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2410.15330

Decoding how higher-order network interactions shape complex contagion dynamics

István Z. Kiss, Christian Bick, Péter L. Simon

wrongmedium confidenceCounterexample detected
Category
math.DS
Journal tier
Specialist/Solid
Processed
Sep 28, 2025, 12:56 AM

Audit review

The paper’s Proposition 3.3 asserts that for the 4th-order mean-field SIS model ẏ = (C2−γ)y + (C3−C2)y^2 + (C4−C3)y^3 − C4y^4, if C3 < γ and C4 > γ, then the (C2,y) equilibrium curve has two fold points, citing the identity C2(y)=γ/(1−y)−C3 y−C4 y^2 and a discussion of an inflection when C4>γ as its proof sketch . However, differentiating gives F(y)=dC2/dy=γ/(1−y)^2−C3−2C4 y, which is strictly convex, so two folds occur if and only if min F(y)<0. This yields the necessary and sufficient threshold C3>3γ^{1/3}C4^{2/3}−2C4; otherwise there are zero folds (a cusp at equality). The paper’s proof only observes an inflection point and does not establish the two-fold condition, and in fact the unconditional claim is false (e.g., γ=1, C3=0.5, C4=2 gives no folds). By contrast, the candidate solution derives the correct threshold and full stability picture; its local transcritical classification also matches the paper’s 3-body case (Prop. 3.1) and the 4-body local result at C2=γ .

Referee report (LaTeX)

\textbf{Recommendation:} major revisions

\textbf{Journal Tier:} specialist/solid

\textbf{Justification:}

The paper offers a coherent framework linking higher-order contagion mechanisms to low-dimensional mean-field dynamics and gives a useful taxonomy of local and some global behaviors. However, a central global claim in the 4-body case (two folds whenever C3<γ<C4) is stated without the necessary condition and is incorrect as written. The proof sketch conflates the presence of an inflection with the existence of two folds. Correcting Proposition 3.3 with the precise threshold C3>3γ\^{1/3}C4\^{2/3}−2C4 (and discussing the cusp equality) is essential; with this fix, the work would be a solid reference.