A microscopic Landau-Ginzburg theory predicts the self-alignment strength at which an active crystal transitions from disordered motion to collective flocking, with a diverging correlation length.
Self-alignment and anti-self-alignment suppress motility-induced phase separation in active systems
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abstract
In this article, we investigate the impact of self-alignment and anti-self-alignment on collective phenomena in dense active matter. These mechanisms correspond to effective torques that align or anti-align a particles orientation with its velocity, as observed in active granular systems. In the context of motility-induced phase separation (MIPS) - a non-equilibrium coexistence between a dense clustered phase and a dilute homogeneous phase - both self- and anti-self-alignment are found to suppress clustering. Specifically, increasing self-alignment strength first leads to flocking within the dense cluster, and eventually to the emergence of a homogeneous flocking phase. In contrast, anti-self-alignment induces a freezing phenomenon, progressively reducing particle speed until MIPS is suppressed and a homogeneous phase is recovered. These results are supported by scaling arguments and are amenable to experimental verification in high-density active granular systems exhibiting self- or anti-self-alignment.
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cond-mat.soft 1years
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Flocking as a second-order phase transition in self-aligning active crystals
A microscopic Landau-Ginzburg theory predicts the self-alignment strength at which an active crystal transitions from disordered motion to collective flocking, with a diverging correlation length.