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Algorithms - Spectrophotometry

Because the SDSS spectra are obtained through 3-arcsecond fibers during non-photometric observing conditions, special techniques must be employed to spectrophotometrically calibrate the data.

On each spectroscopic plate, 16 objects are targeted as spectroscopic standards. These objects are color-selected to be F8 subdwarfs, similar in spectral type to the SDSS primary standard BD+17 4708.

standard star colors
The color selection of the SDSS standard stars. Red points represent stars selected as spectroscopic standards. (Most are flux standards; the very blue stars in the right hand plot are"hot standards"used for telluric absorption correction.)


The flux calibration of the spectra is handled by the Spectro2d pipeline. It is performed separately for each of the 2 spectrographs, hence each half-plate has its own calibration.

At least 3 exposures are obtained of each plate, sometimes under very different sky conditions, and occasionally on multiple nights. In order to effectively reject bad pixels when the data is combined, the gross exposure-to-exposure differences must first be removed. This is accomplished by the smear procedure which is described in detail separately.

The highest S/N exposure is used to derive the flux calibration. Spectro2d runs a PCA algorithm on the 8 spectra of flux standards and generates an eigenspectrum. This procedure eliminates bad pixels and any star spectra that deviate too much from the others. The eigenspectrum is then ratioed to a model F8 subdwarf. The result is fit with a spline to produce the flux correction. Since the red and blue halves of the spectra are imaged onto separate CCDs, separate red and blue flux calibration vectors are produced. These will resemble the throughput curves under photometric conditions.

throughput plot
Throughput curves for the red and blue channels on the two SDSS spectrographs.

 
Finally, the red and blue halves of each spectrum on each exposure are multiplied by the appropriate flux calibration vector. The spectra are then combined with bad pixel rejection and rebinned to a constant dispersion.

Comparisons of the calibrated spectra with the SDSS photometry allow us to access the spectrophotometric quality.


Last modified: Mon April 23 14:34:30 CST 2003