ON THE ONSET OF QUANTUM FLUCTUATIONS AND CHAOTIC PROBABILITY

In general terms, non-conservation is introduced ad-hoc into the equat ions, in order to get a realistic description. Whether conservative or not, the behavior of the solution is univocal. Here we study two coup led difference logistic equations. Now the system is not univocally co nservative: during a period of time, it will be conservative with Haur sdorff dimension D-H less than or equal to 1 and finally, a smallest p erturbation will get over dimension 1 less than or equal to D-H less t han or equal to 2.