We perform an analysis on the dissipative Olami-Feder-Christensen model on a small world topology considering avalanche size differences. We show that when criticality appears, the probability density functions PDFs for the avalanche size differences at different times have fat tails with a q-Gaussian shape. This behavior does not depend on the time interval adopted and is found also when considering energy differences between real earthquakes. Such a result can be analytically understood if the sizes released energies of the avalanches earthquakes have no correlations. Our findings support the hypothesis that a self-organized criticality mechanism with long-range interactions is at the origin of seismic events and indicate that it is not possible to predict the magnitude of the next earthquake knowing those of the previous ones

Analysis of self-organized criticality in the Olami-Feder-Christensen model and in real earthquakes

VINCIGUERRA, Sergio Carmelo;
2007-01-01

Abstract

We perform an analysis on the dissipative Olami-Feder-Christensen model on a small world topology considering avalanche size differences. We show that when criticality appears, the probability density functions PDFs for the avalanche size differences at different times have fat tails with a q-Gaussian shape. This behavior does not depend on the time interval adopted and is found also when considering energy differences between real earthquakes. Such a result can be analytically understood if the sizes released energies of the avalanches earthquakes have no correlations. Our findings support the hypothesis that a self-organized criticality mechanism with long-range interactions is at the origin of seismic events and indicate that it is not possible to predict the magnitude of the next earthquake knowing those of the previous ones
2007
75
05510(R)
-
http://pre.aps.org/
Caruso F.; Pluchino A.; Latora V.; Vinciguerra S.; Rapisarda A.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/96413
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