Instrument Configuration Files
Most of these parameters are the subject of considerable calibration efforts, and as such, should not be adjusted if the results are to be trusted. These files are obtained with the configuration module and are stored in $HOME/.slitlessutils/<VERSION>/instruments/
Instrument-Wide Settings
Keyword |
Unit |
Description |
|---|---|---|
Image units |
\(\mathrm{e}^-/\mathrm{s}\) or \(\mathrm{e}^-\) |
The units of the images to be written. |
File suffix |
|
The file suffix in the HST parlance denoting files without and
with the CTE corrections, respectively.
|
Path |
|
The relative path from the
yaml file where the files for thisinstrument are stored.
|
Focal-plane position |
3-elements |
The \((v_2,v_3)\) position of the reference point
and \(v_{3y}\) angle with respect the \(v_3\)-axis.
|
Instrument-Wide Grating/Blocking Parameters
Keyword |
Unit |
Description |
|---|---|---|
Global-Sky Image |
The name of the global-sky image. |
|
Tabulation Parameters |
|
This contains the starting wavelength (
wave0), endingwavelength (
wave1), sampling rate (dwave),units (usually
angstrom), and disptype (which isalways “grism”).
|
Extraction Parameters [2] |
|
This contains the starting wavelength (
wave0), endingwavelength (
wave1), sampling rate (dwave),units (usually
angstrom), disptype, and ifalpha for prisms. |
Details on Extraction Settings
The extraction parameters for a grism and prism will be different, owing to the non-linear dispersion in a prism. Since a grism is linear, the formulae for the \(i^\mathrm{th}\) extraction wavelength (\(\lambda_i\)) and the number of wavelength elements (\(N\)) are:
where \(\lambda_0\), \(\lambda_1\), and \(\delta\lambda\) are the starting wavelength (wave0), ending wavelength (wave), and sampling rate (dwave), respectively. The notation \(\lceil x \rceil\) refers to the ceiling function of x. For the prisms, which are highly nonlinear, the same two equations become:
where \(\Delta\lambda\!=\!(\lambda_1-\lambda_0)\) and \(\alpha\) is a curvature parameter that adjust the degree of non-linearity. This form has several limiting forms worth mentioning. If \(\alpha=0\), then there will be a single wavelength element (\(N=1\)), emulating the photometry from an imaging mode. Second, if \(\alpha\gg n\), then the prism function approaches the linear form for a grism.
Note
In general, users are discouraged from adjusting these settings in the reference files, and are recommended to instead use the API (see sources). Extraordinary care should be taken regarding the curvature parameter.
Detector Parameters
Keyword |
Unit |
Description |
|---|---|---|
Focal-plane position |
3-elements |
\((v_2,v_3)\) position of the reference point
\(v_{3y}\) angle with respect the \(v_3\)-axis
|
Extension properties |
name: the name of the extension (must be str)ver: the version of the extension (must be int)dtype: a valid np.dtype |
|
Noise properties |
dark current \(D\) in \(e^-/s\)
readnoise \(R\) in \(e^-\)
|
|
Detector dimensionality |
naxis: 2-element list of size of detector (must be int)crpix: 2-element list for reference position (can be float)scale: 2-element list for pixel scale (can be float) |
|
Distortion model |
SIP coefficients should be a |
|
Configuration files |
The file name for each grating/blocking combination |
Footnotes