subchain.branching_ratios, subchain.decay_constants,
IRRADIATION_DURATION, PRE_MEASUREMENT, POST_MEASUREMENT) *
subchain.countable_photons,
"counts in 1 hr immediately after measurement":
decay_mat_exp_num_decays(
subchain.branching_ratios, subchain.decay_constants,
IRRADIATION_DURATION, POST_MEASUREMENT,
POST_MEASUREMENT + 3600) * subchain.countable_photons
}
population_pre[product][
new_pathway["pathway"]] = decay_mat_exp_population_convolved(
subchain.branching_ratios, subchain.decay_constants,
IRRADIATION_DURATION, PRE_MEASUREMENT)
population_post[product][
new_pathway["pathway"]] = decay_mat_exp_population_convolved(
subchain.branching_ratios, subchain.decay_constants,
IRRADIATION_DURATION, POST_MEASUREMENT)
new_pathway[
"decay rate pre-measurement"] = subchain.decay_constants[
-1] * population_pre[product][new_pathway["pathway"]]
new_pathway[
"decay rate post-measurement"] = subchain.decay_constants[
-1] * population_post[product][new_pathway["pathway"]]
new_pathway[
"count rate pre-measurement"] = subchain.countable_photons * new_pathway[
"decay rate pre-measurement"]
new_pathway[
"count rate post-measurement"] = subchain.countable_photons * new_pathway[
"decay rate post-measurement"]
detected_counts_per_primary_product.append(new_pathway)
total_counts[product] = sum([
path["counts during measurement"]
for path in detected_counts_per_primary_product
])
total_counts_post_meas[product] = sum([
path["counts in 1 hr immediately after measurement"]
for path in detected_counts_per_primary_product
])
activity_pre[product] = sum([
path["decay rate pre-measurement"]
for path in detected_counts_per_primary_product
])
activity_post[product] = sum([
path["decay rate post-measurement"]
for path in detected_counts_per_primary_product
])
cnt_rate_pre[product] = sum([
path["count rate pre-measurement"]
for path in detected_counts_per_primary_product
])
cnt_rate_post[product] = sum([
path["count rate post-measurement"]
for path in detected_counts_per_primary_product
])
# clean out reactions that can't be detected.
tprint(
"Removing all reactions whose products is the same as the product (i.e. elastic scattering reactions):"
)
population = population[ary([
parent_product_mt.split("-")[0] != parent_product_mt.split("-")[1]
for parent_product_mt in population.index
])]
# add the total counts of gamma photons detectable per primary product column
tprint("Matching the reactions to their decay product count...")
# add the final counts measured by detector PPP column
rearranged_total_cnts = ary([
total_counts[parent_product_mt.split("-")[1]]
for parent_product_mt in population.index
])
population['final counts measured by detector PPP'] = rearranged_total_cnts
# sort by activity and remove all nans
tprint(
"Re-ordering the dataframe by the final counts measured by detector PPP and removing the entries with zero counts..."
)
population.sort_values('final counts measured by detector PPP',
inplace=True,
ascending=False)
population = population[population["final counts measured by detector PPP"]
> 0.0] # keeping only those with positive counts.
# save the population breakdown in total_counts
tprint("Saving the population breakdowns as .json files...")
all_significant_products = ordered_set([
parent_product_mt.split("-")[1]
for parent_product_mt in population.index
])
with open(os.path.join(sys.argv[-1], PRE_MEASUREMENT_POPULATION_FILE),
"w") as j:
json.dump(
{
product: population_pre[product]
for product in all_significant_products
},
j,
cls=EncoderOpenMC)
# del population_pre; gc.collect()
with open(os.path.join(sys.argv[-1], POST_MEASUREMENT_POPULATION_FILE),
"w") as j:
json.dump(
{
product: population_post[product]
for product in all_significant_products
},
j,
cls=EncoderOpenMC)
# del population_post; gc.collect()
# add the rest of the information
rearranged_post_cnt_meas = ary([
total_counts_post_meas[parent_product_mt.split("-")[1]]
for parent_product_mt in population.index
])
rearranged_activity_pre = ary([
activity_pre[parent_product_mt.split("-")[1]]
for parent_product_mt in population.index
])
rearranged_activity_post = ary([
activity_post[parent_product_mt.split("-")[1]]
for parent_product_mt in population.index
])
rearranged_cnt_rate_pre = ary([
cnt_rate_pre[parent_product_mt.split("-")[1]]
for parent_product_mt in population.index
])
rearranged_cnt_rate_post = ary([
cnt_rate_post[parent_product_mt.split("-")[1]]
for parent_product_mt in population.index
])
rearranged_max_xs = ary(
[max_xs[parent_product_mt] for parent_product_mt in population.index])
population[
"counts accumulated in the 1 hour following the detection period PPP"] = rearranged_post_cnt_meas # column used to quickly extrapolate the post-measurement decay rate
population["activity before measurement PPP"] = rearranged_activity_pre
population["activity after measurement PPP"] = rearranged_activity_post
population[
"detector count rate before measurement PPP"] = rearranged_cnt_rate_pre
population[
"detector count rate after measurement PPP"] = rearranged_cnt_rate_post
population["max microscopic cross-section"] = rearranged_max_xs
tprint("Saving as 'counts.csv'...")
