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eso-midas-doc-13SEPpl1.2-3.mga5.i586.rpm

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<H3><A NAME="SECTION001857300000000000000">
Individual data</A>
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<P>
Finally, the individual observations themselves are reduced, using the
parameters from the extinction solution.
This is a little tricky, as one needs color values to include the color terms
in both extinction and transformation equations.
If all colors are observed simultaneously, as is done with multichannel
spectrometers, these colors can easily be extracted from the neighboring
data.
But a filter photometer or CCD must observe passbands sequentially.
Again, this may not be a problem, if the star is constant in light.

<P>
However, for variable stars, the brightness is changing in all bands, and it is
difficult to define the correct color to use in the reduction.
In principle, one should construct the full light curve of the star, and then
interpolate the colors to the time at which each passband was observed.
In practice, a simpler compromise is used: the colors are simply interpolated
linearly in time, if there are earlier and later observations of the star on
the same night.
For the first and last observations of a star on a given night, the nearest
observations (in time) in the adjoining bands are used.
In every case, the values of the colors used to reduce each magnitude are shown
on the output.

<P>
Every observation is given individually, including observations of standard and
extinction stars, together with the U.T. day fraction and heliocentric Julian
Date.
These data are of interest for standard and extinction stars if they later
turn out to be variable.
Note that the values of stellar parameters
adopted in the extinction solution are to be preferred to
values obtained by averaging these individual observations
that have been corrected for extinction and transformation.

<P>
NOTE:
Because colors are needed to transform the observations, first to outside the
atmosphere and then to a standard system, only stars that were observed in all
passbands on a given night can be reduced in this section of the program.
This is in contrast to the treatment of constant stars in the general solution,
where even single-passband measurements are useful, provided that (a) every
star was observed at least once during the run in every passband;
and (b) every night has some observations in all passbands.

<P>
That is, the extinction solution can in principle produce results if we observe
extinction star 1 only in passband A and star 2 in passband B on night 1, and
star 1 only in passband B and star 2 in passband A on night 2.
This fulfills the requirements for data in both bands for each night, and for
each star.
Even if the passbands are linked by color terms in the extinction, the solution
is possible, because we do obtain mean colors for each star.
However, none of these data could be reduced individually, as there are no
observations of either star in both bands on the same night.

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<ADDRESS>
<I>Petra Nass</I>
<BR><I>1999-06-15</I>
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