We present here a microscopic theory for fracture nucleation in finite
chains, which may account for results found in simulations and in som
e experimental situations. We obtain the characteristic breaking time
for an ensemble of one-dimensional Lennard-Jones chains, which is main
ly a large prefactor times an Arrhenius rate. We show that the express
ion scales well and that the activation energy agrees with the analyti
cal results. We show that the delay in the fragmentation is a conseque
nce of the long-range time correlation in the relative motion of two a
djacent particles. This correlation is responsible for the origin of a
self-organized memory as well as the large elongation necessary for i
rreversible break to occur. We discuss the possibility of using this s
imple theory to understand the main characteristic of fragmentation in
more complex and realistic systems. [S0163-1829(98)01717-2].