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Gamma ray spectra dep #2793
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Gamma ray spectra dep #2793
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Original file line number | Diff line number | Diff line change |
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@@ -1,7 +1,6 @@ | ||
import numpy as np | ||
from numba import njit | ||
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from tardis.energy_input.gamma_ray_estimators import deposition_estimator_kasen | ||
from tardis.energy_input.gamma_ray_grid import ( | ||
distance_trace, | ||
move_packet, | ||
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@@ -38,17 +37,16 @@ | |
pair_creation_opacity_type, | ||
electron_number_density_time, | ||
mass_density_time, | ||
inv_volume_time, | ||
iron_group_fraction_per_shell, | ||
inner_velocities, | ||
outer_velocities, | ||
times, | ||
dt_array, | ||
times, | ||
effective_time_array, | ||
energy_bins, | ||
energy_df_rows, | ||
energy_plot_df_rows, | ||
energy_out, | ||
energy_deposited_gamma, | ||
energy_deposited_positron, | ||
packets_info_array, | ||
): | ||
"""Propagates packets through the simulation | ||
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@@ -103,21 +101,23 @@ | |
escaped_packets = 0 | ||
scattered_packets = 0 | ||
packet_count = len(packets) | ||
# Logging does not work with numba | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Remove the "print statement". |
||
print("Entering gamma ray loop for " + str(packet_count) + " packets") | ||
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deposition_estimator = np.zeros_like(energy_df_rows) | ||
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for i in range(packet_count): | ||
packet = packets[i] | ||
time_index = get_index(packet.time_current, times) | ||
energy_deposited_positron[ | ||
packet.shell, time_index | ||
] += packet.positron_energy | ||
|
||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Set positron energy to zero here now that it has been deposited? There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Alternatively, remove and calculate separately. There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. i.e. instead of in this loop, use the dataframe and sum all the positron energy per shell per time step and use those to fill out this array |
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if time_index < 0: | ||
print(packet.time_current, time_index) | ||
raise ValueError("Packet time index less than 0!") | ||
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scattered = False | ||
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initial_energy = packet.energy_cmf | ||
# Not used now. Useful for the deposition estimator. | ||
# initial_energy = packet.energy_cmf | ||
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while packet.status == GXPacketStatus.IN_PROCESS: | ||
# Get delta-time value for this step | ||
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@@ -214,17 +214,6 @@ | |
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packet = move_packet(packet, distance) | ||
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deposition_estimator[packet.shell, time_index] += ( | ||
(initial_energy * 1000) | ||
* distance | ||
* (packet.energy_cmf / initial_energy) | ||
* deposition_estimator_kasen( | ||
comoving_energy, | ||
mass_density_time[packet.shell, time_index], | ||
iron_group_fraction_per_shell[packet.shell], | ||
) | ||
) | ||
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if distance == distance_time: | ||
time_index += 1 | ||
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@@ -246,26 +235,9 @@ | |
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packet, ejecta_energy_gained = process_packet_path(packet) | ||
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# Save packets to dataframe rows | ||
# convert KeV to eV / s / cm^3 | ||
energy_df_rows[packet.shell, time_index] += ( | ||
ejecta_energy_gained * 1000 | ||
) | ||
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energy_plot_df_rows[i] = np.array( | ||
[ | ||
i, | ||
ejecta_energy_gained * 1000 | ||
# * inv_volume_time[packet.shell, time_index] | ||
/ dt, | ||
packet.get_location_r(), | ||
packet.time_current, | ||
packet.shell, | ||
compton_opacity, | ||
photoabsorption_opacity, | ||
pair_creation_opacity, | ||
] | ||
) | ||
energy_deposited_gamma[ | ||
packet.shell, time_index | ||
] += ejecta_energy_gained | ||
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if packet.status == GXPacketStatus.PHOTOABSORPTION: | ||
# Packet destroyed, go to the next packet | ||
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@@ -279,14 +251,18 @@ | |
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if packet.shell > len(mass_density_time[:, 0]) - 1: | ||
rest_energy = packet.nu_rf * H_CGS_KEV | ||
lum_rf = (packet.energy_rf * 1.6022e-9) / dt | ||
bin_index = get_index(rest_energy, energy_bins) | ||
bin_width = ( | ||
energy_bins[bin_index + 1] - energy_bins[bin_index] | ||
) | ||
energy_out[bin_index, time_index] += rest_energy / ( | ||
bin_width * dt | ||
freq_bin_width = bin_width / H_CGS_KEV | ||
energy_out[bin_index, time_index] += ( | ||
packet.energy_rf | ||
/ dt | ||
/ freq_bin_width # Take light crossing time into account | ||
) | ||
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luminosity = packet.energy_rf / dt | ||
packet.status = GXPacketStatus.ESCAPED | ||
escaped_packets += 1 | ||
if scattered: | ||
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@@ -303,7 +279,7 @@ | |
packet.nu_cmf, | ||
packet.nu_rf, | ||
packet.energy_cmf, | ||
lum_rf, | ||
luminosity, | ||
packet.energy_rf, | ||
packet.shell, | ||
] | ||
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@@ -313,12 +289,10 @@ | |
print("Scattered packets:", scattered_packets) | ||
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return ( | ||
energy_df_rows, | ||
energy_plot_df_rows, | ||
energy_out, | ||
deposition_estimator, | ||
bin_width, | ||
packets_info_array, | ||
energy_deposited_gamma, | ||
energy_deposited_positron, | ||
) | ||
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