We numerically study the collective dynamics of dense particle assemblies driven by non-reciprocal pairwise forces of amplitude κ. At a critical value κ ₂, the system undergoes a dynamical phase transition from an absorbing state (κ κ ₂). The chaotic phase is marked by nontrivial spatiotemporal velocity correlations and mixing, reminiscent of active turbulence in self-propelled systems. The sharp onset of chaos shows critical scaling consistent with the universality class of directed percolation. We argue that this transition is generic to a broad class of locally-driven, dense disordered materials.
Klamser et al. (Mon,) studied this question.
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