We investigate the spread of correlations carried by an excitation in a
1-dimensional lattice system with high on-site energy disorder and long-range
couplings with a power-law dependence on the distance (∝r−μ). The
increase in correlation between the initially quenched node and a given node
exhibits three phases: quadratic in time, linear in time, and saturation. No
further evolution is observed in the long time regime. We find an approximate
solution of the model valid in the limit of strong disorder and reproduce the
results of numerical simulations with analytical formulas. We also find the
time needed to reach a given correlation value as a measure of the propagation
speed. Because of the triple phase evolution of the correlation function the
propagation changes its time dependence. In the particular case of μ=1, the
propagation starts as a ballistic motion, then, at a certain crossover time,
turns into standard diffusion