it is well known that oxide glasses build up continuous networks. Therefore
the rigidity of the latter plays a key role in understanding glass propert
ies. The network switches from floppy to rigid if the number of covalent br
idges between the network formers exceeds a certain threshold value. One an
d the same structure could behave as rigid network in respect to some prope
rties and could be floppy networks in respect to some other properties. Kin
etics of phase transition (and most the nucleation processes) is very sensi
tive to the rigidity of the network.
Some tiny floppy regions still exist inside the rigid network close above t
he threshold concentration, They can serve as active centers for the beginn
ing of nucleation process, Much later, nucleation can appear in the rigid p
art of the network. Therefore, we predict a certain interval of concentrati
on of rigid bounds in which a bimodal size distribution function of the for
med phase will be observed. This prediction is confirmed by experimental da
ta we find in literature.