  Jammed granular media and glasses exhibit spatial long-range correlations as
a result of mechanical equilibrium. However, the existence of such correlations
in the flowing matter, where the mechanical equilibrium is unattainable, has
remained elusive. Here, we investigate this problem in the context of the
percolation of interparticle forces in flowing granular media. We find that the
flow rate introduces an effective long-range correlation, which plays the role
of a relevant perturbation giving rise to a spectrum of varying exponents on a
critical line as a function of the flow rate. Remarkably, our numerical
simulations along with analytical arguments predict a crossover flow rate
$\dot{\gamma}_c \simeq 10^{-5}$ below which the effect of induced disorder is
weak and the universality of the force chain structure is shown to be given by
the standard rigidity percolation. We also find a power-law behavior for the
critical exponents with the flow rate $\dot{\gamma}>\dot{\gamma}_c$.
