PIA data reduction for P03/P22 ------------------------------ (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 --> Correction --> non-linearity (Nonlinearities in the Cold Read-out Electronics output voltages and also de-biasing effects are mainly affecting the long-wave detectors with low bias P3, C100 and C200 and result in ramp Nonlinearities.) * 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. or --> use subdivided ramps (A better time resolution on the signal level can be reached by using the method of ramp sub-division. The user can define a pseudo-ramp with fewer read-outs than the original one. An important reason for ramp sub-division is for some cases with a very low number of ramps per chopper plateau.) SRD level: * Reset interval correction --> Correction --> Reset interval correction (There exists a signal dependance on the reset interval used for read-outs sampling. The effect is detector and CRE dependent and leads to signal differences if the same flux is measured using different ramp integration times.) * 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: --> 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 --> with drift handling: Stability recognition, ok (More sophisticated methods to derive the final signal are available under --> Process --> with drift handling: Drift modelling, ok) SCP level: * Vignetting correction --> Correction --> (The ISOPHOT detector pixels can be telescope vignetted depending on the aperture used and on the chopper throw. Only implemented for C100 and C200 detectors.) * Determination of actual Response (Measurement title says: staring FCS) --> Process --> Responsivity calculation * Power calibration of your on-source measurement --> Process --> Power calibration --> Actual Response or --> Default Response (orbit dep.): Customize, Perform it 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.) * Color Correction Check the lookup tables on the main PIA panel: --> Files --> Calibration Info --> Colour Correction Divide your obtained (source-background)-flux [Jy] by the color correction factor.