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SWIFT
SWIFTsim
Commits
ae708c04
Commit
ae708c04
authored
Mar 08, 2020
by
Matthieu Schaller
Browse files
Added the documentation of the quick lyman alpha model
parent
7e0a509f
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5
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doc/RTD/source/SubgridModels/Basic/index.rst
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ae708c04
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@@ 2,8 +2,8 @@
Matthieu Schaller, 20th December 2018
Basic model
===========
Basic model
(others)
===========
=========
Cooling: Analytic models
...
...
doc/RTD/source/SubgridModels/EAGLE/index.rst
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ae708c04
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...
@@ 11,8 +11,8 @@ the parameters and values output in the snapshots.
..
_EAGLE_entropy_floors
:
E
ntropy
floors
~~~~~~~~~~~~~~
Gas
e
ntropy
floors
~~~~~~~~~~~~~~
~~~~
The
gas
particles
in
the
EAGLE
model
are
prevented
from
cooling
below
a
certain
temperature
.
The
temperature
limit
depends
on
the
density
of
the
...
...
@@ 327,13 +327,10 @@ along the redshift dimension then becomes a trivial operation.
The
cooling
itself
is
performed
using
an
implicit
scheme
(
see
the
theory
documents
)
which
for
small
values
of
the
cooling
rates
is
solved
explicitly
.
For
larger
values
we
use
a
bisection
scheme
.
Users
can
alternatively
use
a
Newton

Raphson
method
that
in
some
cases
runs
faster
than
the
bisection
method
.
If
the
Newton

Raphson
method
does
not
converge
after
a
few
steps
,
the
code
reverts
to
a
bisection
scheme
,
that
is
guaranteed
to
converge
.
The
cooling
rate
is
added
to
the
calculated
change
in
energy
over
time
from
the
other
dynamical
equations
.
This
is
different
from
other
commonly
used
codes
in
the
literature
where
the
cooling
is
done
instantaneously
.
larger
values
we
use
a
bisection
scheme
.
The
cooling
rate
is
added
to
the
calculated
change
in
energy
over
time
from
the
other
dynamical
equations
.
This
is
different
from
other
commonly
used
codes
in
the
literature
where
the
cooling
is
done
instantaneously
.
We
note
that
the
EAGLE
cooling
model
does
not
impose
any
restriction
on
the
particles
' individual timesteps. The cooling takes place over the time span
...
...
@@ 362,9 +359,8 @@ the case with cooling switched on.
The cooling model is driven by a small number of parameter files in the
`EAGLECooling` section of the YAML file. These are the reionization parameters,
the path to the tables and optionally the modified abundances of `Ca` and `S` as
well as the flag to attempt using the NewtonRaphson scheme to solve the
implicit problem. A valid section of the YAML file looks like:
the path to the tables and optionally the modified abundances of `Ca`
and `S`. A valid section of the YAML file looks like:
.. code:: YAML
...
...
@@ 383,7 +379,6 @@ And the optional parameters are:
EAGLECooling:
Ca_over_Si_in_solar: 1.0 # (Optional) Value of the Calcium mass abundance ratio to solar in units of the Silicon ratio to solar. Default value: 1.
S_over_Si_in_solar: 1.0 # (Optional) Value of the Sulphur mass abundance ratio to solar in units of the Silicon ratio to solar. Default value: 1.
newton_integration: 0 # (Optional) Set to 1 to use the NewtonRaphson scheme for the explicit cooling problem.
.. _EAGLE_tracers:
...
...
doc/RTD/source/SubgridModels/QuickLymanAlpha/index.rst
0 → 100644
View file @
ae708c04
.. Quick Lymanalpha subgrid model
Matthieu Schaller, 7th March 2020
Quick Lymanalpha (QLA) model
=============================
This section of the documentation gives a brief description of the different
components of the quick Lymanalpha subgrid model. We mostly focus on the
parameters and values output in the snapshots.
Given the nature of the model, no feedback or black holes are used. The star
formation model is minimalistic and the chemistry/cooling models are limited to
primordial abundances.