try:
population.to_csv(os.path.join(sys.argv[-1], 'counts.csv'),
index_label='rname')
except ZeroDivisionError:
tprint(
"Minor issue when trying to print the values which are too small. Plese wait for a couple more minutes..."
)
not_uncertain_columns = [
"production of primary product per reactant atom",
"max microscopic cross-section",
]
for col in population.columns:
if col not in not_uncertain_columns:
# when trying to express uncertainties.core.Variable using the __str__ method, it will try to factorize it.
# But if the GCD between the norminal value and uncertainty is rounded down to 1E-323 or smaller, it will lead to ZeroDivisionError.
floating_point_problem = population[
col] < 12.5E-324 # therefore we set all small values
# this method is harsher than it needs to because it forces items
# with nominal value < 12.5E-324 but error > 12.5E-324 to be 0 as well,
# even though they are perfectly expressible as strings without errors.
population[col][floating_point_problem] = 0
population.to_csv(os.path.join(sys.argv[-1], 'counts.csv'),
index_label='rname')
save_parameters_as_json(
sys.argv[-1],
dict(
IRRADIATION_DURATION=IRRADIATION_DURATION,
TRANSIT_DURATION=TRANSIT_DURATION,
MEASUREMENT_DURATION=MEASUREMENT_DURATION,
# PRE_MEASUREMENT_POPULATION_FILE=PRE_MEASUREMENT_POPULATION_FILE,
# POST_MEASUREMENT_POPULATION_FILE=POST_MEASUREMENT_POPULATION_FILE,
))
tprint("Run complete. See results in 'counts.csv'.")
def run():
def tprint(*msg):
print("\n[t=+{:2.2f}s]".format(time.time()-prog_start_time), *msg)
from .get_reaction_rates import *
# typical system/python stuff
import sys, os, time, json
from tqdm import tqdm
# numerical packages
from numpy import array as ary; import numpy as np
from numpy import log as ln; from numpy import sqrt
import pandas as pd
# openmc/specialist packages
import openmc
import uncertainties
from uncertainties.core import Variable
#collections
from collections import namedtuple, OrderedDict
# foilselector
from misc_library import save_parameters_as_json, unserialize_dict
from misc_library import BARN, MM_CM, get_apriori, decay_mat_exp_num_decays, Bateman_convolved_generator
# main script
prog_start_time = time.time()
apriori_flux, apriori_fluence = get_apriori(sys.argv[-1], IRRADIATION_DURATION)
with open(os.path.join(sys.argv[-1], CONDENSED_DECAY_INFO_FILE), 'r') as f:
decay_dict = json.load(f)
decay_dict = unserialize_dict(decay_dict)
sigma_df = pd.read_csv(os.path.join(sys.argv[-1], 'response.csv'), index_col=[0])
count_contribution_per_primary_product, total_counts_per_primary_product = {}, {}
tprint("Calculating the expected number of photopeak counts for each type of product created:")
product_set = set([parent_product_mt.split("-")[1] for parent_product_mt in sigma_df.index])
for product in tqdm(product_set):
count_contribution_per_primary_product[product] = [{
'pathway': '-'.join(subchain.names),
# (# of photons detected per nuclide n decayed) = (# of photons detected per decay of nuclide n) * lambda_n * \int(population)dT
# 'counts':Bateman_num_decays_factorized(subchain.branching_ratios, subchain.decay_constants,
'counts':np.product(subchain.branching_ratios[1:])*
decay_mat_exp_num_decays(subchain.decay_constants,
IRRADIATION_DURATION,
IRRADIATION_DURATION+TRANSIT_DURATION,
IRRADIATION_DURATION+TRANSIT_DURATION+MEASUREMENT_DURATION
)*subchain.countable_photons,
} for subchain in linearize_decay_chain(build_decay_chain(product, decay_dict))]
total_counts_per_primary_product[product] = sum([path["counts"] for path in count_contribution_per_primary_product[product]])
# get the production rate for each reaction
population = pd.DataFrame({'production of primary product per reactant atom':(sigma_df.values*BARN) @ apriori_fluence}, index=sigma_df.index)
# clean out reactions that can't be detected.
tprint("Removing all reactions whose products is the same as the product (i.e. elastic scattering reactions):")
population = population[ary([parent_product_mt.split("-")[0] != parent_product_mt.split("-")[1] for parent_product_mt in population.index])]
# add the total counts of gamma photons detectable per primary product column
tprint("Matching the reactions to their decay product count...")
