Motility-Induced Phase Separation (MIPS)
Run-and-tumble particles · self-trapping · dense cluster nucleation
MIPS arises purely from motility — no attractive forces needed. Fast self-propelled particles
accumulate where they slow down (dense regions), creating a positive feedback: dense → slow → denser.
The effective swim pressure Pswim = ρv₀²τ/d decreases with density (anomalous EOS),
triggering a mechanical instability analogous to van der Waals. The critical Péclet number
Pe = v₀/(λσ) must exceed ~5–10 depending on φ. Above the binodal, the system
phase-separates into a dense solid-like cluster and a dilute gas of fast swimmers.