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Added photoionization cross-sectional areas.
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byrdie committed Jul 8, 2024
1 parent 62a4527 commit ed023c1
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9 changes: 9 additions & 0 deletions fano/__init__.py
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"""
Theoretical model of the Fano noise and pair-production energy for silicon.
"""

from . import photons

__all__ = [
"photons",
]
9 changes: 9 additions & 0 deletions fano/photons/__init__.py
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"""
Models of the interaction of photons with silicon.
"""

from . import areas

__all__ = [
"areas",
]
64 changes: 64 additions & 0 deletions fano/photons/areas/__init__.py
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"""
Cross-sectional areas of silicon subshells for photon interactions.
Examples
--------
Plot the cross-section areas of each silicon subshell as a function of
photon energy.
.. jupyter-execute::
import numpy as np
import matplotlib.pyplot as plt
import astropy.units as u
import astropy.visualization
import fano
# Define of grid of photon energies to sample
energy = np.geomspace(1, 10000, num=1001) * u.eV
# Evaluate the area of each subshell for the given
# photon energy.
area_k1 = fano.photons.areas.area_photoionization_k1(energy)
area_l1 = fano.photons.areas.area_photoionization_l1(energy)
area_l2 = fano.photons.areas.area_photoionization_l2(energy)
area_l3 = fano.photons.areas.area_photoionization_l3(energy)
area_m1 = fano.photons.areas.area_photoionization_m1(energy)
area_m2 = fano.photons.areas.area_photoionization_m2(energy)
area_m3 = fano.photons.areas.area_photoionization_m3(energy)
# Plot the areas as a function of photon energy.
with astropy.visualization.quantity_support():
fig, ax = plt.subplots()
ax.loglog(energy, area_k1, label="$K_1$")
ax.loglog(energy, area_l1, label="$L_1$")
ax.loglog(energy, area_l2, label="$L_2$")
ax.loglog(energy, area_l3, label="$L_3$")
ax.loglog(energy, area_m1, label="$M_1$")
ax.loglog(energy, area_m2, label="$M_2$")
ax.loglog(energy, area_m3, label="$M_3$")
ax.set_xlabel(f"photon energy ({ax.get_xlabel()})")
ax.set_ylabel(f"cross-sectional aread ({ax.get_ylabel()})")
ax.legend()
"""

from ._ionization import (
area_photoionization_k1,
area_photoionization_l1,
area_photoionization_l2,
area_photoionization_l3,
area_photoionization_m1,
area_photoionization_m2,
area_photoionization_m3,
)

__all__ = [
"area_photoionization_k1",
"area_photoionization_l1",
"area_photoionization_l2",
"area_photoionization_l3",
"area_photoionization_m1",
"area_photoionization_m2",
"area_photoionization_m3",
]
208 changes: 208 additions & 0 deletions fano/photons/areas/_ionization.py
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import pathlib
import numpy as np
import numba
import astropy.units as u
import endf

__all__ = [
"area_photoionization_k1",
"area_photoionization_l1",
"area_photoionization_l2",
"area_photoionization_l3",
"area_photoionization_m1",
"area_photoionization_m2",
"area_photoionization_m3",
]

_path_epdl = pathlib.Path(__file__).parent / "epdl-silicon.endf"

_mf = 23

_mt_k1 = 534
_mt_l1 = 535
_mt_l2 = 536
_mt_l3 = 537
_mt_m1 = 538
_mt_m2 = 539
_mt_m3 = 540

_mat = endf.Material(_path_epdl)

_xs_k1 = _mat.section_data[_mf, _mt_k1]["sigma"]
_xs_l1 = _mat.section_data[_mf, _mt_l1]["sigma"]
_xs_l2 = _mat.section_data[_mf, _mt_l2]["sigma"]
_xs_l3 = _mat.section_data[_mf, _mt_l3]["sigma"]
_xs_m1 = _mat.section_data[_mf, _mt_m1]["sigma"]
_xs_m2 = _mat.section_data[_mf, _mt_m2]["sigma"]
_xs_m3 = _mat.section_data[_mf, _mt_m3]["sigma"]

_energy_k1 = _xs_k1.x
_energy_l1 = _xs_l1.x
_energy_l2 = _xs_l2.x
_energy_l3 = _xs_l3.x
_energy_m1 = _xs_m1.x
_energy_m2 = _xs_m2.x
_energy_m3 = _xs_m3.x

_area_k1 = _xs_k1.y
_area_l1 = _xs_l1.y
_area_l2 = _xs_l2.y
_area_l3 = _xs_l3.y
_area_m1 = _xs_m1.y
_area_m2 = _xs_m2.y
_area_m3 = _xs_m3.y

_unit_energy = u.eV
_unit_area = u.barn

_energy = [
[_energy_k1],
[_energy_l1, _energy_l2, _energy_l3],
[_energy_m1, _energy_m2, _energy_m3],
]

_area = [
[_area_k1],
[_area_l1, _area_l2, _area_l3],
[_area_m1, _area_m2, _area_m3],
]


def area_photoionization_k1(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`K_1` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_k1(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_k1(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_k1, _area_k1)


def area_photoionization_l1(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`L_1` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_l1(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_l1(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_l1, _area_l1)


def area_photoionization_l2(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`L_2` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_l2(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_l2(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_l2, _area_l2)


def area_photoionization_l3(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`L_3` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_l3(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_l3(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_l3, _area_l3)


def area_photoionization_m1(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`M_1` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_m1(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_m1(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_m1, _area_m1)


def area_photoionization_m2(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`M_2` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_m2(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_m2(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_m2, _area_m2)


def area_photoionization_m3(energy: u.Quantity) -> u.Quantity:
"""
Calculate the cross-section area of the :math:`M_3` shell for a photon of a
given energy.
Parameters
----------
energy
The energy of the incident photon
"""
energy = energy.to_value(_unit_energy, equivalencies=u.spectral())
result = _area_photoionization_m3(energy) << _unit_area
return result


@numba.njit
def _area_photoionization_m3(energy: np.ndarray) -> np.ndarray:
return np.interp(energy, _energy_m3, _area_m3)
30 changes: 30 additions & 0 deletions fano/photons/areas/_ionization_test.py
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from typing import Callable
import pytest
import numpy as np
import astropy.units as u
import fano

_energy = [
2000 * u.eV,
np.linspace(5, 2000, num=11) * u.eV,
np.linspace(1, 1000, num=12) * u.nm,
]


@pytest.mark.parametrize(
argnames="func",
argvalues=[
fano.photons.areas.area_photoionization_k1,
fano.photons.areas.area_photoionization_l1,
fano.photons.areas.area_photoionization_l2,
fano.photons.areas.area_photoionization_l3,
fano.photons.areas.area_photoionization_m1,
fano.photons.areas.area_photoionization_m2,
fano.photons.areas.area_photoionization_m3,
]
)
@pytest.mark.parametrize("energy", _energy)
def test_area_photoionization(func: Callable, energy: u.Quantity):
result = func(energy)
assert np.all(result >= 0)
assert result.unit.is_equivalent(u.barn)
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