gamma_counts_at_measurement_per_reactant = ary([total_counts_per_primary_product[parent_product_mt.split("-")[1]] for parent_product_mt in sigma_df.index])
# add the final counts accumulated per reactant atom column
population['final counts accumulated per reactant atom'] = gamma_counts_at_measurement_per_reactant * population['production of primary product per reactant atom']
# sort by activity and remove all nans
tprint("Re-ordering the dataframe by the final counts accumulated per reactant atom and removing the entries with zero counts...")
population.sort_values('final counts accumulated per reactant atom', inplace=True, ascending=False)
population = population[gamma_counts_at_measurement_per_reactant>0.0] # keeping only those with positive counts.
if GUESS_MATERIAL:
from misc_library import extract_elem_from_string, pick_material, PHYSICAL_PROP_FILE, get_physical_property
# read the physical property file to get the number densities.
tprint(f"Reading ./{os.path.relpath(PHYSICAL_PROP_FILE)} to extract the physical parameters about various solids.")
physical_prop = get_physical_property(PHYSICAL_PROP_FILE)
# select the default materials and get its relevant parameters
default_material, partial_number_density = [], []
tprint("Selecting the default material to be used:")
for parent_product_mt in tqdm(population.index):
parent = parent_product_mt.split('-')[0]
if parent[len(extract_elem_from_string(parent)):]=='0': # take care of the species which are a MIXED natural composition of materials, e.g. Gd0
parent = parent[:-1]
if ENRICH_TO_100_PERCENT: # allowing enrichment means 100% of that element being made of the specified isotope only
parent = extract_elem_from_string(parent)
if parent not in physical_prop.columns:
# if there isn't a parent material
default_material.append('Missing (N/A)')
partial_number_density.append(0.0)
continue
material_info = pick_material(parent, physical_prop)
default_material.append(material_info.name+" ("+material_info['Formula']+")")
partial_number_density.append(material_info['Number density-cm-3'] * material_info[parent]) # material_info[parent] chooses the fraction of atoms which is made of .
population["default material"] = default_material
population["partial number density (cm^-3)"] = partial_number_density
population["gamma counts per volume of foil (cm^-3)"] = population["final counts accumulated per reactant atom"] * population["partial number density (cm^-3)"]
population["gamma counts per unit thickness of foil (mm^-1)"] = population["gamma counts per volume of foil (cm^-3)"] * MAX_AREA * MM_CM# assuming the area = Foil Area
tprint("Re-ordering the dataframe according to the counts per volume...")
population.sort_values("gamma counts per volume of foil (cm^-3)", inplace=True, ascending=False) # sort again, this time according to the required volume
tprint("Saving as 'counts.csv'...")
try:
population.to_csv(os.path.join(sys.argv[-1], 'counts.csv'), index_label='rname')
except ZeroDivisionError:
tprint("Minor issue when trying to print the values which are too small. Plese wait for a couple more minutes...")
uncertain_columns = ["final counts accumulated per reactant atom"]
if GUESS_MATERIAL:
uncertain_columns+= ["gamma counts per volume of foil (cm^-3)", "gamma counts per unit thickness of foil (mm^-1)"]
for col in uncertain_columns:
less_than_mask = population[col]<12.5E-324 # when trying to express uncertainties.core.Variable using the __str__ method, it will try to factorize it.
# But if the GCD (between the norminal value and its counterpart) is rounded down to 1E-323 or smaller, it will lead to ZeroDivisionError.
population[col][less_than_mask] = uncertainties.core.Variable(0.0, 0.0)
population.to_csv(os.path.join(sys.argv[-1], 'counts.csv'), index_label='rname')
# save parameters at the end.
save_parameters_as_json(sys.argv[-1], dict(
IRRADIATION_DURATION=IRRADIATION_DURATION,
TRANSIT_DURATION=TRANSIT_DURATION,
MEASUREMENT_DURATION=MEASUREMENT_DURATION,
MAX_AREA=MAX_AREA,
ENRICH_TO_100_PERCENT=ENRICH_TO_100_PERCENT,
)
)
tprint("Run complete. See results in 'counts.csv'.")