3.7. Spectrometer relative spectral response function

The relative spectral response function (RSRF) measured on-ground during PACS flight-module black-body measurements is displayed in Figure 3.14. Besides the overall trend of the RSRF, one of the most important issue is to calibrate with a high accuracy the ripples on short wavelength scales. It is particularly important for faint line detection and identification. The RSRF does not change (a lot) over the mission lifetime, however, an updated version will be made available to PACS observers when it is appropriate.

PACS spectrometer relative spectral response function measured on-ground, colored signs show the key wavelengths measured in the calibration block of every single observation.

Figure 3.14.  PACS spectrometer relative spectral response function measured on-ground, colored signs show the key wavelengths measured in the calibration block of every single observation.

The wavelength dependence of the absolute response of each spectrometer pixel is characterised by an individual relative spectral response function. Since this calibration file has been derived from the extended laboratory black-body measurements, its application to point sources requires additional diffraction corrections. The required correction curve is provided in Figure 3.15; however, partly extended sources may consequently show deviating spectral shapes according to their size and morphology.

Point source correction: The fraction of signal seen by the central PACS spectrometer spaxel. Dashed line: theoretical calculation from idealised PSF; solid line: 3rd order polynomial fit to results from rasters on Neptune.

Figure 3.15. Point source correction: The fraction of signal seen by the central PACS spectrometer spaxel. Dashed line: theoretical calculation from idealised PSF; solid line: 3rd order polynomial fit to results from rasters on Neptune.