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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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