.. _QLA_entropy_floors:
Gas entropy floor
~~~~~~~~~~~~~~~~~
The gas particles in the QLA model are prevented from cooling below a certain
temperature. The temperature limit depends on the density of the particles. The
floor is implemented as a polytropic "equation of state":math:`P = P_c
\left(\rho/\rho_c\right)^\gamma` (all done in physical coordinates), with the
constants derived from the user input given in terms of temperature and Hydrogen
number density. We use :math:`gamma=1` in this model. The code computing the
entropy floor is located in the directory ``src/entropy_floor/QLA/`` and the
floor is applied in the drift and kick operations of the hydro scheme.
An additional overdensity criterion above the mean baryonic density is applied
to prevent gas not collapsed into structures from being affected. To be precise,
this criterion demands that the floor is applied only if :math:`\rho_{\rm com} >
\Delta_{\rm floor}\bar{\rho_b} = \Delta_{\rm floor} \Omega_b \rho_{\rm crit,0}`,
with :math:`\Delta_{\rm floor}` specified by the user, :math:`\rho_{\rm crit,0}
= 3H_0/8\pi G` the critical density at redshift zero [#f1]_, and
:math:`\rho_{\rm com}` the gas comoving density. Typical values for
:math:`\Delta_{\rm floor}` are of order 10.
The model is governed by 3 parameters for each of the two limits. These are
given in the ``QLAEntropyFloor`` section of the YAML file. The parameters are
the Hydrogen number density (in :math:`cm^{3}`) and temperature (in :math:`K`)
of the anchor point of the floor as well as the minimal overdensity required to
apply the limit. To simplify things, all constants are converted to the internal
system of units upon reading the parameter file.
For a normal quick Lymanalpha run, that section of the parameter file reads:
.. code:: YAML
QLAEntropyFloor:
density_threshold_H_p_cm3: 0.1 # Physical density above which the entropy floor kicks in expressed in Hydrogen atoms per cm^3.
over_density_threshold: 10. # Overdensity above which the entropy floor can kick in.
temperature_norm_K: 8000 # Temperature of the entropy floor at the density threshold expressed in Kelvin.
SWIFT will convert the temperature normalisations and Hydrogen number density
thresholds into internal energies and densities respectively assuming a neutral
gas with primoridal abundance pattern. This implies that the floor may not be
exactly at the position given in the YAML file if the gas has different
properties. This is especially the case for the temperature limit which will
often be lower than the imposed floor by a factor :math:`\frac{\mu_{\rm
neutral}}{\mu_{ionised}} \approx \frac{1.22}{0.59} \approx 2` due to the
different ionisation states of the gas.
Recall that we additionally impose an absolute minium temperature at all
densities with a value provided in the :ref:`Parameters_SPH` section of the
parameter file. This minimal temperature is typically set to 100 Kelvin.
.. _QLA_cooling:
Gas cooling: Wiersma+2009a with fixed primoridal metallicity
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
The gas cooling is based on the redshiftdependent tables of `Wiersma et
al. (2009)a <http://adsabs.harvard.edu/abs/2009MNRAS.393...99W>`_ that include
elementbyelement cooling rates for the 11 elements (`H`, `He`, `C`, `N`, `O`,
`Ne`, `Mg`, `Si`, `S`, `Ca` and `Fe`) that dominate the total rates. The tables
assume that the gas is in ionization equilibrium with the cosmic microwave
background (CMB) as well as with the evolving Xray and UV background from
galaxies and quasars described by the model of `Haardt & Madau (2001)
<http://adsabs.harvard.edu/abs/2001cghr.confE..64H>`_. Note that this model
ignores *local* sources of ionization, selfshielding and nonequilibrium
cooling/heating. The tables can be obtained from this `link
<http://virgodb.cosma.dur.ac.uk/swiftwebstorage/CoolingTables/EAGLE/coolingtables.tar.gz>`_
which is a repackaged version of the `original tables
<http://www.strw.leidenuniv.nl/WSS08/>`_. The code reading and interpolating the
table is located in the directory ``src/cooling/QLA/``.
The Wiersma tables containing the cooling rates as a function of redshift,
Hydrogen number density, Helium fraction (:math:`X_{He} / (X_{He} + X_{H})`) and
element abundance relative to the solar abundance pattern assumed by the tables
(see equation 4 in the original paper). Since the quick Lymanalpha model is
only of interest for gas outside of haloes, we can make use of primoridal gas
only. This means that the particles do not need to carry a metallicity array or
any individual element arrays. Another optimization is to ignore the cooling
rates of the metals in the tables.
