Chiral motion in the non-reciprocal two-species Vicsek model is stable only inside a narrow window of high density, very low speed, small system size, and dominant aligning couplings; imbalances or strong anti-alignment drive segregation or parallel flocking instead.
Predator–prey interactions between droplets driven by non-reciprocal oil exchange,
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Stability and breakdown of chiral motion in non-reciprocal flocking
Chiral motion in the non-reciprocal two-species Vicsek model is stable only inside a narrow window of high density, very low speed, small system size, and dominant aligning couplings; imbalances or strong anti-alignment drive segregation or parallel flocking instead.