When random assemblies of particles are cyclically sheared with a shear amplitude d, collisions between the particles cause the system to self-organize into a relatively ordered configuration where less collisions occur.For a small shear amplitude d, the particles finally settle into a reversible state where all the particles return to their initial position after each shear cycle, while they reach an irreversible state for d above a threshold amplitude dc . Using cyclically sheared vortices in amorphous MoxGe1-x films with random pinning, we have demonstrated the critical behavior of the reversible-irreversible transition (RIT). The relaxation time τ(d) to reach the steady state shows a power-law divergence at dc, indicative of a nonequilibrium RIT [2,3]. The critical exponent agrees with the value expected for an absorbing phase transition in the two-dimensional directed-percolation universality class . Recently, we have found that, when d is decreased to the average intervortex spacing in the reversible regime, τ(d) shows a significant drop, reflecting the suppression of vortex-vortex collisions . This indicates a transition or crossover from a loop-reversible state with vortex-vortex collisions to a collisionless point-reversible state . Here, we perform a detailed analysis of τ(d) in the reversible states and find that, in either regime, τ(d) exhibits a power-law divergence at the same dc with nearly the same exponent .
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Keywords: nonequilibrium transition, reversible-irreversible transition, absorbing phase transition