Exoplanet Timeseries Characterisation - Instrument Systematic Marginalisation
This code performs Levenberg-Marquardt least-squares minimisation across a grid of pseudo-stochastic instrument systematic models to produce marginalised transit parameters given a lightcurve for a specified wavelength range.
This was developed and tested for data from Wide Field Camera 3 (WFC3) on the Hubble Space Telescope (HST), specifically with the G141 spectroscopic grism, as published in Wakeford et al. (2016). This method can also be applied to the WFC3 IR G102 grism, and UVIS G280 grism by selecting the correct parameters. Future work includes plans to extend this to Space Telescope Imaging Spectrograph (STIS) instrument data, and eventually data from the James Webb Space Telescope (JWST).
This code follows the method outlined in Wakeford et al. (2016), using marginalisation across a stochastic grid of 50 polynomial models (see bottom for full grid). These 50 instrument systematic models contain a combination of corrective factors for likely HST systematics. These include a linear trend in time across the whole lightcurve, accounting for HST breathing effects caused by thermal changes in the telescope with up to a 4th order polynomial, and correcting for positional shifts of the target spectrum on the detector fitting up to a 4th order polynomial. See Wakeford et al. (2016) section 2.2 for details and Table 2 therein for the full grid of systematic models included.
The evidence (marginal liklihood) is calculated from the AIC for each model when fit with the data and converted to a normalised weighting that is used to marginalise each of the global fit parameters. See equations 15 and 16 in Wakeford et al. (2016) to marginalise over the parameters and their uncertainties.
Additional functions in this package that can be utilized independently include the following:
- The program makes use of the analytic transit model in Mandel & Agol (2002) that has been translated into python and can be used independently to fit any transit lightcurve once exotic-ism has been installed.
- It utilizes Levenberg-Marquardt least squares minimisation using Sherpa, a Python package for modeling and fitting data.
- The transit model uses a 4-parameter limb darkening law, as outlined in Claret (2010) and Sing (2010) using 1D Kurucz stellar models (provided on install of this package) or 3D stellar models for a smaller subset of parameters from Magic et al. (2015).
This package was built from the original IDL code used for the analysis in Wakeford et al. (2016), initially translated by Matthew Hill and then further adapted and transformed into a full astronomy Python package with the help of Iva Laginja.
Note how this package is not distributed through pip or conda, so you will always need to clone it if you want to work with it.
Current supported instruments and gratings are:
HST WFC3 IR/G102, IR/G141 grisms
This section will you give all the necessary terminal commands to go from opening our GitHub page in the browser to having reduced results of the template data on your local machine. For a more thorough description of the individual steps, please continue to the section Prerequisites and beyond.
For a tutorial on ExoTiC-ISM, please see notebooks
--> tutorials
--> 1_Intro-tutorial.ipynb
.
We assume that you have conda
and git
installed and that you're using bash
.
- Navigate to the directory you want to clone the repository into:
$ cd /User/<YourUser>/repos/
- Clone the repository:
$ git clone https://github.com/hrwakeford/ExoTiC-ISM.git
or use SSH if that is your preferred way of cloning repositories:
$ git clone [email protected]:hrwakeford/ExoTiC-ISM.git
- Navigate into the cloned repository:
$ cd ExoTiC-ISM
- Create the
exoticism
conda environment:
$ conda env create --file environment.yml
- Activate the environment:
$ conda activate exoticism
- Install the package into this environment, in editable mode:
$ python setup.py develop
- Go into the code directory:
$ cd exoticism
-
Copy the file
config.ini
and name the copyconfig_local.ini
. -
Open your local configfile
config_local.ini
and edit the entry[data_paths][local_path]
to point to your local repo clone that you just created, e.g.:
[data_paths]
local_path = /Users/<YourUser>/repos/ExoTiC-ISM
- In the same file, define with
[data_paths][output_path]
where your output data should be saved to, e.g.:
[data_paths]
...
output_path = /Users/<YourUser>/<path-to-data>
- Activate the conda environment you just created:
$ conda activate exoticism
- Run the marginalisation on the demo data from the template:
$ python marginalisation.py
The script takes a short while to run and will output messages to the terminal and save the final data to the path you
specified under [data_paths][output_path]
in your config_local.ini
!
This is not an installable package (yet), so you will need to clone it if you want to work with it. Sherpa is distributed for Mac and Linux, this means Windows users will have to use a Linux virtual machine or find an alternative solution.
We highly recommend the usage of the package and environment manager Conda, which is free and runs on Windows, macOS and Linux. We have included an environment file in our repository from which you can directly build a new conda environment in which we have tested our package. We developed and tested our package with Python 3.7.3 in conda 4.6.7.
After cloning the repository, run
$ conda env create --file environment.yml
to build the environment, or optionally
$ conda env create --name <myEnvName> --file environment.yml
to give the environment your own name.
