We discuss the scaring laws of both the charged fragments multiplicity a fl
uctuations and the charge of the largest fragment Z(max) fluctuations for X
e + Sn collisions in the range of bombarding energies between 25A MeV and 5
0A MeV. We show at E-lab greater than or similar to 32 MeV/A the transition
in the Fluctuation regime of Z(max) which is compatible with the transitio
n From the ordered to disordered phase of excited nuclear matter. The size
(charge) of the largest fragment is closely related to the order parameter
characterizing this process.