UCL MSSL Swift


A Statistical overview of the wavelength calibration accuracy

anchor position for clocked V grism

This figure shows the errors in the wavelength calibration. The blue dots are the anchor positions (at 260nm in first order) of the calibration spectra on the detector. The contours are a fit to the accuracy of the dispersion expressed as the RMS error between measured and predicted wavelength for known lines in the spectrum. 

The inset in the top left corner shows that at most times the anchor point that was predicted using the source position in the lenticular filters taken just before and after the observation has a systematic offset of 15.9 A.  Disregarding the systematic offset, the anchor position typically falls within 23 A (about 7 pixels) of the correct position. This is sufficient to avoid making misidentifications of the larger spectral features which have a FWHM which is comparable in magnitude.

The inset in the top right corner shows the accuracy of the adopted dispersion from the scaled zemax model after removal of the anchor point offsets as a root mean squared measure. The contours show the overall variaton over the detector.  For details, the actual fits given in the maps on this page should be consulted. The main result is, that the RMS error in the wavelengths in a spectrum is typically less than 16 A, which is about 5 pixels.


How to read the wavelength accuracy plots

Wavelength accuracy plots were made for each useful calibration spectrum.  The format of the accuracy plots is to have two panels.  Since the main variation of the dispersion can be represented by a constant with a linear term, the top panel of the accuracy plot has taken those two terms out. The higher order terms tend to zero near the adopted anchor point, which for the V-clocked grism mode is ~4200  Å.  The dispersion from the scaled optical model has been approximated with a polynomial. The observed line positions from lines identified in the calibration spectrum have been plotted as blue dots. The lower panel of these wavelength accuracy plots shows the remainder after subtraction of the predicted position. The observed position was found from the pixel distance to the anchor point and the dispersion relation, while the predicted position was found using the known wavelength.  If the model dispersion is good, the difference can be divided into an offset and a random looking spread around that offset. The values for that case are given in the plot. In some points near the edges of the detector, the scaled model dispersion deviates and the points will not evenly be distributed around some mean offset. 

The upper left corner (low det-X, high det-Y)  has no first orders because of the aperture effect from rotating the filterwheel.

A map for wavelength accuracy plots

The map below provides links to the wavelength accuracy plots.

anchor position for clocked UV grism

WR121 sw00057520006_1 WR4 sw00056900002_1 WR4 sw00056900004_1 WR4 sw00056900003_1 WR86 sw00057000002_1 WR52 sw00056950004_1 WR52 sw00057914001_1 WR52 sw00057911001_1 WR52 sw00057912001_1 WR52 sw00057913001_1 WR52 sw00057918001_1 WR52 sw00057920001_1 WR52 sw00057926001_1 WR52 sw00057916001_1 WR52 sw00057924001_1 WR52 sw00057915001_1 WR52 sw00057922001_1 WR52 sw00057919001_1 WR52 sw00057908001_1 WR52 sw00057905001_1 WR52 sw00057909001_1 WR52 sw00057923001_1 WR52 sw00057925001_1 WR52 sw00057921001_1 WR52 sw00057906001_1 WR52 sw00057904001_1 WR52 sw00057901001_1 WR52 sw00057902001_1 WR4 sw00056900001_1

A Map for count rate spectra

Here the count rate calibration spectra can be found. The top panel as a function of fitted wavelength, the bottom panel as function of pixel coordinate. The stronger lines have been identified. Any shifts between the predicted line position and the actual spectrum can be seen in the top panel as an offset.


anchor position for clocked UV grism
WR121 sw00057520006_1 WR4 sw00056900002_1 WR4 sw00056900004_1 WR4 sw00056900003_1 WR86 sw00057000002_1 WR52 sw00056950004_1 WR52 sw00057914001_1 WR52 sw00057911001_1 WR52 sw00057912001_1 WR52 sw00057913001_1 WR52 sw00057918001_1 WR52 sw00057920001_1 WR52 sw00057926001_1 WR52 sw00057916001_1 WR52 sw00057924001_1 WR52 sw00057915001_1 WR52 sw00057922001_1 WR52 sw00057919001_1 WR52 sw00057908001_1 WR52 sw00057905001_1 WR52 sw00057909001_1 WR52 sw00057923001_1 WR52 sw00057925001_1 WR52 sw00057921001_1 WR52 sw00057906001_1 WR52 sw00057904001_1 WR52 sw00057901001_1 WR52 sw00057902001_1 WR4 sw00056900001_1
The count rate in the spectra can be seen to vary across the detector, which is partly due to variations in sensitivity, and perhaps also to variablility in the source, which was chosen for calibrating the wavelengths using the many spectral lines.

The calibration file used was swwavcal20090626_v2_mssl_uc160_wlshift6.1.fits. In some browsers the maps do not work. In that case the plots/images can be found here.

In part, the uncertainty in the position of the anchor point is due to a possible drift of the pointing during the observation which can typically be around 4 pixels, which for a dispersion of 3.2A/pixel translates to about 13A.