Abstract

In evolutionary game dynamics, reproductive success increases with the performance in an evolutionary game. If strategy A performs better than strategy B, strategy A will spread in the population. Under stochastic dynamics, a single mutant will sooner or later take over the entire population or go extinct. We analyze the mean exit times (or average fixation times) associated with this process. We show analytically that these times depend on the payoff matrix of the game in an amazingly simple way under weak selection, i.e. strong stochasticity: the payoff difference Δπ is a linear function of the number of A individuals i, Δπ=u i+v. The unconditional mean exit time depends only on the constant term v. Given that a single A mutant takes over the population, the corresponding conditional mean exit time depends only on the density dependent term u. We demonstrate this finding for two commonly applied microscopic evolutionary processes.

Highlights

  • The average fixation times for such onedimensional random walks can be interpreted as mean first passage times or mean exit times [27]–[29]

  • We show that under weak selection, the conditional time (t1A) during which a single mutant takes over the whole population depends only on u

  • Our results are valid for a broader class of processes, we only present the full calculation for this evolutionary process

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Summary

Fermi process

In a finite population of size N with two possible strategies A and B, the state of the system is characterized by the number of type A individuals i. B players is given by π = u i + v, with i as the number of A players Both the transition probabilities Ti+ and Ti− and the probability that a single A player takes over the population φ1 depend on u and v. The first individual switches to the second’s strategy with probability pi±. The second individual can switch to the first individual’s strategy with probability 1 − pi±. This yields a factor 2 in the transition probabilities This process has a proper strong selection limit, i.e. it is possible to examine β → ∞ In this latter case, we have pi± → ( π(i)), where (x) is the step function. Weak selection links the Fermi process to a variety of birth–death processes, cf [8, 33]

Fixation probabilities and fixation times
Neutral selection
Weak selection
Frequency dependent Moran process
Discussion
Dominance of A
Coordination games
Full Text
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