Fig. 8

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Raw interaction rate λ(q, q′) and entity interaction rate λent(q, q′, δ) for the runaway kernel (Eq. (70)). Parameters are: λ0 = 10−10, threshold mass mth = 107, total mass ℳ = 1011, n = 2048 representative particles, particle regime threshold Nth = 10. Many-particles swarms (N(q) > Nth) are assumed to have homogeneous swarm mass M(q) = ℳ/n, whereas few-particles swarms (N(q) ≤ Nth) are assumed to have been split up to represent only themselves, N(q) = 1, and thus have swarm mass M(q) = m(q); hence the discontinuity at mcrit.
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