Fast Lyman alpha Radiative Transfer for everyone!
Project description
LyaRT;Grid
In this Universe everything is neat, even stochasticity.
Lyman alpha Resonant Scatter is dominated by random processes.
Although there is chaos, there is also an order.
WARNING : THIS IS BETA VERSION! BUGS EVERYWHERE, BE AWARE!
Origins and motivation
Due to the Lyman alpha Radiative Transfer large complexity, the efforts of understanding it moved from pure analytic studies to the socalled radiative transfer Monte Carlo (RTMC) codes that simulate Lyman alpha photons in arbitrary gas geometries. These codes provide useful information about the fraction of photons that manage to escape and the resulting Lyman alpha line profiles. The RTMC approach has shown to reproduce the observed properties of LAEs.
LyaRT;Grid
is a publicly available python
package based on a RTMC (Orsi et al. 2012) able to predict large amounts of Lyman alpha line profiles and escape fractions with high accuracy. We designed this code hoping that it helps researches all over the wolrd to get a better understanding of the Universe.
LyaRT;Grid
is fast and simple.

Fast : This code is able to predict Lyman alpha escape fractions and line profiles in an unprecedentedly low amount of time. In particular thousands of escape fractions and line profiles can be computed in less than a second of computational time.

Simple : This code is OneLineRunning. Everyone, from a good trained monkey, passing through undergrade studients, to researches with basic python knowlege should be able to use
LyaRT;Grid
.
Although LyaRT;Grid
is completely open source and is available for everyone, please, if you are using this code ( for whatever reason ) we will be very glad to hear about you and how you are using it. it's just a curiosity and efficiency matter. Maybe we can help you to have a smoother experience with LyaRT;Grid
. For any issue or suggestion, please, contact sidgurung@cefca.es
. Thank you.
Installation
The easiest way to get LyaRT;Grid
in your machine is through pip
:
pip install LyaRT_Grid
This should do the trick. However, you can also install LyaRT_Grid
downloading this repository and running
pip install .
in it.
In order to finish installation and check that everything is working properly, please, opening a python
/ipython
terminal and execute:
import LyaRT_Grid as Lya Lya.Test_Installation( Make_Plots = True )
This function checks if the pip installation downloaded everything. Then, if the data files are not found it tries to download them. Please, note that you should have about 1GB of free memory in you machine in order to install LyaRT_Grid
. Also note that as ~1GB of data has to be downloaded, it might take some time depending on your internet conection.
After Checking that you have got the data in your machine LyaRT_Grid
will check that everyhting works smoothly. For this some escape fractions and line profiles will be computed. The status of the operation should appear in the screen. Everything should get a Succsess!!
. The only exception is
Running : Bicone_X_Slab Analytic > ERROR. HUMAN IS DEAD. MISMATCH!!
Do not worry. The only reason why you are getting this error is because this algorithm is not implemented yet. Then the function will produce some plots. In case you want to run the tests without plotting just set Make_Plots = False
when calling the Lya.Test_Installation
.
This should be all for the installation. If you find any trouble/bug duruing it, please, contact us at sidgurung@cefca.es
. Thank you for your patience.
Hands on the code.
( Assuming everything went smoothly in the installation... )
Congratulations!! You have just become one of the few chosen ones in the history of humankind to have the great pleasure of using LyaRT_Grid
.
The units: This code uses velocites in km/s , column densities in cm^{2} and wavelengths in meters.
First let's have a look to the dynamical range of the different parameters covered by LyaRT;Grid
. For this we only need to do:
import LyaRT_Grid as Lya Lya.Print_the_grid_edges()
Predicting thousands of Lyman alpha escape fractions.
Let's move to one of the most powerful products of LyaRT;Grid
: predicting huge amounts of Lyman alpha escape fractions.
In theory only one line is needed to predict the escape fraction for a thin shell geometry with expasion velocity (V) of 200km/s, logarithmic of column density (logNH) of 19.5 and dust optical depth (ta) of 0.1 :
f_esc_Arr = Lya.RT_f_esc( 'Thin_Shell' , [ 200 ] , [ 19.5 ] , [ 0.1 ] )
In this way f_esc_Arr
is an Array of 1 dimension and length 1 that contains the predicted escape fraction for this configuration.
However, LyaRT;Grid
implements several gas geometries and is optimized to obtain large amount of escape fractions with only one line of code, so lets expand this a little bit more. If we want to compute the escape fraction in a thin shell outflow with the configurations { V , logNH , ta } , { 200 , 19.5 , 0.1 }, { 300 , 20.0 , 0.01 } and { 400 , 20.5 , 0.001 } we could do
Geometry = 'Thin Shell' # Other options: 'Galactic Wind' or 'Bicone_X_Slab' V_Arr = [ 200 , 300 , 400 ] # Expansion velocity array in km/s logNH_Arr = [ 19.5 , 20.0 , 20.5 ] # Logarithmic of column densities array in cm**2 ta_Arr = [ 0.1 , 0.01 , 0.001 ] # Dust optical depth Array f_esc_Arr = Lya.RT_f_esc( Geometry , V_Arr , logNH_Arr , ta_Arr )
The variable f_esc_Arr
is an Array of 1 dimension and length 3 that encloses the escape fractions for the configurations. In particular f_esc_Arr[i]
is computed using V_Arr[i]
, logNH_Arr[i]
and ta_Arr[i]
.
If the user wants to change the outflow gas geometry, they only have to do
Geometry = 'Galactic Wind' # Other options: 'Thin Shell' or 'Bicone_X_Slab' f_esc_Arr = Lya.RT_f_esc( Geometry , V_Arr , logNH_Arr , ta_Arr )
Note that only one geometry can be used at the same time. If you want to compute different escape fractions ( or line profiles ) for different configurations you will need to call LyaRT;Grid
once per geometry.
These examples show how the 'Thin_Shell'
and 'Galactic_Wind'
geometries work. These geometries have spherical symmetry so there is no Line of Sight (LoS) dependence in the output escape fraction or line profile. However, LyaRT;Grid
implements a nonsphericalsymmetric geometry, the 'Bicone_X_Slab'
geometry (for details, again, we refer you to the presentation letter). In this particular geometry the escape fraction (and line profile) depends on the LoS. In particular, if you observed faceon (throught the biconical outflow) the optical depth is lower than observeing edgeon (through the static dense slab).
In order to tell LyaRT;Grid
the orientation of observation ( edgeon or faceon ) the user needs to provide anther varible when calling the code: Inside_Bicone_Arr
. If this is not given it is assumed that it's always observed faceon. This variable has to be a boolean array with the same size as V_Arr
, logNH_Arr
ot ta_Arr
. Additionally, the aperture angle of the bicone is 45deg, so to produce a set of escape fractions with random orientations in the biconenical geometry you should use:
import numpy as np Geometry = 'Bicone_X_Slab' Area_in_bicone = 1.  np.cos( np.pi/4. ) # the apperture angle is pi/4 Inside_Bicone_Arr = np.random.rand( len(V_Arr) ) < Area_in_bicone f_esc_Arr = Lya.RT_f_esc( Geometry , V_Arr , logNH_Arr , ta_Arr , Inside_Bicone_Arr=Inside_Bicone_Arr )
Deeper options on predicting the escape fraction (Unuseful section?).
There are many algorithims implemented to compute f_esc_Arr
. By default LyaRT;Grid
uses a machine learning decision tree regressor and a parametric equation for the escape fraction as function of the dust optical depth (Go to the LyaRT;Grid
presentation paper GurungLopez et al. in prep for more information). These settings were chosen as default since they give the best performance. However the user might want to change the computing algorithm so here leave a guide with all the available options.

