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Once the covariance matrix is built
one uses it in a
fit to get the
parameters of a function.
The quantity to be minimized is
, defined as
 |
(6.47) |
where
is the vector of the differences
between the theoretical and the experimental values.
Let us
consider the simple case in which two results of the same physical quantity
are available, and the individual and the common
standard uncertainty are known.
The best estimate of the true value of the physical quantity
is then obtained by fitting the constant
through the data points. In this simple case
the
minimization can be performed easily.
We will consider
the two cases of offset and normalization uncertainty. As before,
we assume that the detector is well calibrated, i.e. the most
probable value of the calibration constant is, respectively
for the two cases, 0 and 1, and hence 
Next: Offset uncertainty
Up: Use and misuse of
Previous: Use and misuse of
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Giulio D'Agostini
2003-05-15