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ISOCAM Interactive Analysis User's Manual Version 5.0 - ISO - ESA

ISOCAM Interactive Analysis User's Manual Version 5.0 - ISO - ESA

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280 CHAPTER 21. USING SLICE WITHIN CIA<br />

The third one corresponds to the “inflat” method of CIA where you provide a flat-field to<br />

SLICE. The only enhancement here is that you can either use a single flat-field image or provide<br />

a flat-field cube with as many planes as the data cube. Assuming you have this flat in variable<br />

my flat, to use this method you need to type:<br />

CIA> red param=set red param(tdt=’65801627’)<br />

CIA> act = set act(/make map)<br />

CIA> slice pipe,flat in=my flat<br />

For some reason, SLICE will erase your flat variable during its processing, so before starting<br />

slice pipe, make a copy of your flat-field cube.<br />

Now the three specifically SLICE methods are:<br />

• Sliding Mean flat-field: where the flat-field is derived from the mean of the data cube<br />

taken on a sliding window of readouts. This is satisfactory if your sources are not very<br />

strong, but if this is not the case, or if you have large scale structures, you run the risk<br />

of seeing some of these structures go into the flat-field, which is not advisable. You could<br />

protect yourself from that using a large sliding window, typically around 10 time N exp but<br />

this is not always possible (i.e. when you have a small number of raster positions).<br />

• Perturbed Single Flat-Field: although this does not sound much better, this is actually<br />

an improved flat-field method. Here, using a median filter on the individual raster pointings,<br />

the object structures are removed before an “auto”-like flat is computed. Then, still<br />

using a sliding window over the readouts, perturbations to this single flat-field are computed.<br />

The interesting point here is that since the object structures have been removed,<br />

the size of the window can be smaller than in the previous case.<br />

• Variable flat with Sky Divided (or DivSky): this is the ideal method where an<br />

estimation of the sky is divided out of the images before the flat-field is computed. This<br />

estimate of the ideal sky is done by smoothing the current value of the map. Therefore<br />

it is immediately clear than a first flat-field correction must have occurred through the<br />

make map action 3 . This is also the reason why two successive make map actions using<br />

DivSky with the same settings can produce different maps (although the differences are<br />

small). This is however the method which can be affected by the long-term transient or<br />

affect its determination. Therefore we recommend to use it after the long-term transient<br />

has been removed, and in combination with another flat-field method to produce the first<br />

version of map.<br />

You will rapidly see that in general, as far as flat-fielding quality goes, the DivSky method<br />

produces apparently the best results (compare, for instance, Fig. 21.2 with Fig. 21.3). However,<br />

it is also the method whose interaction with the long-term transient correction is the most<br />

complex, and which can lead to strong artifacts. Therefore, in this section we describe them<br />

both, but in sec. 21.5.3 we will use the Perturbed Single Flat-Field method to determine<br />

the long-term transient correction.<br />

Also note that SLICE now gives you the choice of working either on the cube of raster<br />

positions, or on the full readout cube. The latter option is obtained by adding /docube on the<br />

slice pipe command line. Although this is in principle better, the differences at this stage are<br />

3 try using it at the start of your SLICE session and you will see that SLICE uses the Sliding Mean<br />

Flat-Field method instead!

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