MODE
variable refers to mode in which the escape fraction is computed. There are 3 ways in whichLyaRT;Grid
can compute this. i)'Raw'
Using the raw data from the RTMC (Orsi et al. 2012). ii)'Parametrization'
Assume a parametric equation between the escape fraction and the dust optical depth that allows to extend calculations outside the grid with the highest accuracy (inLyaRT;Grid
). iii)'Analytic'
Use of the recalibrated analytic equations presented by GurungLopez et al. 2018. Note that the analytic mode is not enabled in the bicone geometry although it is in the'Thin_Shel'
and'Galactic_Wind'

Algorithm
varible determines the technique used. This can be i)'Intrepolation'
: lineal interpoation is used. ii)'Machine_Learning'
machine learning is used. To determine which machine learning algorithm you would like to use please, provide the variableMachine_Learning_Algorithm
. The machine learning algorithms implemented are Decision tree regressor ('Tree'
), Random forest regressor ('Forest'
) and KN regressor ('KN'
). The machine learning is implemented byScikitlearn
, please, visit their webside for more information (http://scikitlearn.org/stable/).
MODE = 'Raw' # Other : 'Parametrization' , 'Analytic' Algorithm = 'Intrepolation' # Other : 'Machine_Learning' Machine_Learning_Algorithm = 'KN' # Other 'Tree' , 'Forest' f_esc_Arr = Lya.RT_f_esc( Geometry , V_Arr , logNH_Arr , ta_Arr , MODE=MODE )
Finally, any combination of MODE
, Algorithm
and Machine_Learning_Algorithm
is allowed. However, note that the variable Machine_Learning_Algorithm
is useless if Algorithm='Intrepolation'
.
Predicting thousands of Lyman alpha escape fractions.
In this section we explain how to obtain in a fast way an arbitray number of Lyman alpha line porfiles. The syntax is very similar to the one of escape fraction functions. The main difference is that the user must provide a wavelength array (in meters) where the line profile will be evaluated. The line profile of a thin shell outfow with expansion velocity (V) 200 km/s, logarithmic of column density (logNH) of 19.5 and dust optical depth (ta) of 0.1 in 20 amstrongs arround Lyman alpha can be computed as
wavelength_Arr = np.linspace( 1215.68  20 , 1215.68 + 20 , 1000 ) * 1e10 # meters, please! Line_profile_Arr = Lya.RT_Line_Profile( 'Thin_Shell' , wavelength_Arr , [ 200 ] , [ 19.5 ] , [ 0.1 ] )
As in the case of the escape fraction, in order to compute multiple line profiles at the same time just make
wavelength_Arr = np.linspace( 1215.68  20 , 1215.68 + 20 , 1000 ) * 1e10 # meters, please! V_Arr = [ 200 , 300 , 400 ] # Expansion velocity array in km/s logNH_Arr = [ 19.5 , 20.0 , 20.5 ] # Logarithmic of column densities array in cm**2 ta_Arr = [ 0.1 , 0.01 , 0.001 ] # Dust optical depth Array Line_profile_Arr = Lya.RT_Line_Profile( 'Thin_Shell' , wavelength_Arr , V_Arr , logNH_Arr , ta_Arr )
In this case, Line_profile_Arr
is an array with shape (3,1000) that contains the computed line profiles. In particular Line_profile_Arr[i,:]
is the line profile evaluated in wavelength_Arr
computed with V_Arr[i]
, logNH_Arr[i]
and ta_Arr[i]
.
The other geometries ('Galactic_Wind'
or 'Bicone_X_Slab'
) are also implemented. In particular, in the biconical geometry it is also possible to chose a line of sight observations. This is implemented in the same way as in the escape fraction.
In opposite to escape fraction calculations, the line profile only supports by now linear interpolation between the precomputed grids. Machine learning or deep learning might be implement in a future.
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