Intermittency quantification
The intermittency can be quantified using the definition of the flatness. To this end, we use a high pass filtered signal
defined as :

We can say that the variable
is intermittent at small scales if the flatness grows without bound with the filter frequency
.


The flatness is useful measure of intermittency for signals having a bursty aspect. Instead of flatness it is possible to use other nondimensional ratios, such as the moment of order 6 divided by the cube of the second moment order.