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where n is the signal X length, k is a fixed window size, and m is the largest integer not
exceeding n/k .
The local Hölder function H ( x ) at point
i
x
(5)
n
1
is given by (Peltier and Lévy-Véhél, 1994, 1995; Muniandy et al. , 2001 ; Li et al. , 2007, 2008;
Gaci et al. , 2010):

log
2
k, Si
ˆ Hi


(6)
log
n
1
From figure 3, it can be seen that all the calculated amplitude spectra, represented in a log-
log plan, decay algebraically, the analyzed data exhibit then a fractal behavior. Moreover,
the latter is described by a Hölder exponent varying with the latitude of the measure. Hence
the data can be considered as paths of multifractional Brownian motions (mBms) (Peltier
and Lévy-Véhel, 1995; Gaci et al. , 2011).
A significant result deserves to be noted is the fact that the spectra obtained from the ''raw'',
''corrected'' and ''corrected and interpolated'' measurements display a similar form. That is
the applied operations (corrections and interpolations) do not affect the fractal aspect of the
raw data.
a)
Fig. 3. (Continued)
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