.. _phlist_overview:
Overview of pyXSIM's Photon Lists
=================================
The Heritage of pyXSIM's Photon Lists
-------------------------------------
The photon list capability in pyXSIM is an independent implementation of the
`PHOX `_
algorithm, developed for constructing mock X-ray observations from SPH datasets
by Veronica Biffi and Klaus Dolag. There are two relevant papers:
`Biffi, V., Dolag, K., Bohringer, H., & Lemson, G. 2012, MNRAS, 420,
3545 `_
`Biffi, V., Dolag, K., Bohringer, H. 2013, MNRAS, 428,
1395 `_
pyXSIM had a previous life as the ``photon_simulator`` analysis module as a part
of the `yt Project `_. pyXSIM still depends critically on
yt to provide the link between the simulation data and the algorithm for
generating the X-ray photons. For detailed information about the design of the
algorithm in yt, check out
`the SciPy 2014 Proceedings. `_
.. _how-it-works:
How Photon Lists Work
---------------------
This section details in brief the model, assumptions, and basic algorithms of
pyXSIM's photon lists in terms of three basic steps.
Step 1: Generate Photons
++++++++++++++++++++++++
We begin with a three-dimensional model of a source, whether from a dataset from
some type of dynamical simulation or from a dataset constructed by hand. This
dataset is comprised of cells or particles, and is understandable by yt.
Examples of this may be:
* A model of a galaxy cluster plasma, where the emission arises from various
interactions between the thermal electrons and ions
* A model of relativistic particles which emit inverse-Compton emission in a
power-law spectrum
* A model of dark matter particles where line emission arises from annihilation
or decay of the particles
In any case, there is a fair amount of flexibility in the type of source and its
emission that can be modeled. The basic idea is that for each cell or particle
in a specified region of the source, photons are generated assuming the physical
properties of the call and an emission model for X-rays based on those physical
properties. The number of photons to be generated is controlled by specifying a
fiducial exposure time, collecting area, and redshift and/or distance to the
source. Typically, at this stage the values of these parameters are chosen such
that they generate a large number of photons, much larger than would be actually
observed, since the goal is to create an initial distribution that will be a
statistically robust sample from which to draw events when creating synthetic
observations. The photons are generated with three-dimensional positions in the
rest frame of the source (except that their energies are potentially
cosmologically redshifted with the given redshift, if the source is
cosmologically distant), since the positions on the sky and the Doppler shifting
of the photons are taken into account in the next step when a line of sight is
provided.
Figure 1 shows a schematic example of a three-dimensional source and how the
photons are generated from it. The details of how photons are created can be
found in :ref:`generating-photon-lists`.
.. figure:: ../_images/schematic.png
:align: center
:figclass: w
:scale: 40 %
Figure 1: Schematic representation of a roughly spherical X-ray emitting
object, such as a galaxy cluster. The volume element :math:`\Delta{V}_i`
at position :math:`{\bf r}_i` in the coordinate system :math:`{\cal O}`
of the source has a velocity :math:`{\bf v}_i`. Photons emitted along the
direction given by :math:`\hat{\bf n}` will be received in the observer's
frame in the coordinate system :math:`{\cal O}'`, and will be
Doppler-shifted by the line-of-sight velocity component :math:`v_{i,z'}`.
:math:`{\rm Chandra}` telescope image credit: NASA/CXC.
Step 2: Project Photons to Create Events
++++++++++++++++++++++++++++++++++++++++
Once we have generated our large sample of photons in the previous step, we
can create a set of simulated events by projecting them along a particular
line of sight. The line of sight is used to determine both the position of
each event on the sky as well as the Doppler shift of the photon from the
velocity of the material it was emitted from. Additionally, this is the step
where foreground Galactic absorption is optionally applied. The final product
is a set of events.
Figure 1 also shows how the photons are projected from the three-dimensional
source along the sight-line toward the observer. The details of how events
are created can be found in :ref:`event-lists`.
Step 3: Convolve Events with Instrumental Responses
+++++++++++++++++++++++++++++++++++++++++++++++++++
Finally, the last step is to take the sky-projected event positions and
energies and convolve them with instrumental responses to produce realistic
images and spectra that can be processed with standard software tools for
working with X-ray observations. pyXSIM provides a way to export the simulated
events for use with other packages which simulate X-ray observatories more
accurately. The details on how to do this can be found in :ref:`instruments`.