In this article we study the characteristics of multifragmentation pat
terns induced by spinodal instabilities using a stochastic mean-field
approach. For two-dimensional unstable nuclear matter, we find that th
e early fragmentation process occurs accordingly to few dominant unsta
ble wavelengths, This favours the partition of the system in close-mas
s pieces, with a lack of very small fragments, Then, we consider the r
ealistic case of spherical systems initialized at low density. The rol
e of finite-size effects, final-state interaction and secondary decay
is carefully investigated. We discuss under which conditions some memo
ry of the first dynamical stage survives in the final fragment partiti
ons.