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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
 fit to get the 
 parameters of a function. 
The quantity to be minimized is 
 , defined as
, 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
 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
 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
 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