PIA data reduction for P40 ------------------------------ (details about the individual correction/processing algorithms can be found in: http://www.iso.vilspa.esa.es/manuals/PHT/pia/um/processing.html) ERD level: * Non-linearity correction (not available for P40) * Read-out deglitching --> Test processing --> Test deglitching (single or 2 Threshold method) --> Accept & Quit --> Correction --> Read-out simple deglitching or 2 Threshold deglitching (Cosmic particles hit the detector pixels with such energy, that the voltage ramps are seriously disturbed: local 'jumps' between 2 read-outs, or even 3 read-outs, and an immediate relaxation. the information redundancy on voltage differences between read-outs allows us to pick out those anomalous jumps and to correct the ramps affected. The 2 Threshold deglitching is more efficient.) * Saturated Ramps --> Correction --> Change Saturation Params (Integration of a ramp above the saturation limit (~ 1.2 V) is not possible. An automatic recognition for all cases has been introduced in PIA. Changing the Parameters is usually not necessary.) * Raster point ID correction for tracked SSO observations --> Correction --> Set RPID -> [1,1] (PIA considers now the measurement as tracked observation. PIA does not automatically recognize the tracking mode, since it is performed in the same way as rasters.) * Ramp fitting --> Process Measurement --> Fit ramps --> 1st order Pol. SRD level: * Reset interval correction (not applicable at the moment) * Signal Deglitching --> Correction --> Deglitching --> Customize: 2 Iterations (or more), Use max/min clipping --> Correction --> Deglitching --> Perform it (There is also the posibility to do the deglitching manually for each pixel: --> Test processing --> discard area graphically) * Dark current subtraction --> Correction --> Dark current subtr. (orbital dep.) --> Customize: Interpolate one value per data point, ok --> Correction --> Dark current subtr. (orbital dep.) --> Perform it (Dark currents exist for every detector pixel, binned reflecting the dependence of the dark currents on the orbital position. For several detectors (mainly Ge:Ga) the cosmic hit radiation plays a dominant role and changes the dark currents with orbit position.) * Signal derivation --> Process --> dynamic calibration --> customize & perform: select 2 or more standard stars (deselect late type stars) (The basic assumption of the dynamic calibration is that the transients behaviour (eg temporal response) of an individual pixel depends primarily on the flux level observed with a high reproducibility under a similar illumination history of the detector. A comparison of the signals achieved by the target to the ones achieved by different calibrators after same time intervals within an observation allows a discrimination of the nearest calibrators in flux to the target. The ratios obtained are then used for deriving the unknown target flux. A deselection of late type stars (K2 and later) from the list of standards is in some cases recommended. Late type stars show the fundamental SiO absorption band (between 7 and 9.5 micron), which seems to be not well modelled.) Dynamic Calibration Data Display * Flux Calibration --> Process --> Combine all calibrators --> weighting by ratio or --> weighting by sigma AAP level: * Background subtraction (should be done preferably on SCP level to avoid color correction problems) --> Process --> Background Subtraction --> another measurement (the background measurement has to be in the buffer, reduced in the same way.) * Display the SS-part of the spectrum --> Array --> Spectra --> Flux Density --> New * Load the SL-part of the spectrum --> Data --> Load (click on SL-Measurement, ok) * Overplot the SL-part of the spectrum --> Array --> Spectra --> Flux Density --> Overplot --> Synchronized