Above the redshift of Hydrogen reionization we use the extra table containing
net cooling rates for gas exposed to the CMB and a UV + Xray background at
redshift nine truncated above 1 Rydberg. At the redshift or reionization, we
additionally inject a fixed userdefined amount of energy per unit mass to all
the gas particles.
In addition to the tables we inject extra energy from Helium II reionization
using a Gaussian model with a userdefined redshift for the centre, width and
total amount of energy injected per unit mass. Additional energy is also
injected instantaneously for Hydrogen reionisation to all particles (active and
inactive) to make sure the whole Universe reaches the expected temperature
quickly (i.e not just via the interaction with the now much stronger UV
background).
The cooling itself is performed using an implicit scheme (see the theory
documents) which for small values of the cooling rates is solved explicitly. For
larger values we use a bisection scheme. The cooling rate is added to the
calculated change in energy over time from the other dynamical equations. This
is different from other commonly used codes in the literature where the cooling
is done instantaneously.
We note that the QLA cooling model does not impose any restriction on the
particles' individual timesteps. The cooling takes place over the time span
given by the other conditions (e.g the Courant condition).
Finelly, the cooling module also provides a function to compute the temperature
of a given gas particle based on its density, internal energy, abundances and
the current redshift. This temperature is the one used to compute the cooling
rate from the tables and similarly to the cooling rates, they assume that the
gas is in collisional equilibrium with the background radiation. The
temperatures are, in particular, computed every time a snapshot is written and
they are listed for every gas particle:
+++++
 Name  Description  Units  Comments 
+=====================+=====================================+===========+=====================================+
 ``Temperatures``   Temperature of the gas as  [U_T]   The calculation is performed 
   computed from the tables.    using quantities at the last 
     timestep the particle was active 
+++++
Note that if one is running without cooling switched on at runtime, the
temperatures can be computed by passing the ``temperature`` runtime flag (see
:ref:`cmdlineoptions`). Note that the tables then have to be available as in
the case with cooling switched on.
The cooling model is driven by a small number of parameter files in the
`QLACooling` section of the YAML file. These are the reionization parameters
and the path to the tables. A valid section of the YAML file looks like:
.. code:: YAML
QLACooling:
dir_name: /path/to/the/Wiersma/tables/directory # Absolute or relative path
H_reion_z: 11.5 # Redhift of Hydrogen reionization
H_reion_ev_p_H: 2.0 # Energy injected in eV per Hydrogen atom for Hydrogen reionization.
He_reion_z_centre: 3.5 # Centre of the Gaussian used for Helium reionization
He_reion_z_sigma: 0.5 # Width of the Gaussian used for Helium reionization
He_reion_ev_p_H: 2.0 # Energy injected in eV per Hydrogen atom for Helium II reionization.
.. _QLA_star_formation:
Star formation
~~~~~~~~~~~~~~
The star formation in the Quick Lymanalpha model is very simple. Any gas
particle with a density larger than a multiple of the critical density for
closure is directly turned into a star. The idea is to rapidly eliminate any gas
that is found within bound structures since we are only interested in what
happens in the intergalactic medium. The overdensity multiple is the only
parameter of this model.
The code applying this star formation law is located in the directory
``src/star_formation/QLA/``.
For a normal Quick Lymanalpha run, that section of the parameter file reads:
.. code:: YAML
# Quick Lymanalpha star formation parameters
QLAStarFormation:
over_density: 1000 # The overdensity above which gas particles turn into stars.
.. [#f1] Recall that in a noncosmological run the critical density is
set to 0, effectively removing the overdensity
constraint of the floors.
doc/RTD/source/SubgridModels/index.rst
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ae708c04
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...
@@ 13,6 +13,7 @@ be use as an empty canvas to be copied to create additional models.
:maxdepth: 2
:caption: Available models:
Basic/index
EAGLE/index
QuickLymanAlpha/index
GEAR/index
Basic/index
doc/RTD/source/conf.py
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ae708c04
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@@ 19,7 +19,7 @@
#  Project information 
project
=
'SWIFT: SPH With Interdependent Finegrained Tasking'
copyright
=
'201
9
, SWIFT Collaboration'
copyright
=
'201
42020
, SWIFT Collaboration'
author
=
'SWIFT Team'
# The short X.Y version
...
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