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. 2024 May 8;121(20):e2400689121. doi: 10.1073/pnas.2400689121

Fig. 2.

Fig. 2.

Sufficiently long gossip stabilizes cooperation. (AD) Dynamics of competition among strategies ALLC, ALLD, and DISC under the Stern Judging norm, with a fixed benefit-to-cost ratio (b/c=5). (A and C) Gradients of selection (arrows) in the replicator dynamics (Eq. 6)). There is a basin of attraction toward the DISC vertex (shaded region) when τ=0.4>τ (A) but not when τ=0.0<τ (C). (B and D) Trajectories of stochastic simulations in a finite population (N=100), with x’s indicating different initial conditions (Materials and Methods). The long-term behavior of the stochastic simulations is consistent with the analytical predictions of the replicator-dynamic ODEs (B vs. A; D vs. C): When τ=0.4>τ (B), trajectories starting from initial conditions above the separatrix tend to converge to the DISC vertex (the shaded region denotes the basin of attraction in A). When τ=0.0<τ (D), all six trajectories converge to the ALLD vertex. (E) The discriminator-only equilibrium (fALLD=1) is locally stable only if the scaled gossip duration τ exceeds a critical value τ (solid orange curve defined by condition ii) and b/c exceeds a critical value (b/c) (dashed gray line defined by condition i). The orange region indicates parameter values where both these conditions are satisfied. The critical gossip duration τ decreases with the benefit-to-cost ratio, b/c. (F and G) The average reputation and agreement level as a function of time t during the process of reputation dynamics by independent observations and gossip (Eq. 2). These quantities are evaluated at the DISC vertex (fDISC=1) with a fixed benefit-to-cost ratio (b/c=5). Colors correspond to different values for the duration of gossip periods, τ. The lightest green corresponds to τ=0.0 (no gossip), which is equivalent to private reputations. The gray dashed curves correspond to τ (infinitely long gossip), which is equivalent to public reputations. Other parameters: ua=ue=0.02. Analogous results for the Simple Standing and Shunning norms are shown in SI Appendix, Fig. S2.