The last step is to install the exoticism
package into your newly created environment. We do currently not support a
plain install ($ python setup.py install), instead please install it in editable mode:
$ python setup.py develop
The main configuration file is config.ini
, which holds all of your simulation parameters. This specific file,
however, is version controlled, and the paths to local directories will get messed up if you push or pull this
file; you might also lose the changes you made to the parameters. This is why config.ini
is initially supposed to be used as a template.
In order to make it work for you, copy config.ini
and rename the copy to config_local.ini
. In this local configfile,
you can set all your parameters, and it will override the config.ini
at runtime. Whichever configfile is used in the end,
the version controlled one or the local one, a copy of it is always saved together with the output data. In the case you
want to version control the configfile you use, we recommend that you fork the repository and simply use the config.ini
file directly.
The configfile has the following structure, except here we added some extra comments for clarity:
[data_paths]
local_path = /Users/MyUser/repos/ExoTiC-ISM ; your global path to the repo clone
input_path = ${local_path}/data ; global path to the input data, defaults to template data in repo
output_path = /Users/MyUser/outputs ; global path ot the output directory
run_name = testing ; suffix for output data directory
[setup]
data_set = W17 ; data selection; refers to section in configfile
instrument = WFC3
grating = G141
grid_selection = fit_time
ld_model = 3D ; 3D or 2D limb darkening model
plotting = True
report = True
[smooth_model]
resolution = 0.0001
half_range = 0.2
; Stellar and planet system parameters - make a new section for each new data set
[W17]
lightcurve_file = W17_${setup:grating}_lightcurve_test_data.txt ; lightcurve data file
wvln_file = W17_${setup:grating}_wavelength_test_data.txt ; wavelength data file
rl = 0.12169232 ; Rp/R* estimate - the transit depth
epoch = 57957.970153390 ; in MJD
inclin = 87.34635 ; inclination in deg
ecc = 0.0 ; eccentricity in deg
omega = 0.0 ; deg
Per = 3.73548535 ; planet period in days
aor = 7.0780354 ;a/r* (unitless) --> "distance of the planet from the star (meters)/stellar radius (meters)"
; limb darkening parameters
metallicity = -1.0 ; stellar metallicity
Teff = 6550 ; stellar effective temperature
logg = 4.5 ; log gravity of star
[constants]
dtosec = 86400 ; conversion factor from days to seconds
HST_period = 0.06691666 ; Hubbe Space Telescope period in days
The relevant data files and plots from your run, together with the used configfile, will be saved to the directory you specify under output_path
in your
local configfile. The results of each new run will be saved in a subdirectory under [data_paths] -> output_path
that is labelled with a time stamp, the
name of the stellar system data and a custom suffix, which you set in the configfile.
We provide demo data for the exoplanet WASP-17b, which is one of the datasets analyzed in Wakeford et al. (2016). Please refer to section "Supported instruments and gratings" for a list of currently supported instruments and gratings. If you want to perform the marginalisation on a different transit dataset, you have to point the configfile to your input data folder and also update the planetary parameters by adding a new section to the configfile.
Due to the structure of the configfile (see above), we follow this naming convention for input files:
star + grating + arbitrary string + .txt
E.g.: "W17_G141_lightcurve_test_data.txt"
The star and grating can then be set once in the config section '[setup]', while the full filename needs to be added in
the respective stellar and planetary parameters section, with a placeholder for the grating name.
E.g.: "W17_${setup:grating}_lightcurve_test_data.txt"
All header lines should start with '#'.
This table shows the functional form of the systematic models as presented in Wakeford et al. (2016). Each check mark shows which of the parameters are thawed in the model and fit to the data in combination. The grid contains corrections for a linear trend in time across the whole observation, corrections for thermal variations on the time scale of a HST orbit around the Earth, and positional shifts of the observed spectrum on the detector.Please see here how to run our units tests locally.
Please read CONTRIBUTING.md for contribution guidelines, and the process for submitting issues and pull requests to us. Please also see our CODE OF CONDUCT.
If you use this code in your work, please find citation snippets to give us credits with in CITATION.txt.
- Hannah R. Wakeford - Method author - @hrwakeford
- Iva Laginja - Turning the code into a functional Python repository - @ivalaginja
- Matthew Hill - Translation from IDL to Python - @mattjhill
This project is licensed under the MIT License - see the LICENSE.md file for details.
- Tom J. Wilson for statistical testing of the code
- Matthew Hill for a functional translation from IDL to Python
- Iva Laginja for finding
Sherpa
, making the clunkympfit
dispensable - The
Sherpa
team, providing a fantastic package and answering fast to GitHub issues - This work is based on observations made with the NASA/ESA Hubble Space Telescope, HST-GO-14918, that were obtained at the Space Telescope Science Institute, which isoperated by the Association of Universities for Research in Astronomy, Inc.