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Édouard Strickler

Publications and source records attributed to Édouard Strickler.

3 recordsLinked to original sources

Impacts of Tempo and Mode of Environmental Fluctuations on Population Growth: Slow- and Fast-Limit Approximations of Lyapunov Exponents for Periodic and Random Environments

We examine to what extent the tempo and mode of environmental fluctuations matter for the growth of structured populations. The models are switching, linear ordinary differential equations $x'(t)=A(σ(ωt))x(t)$ where $x(t)=(x_1(t),\dots,x_d(t))$ corresponds to the population densities in the $d$ individual states, $σ(t)$ is a piece-wise constant function representing the fluctuations in the environmental states $1,\dots,N$, $ω$ is the frequency of the environmental fluctuations, and $A(1),\dots,A(n)$ are Metzler matrices. $σ(t)$ can either be a periodic function or correspond to a continuous-time Markov chain. Under suitable conditions, there is a Lyapunov exponent $Λ(ω)$ such that $\lim_{t\to\infty} \frac{1}{t}\log\sum_i x_i(t)=Λ(ω)$ for all non-negative, non-zero initial conditions $x(0)$ (with probability one in the random case). For both forms of switching, we derive analytical first-order and second-order approximations of $Λ(ω)$ in the limits of slow ($ω\to 0$) and fast ($ω\to\infty$) environmental fluctuations. When the order of switching and the average switching times are equal, we show that the first-order approximations of $Λ(ω)$ are equivalent in the slow-switching limit, but not in the fast-switching limit. We illustrate our results with applications to stage-structured and spatially-structured models. When dispersal rates are symmetric, the first order approximations suggest that population growth rates increase with the frequency of switching -- consistent with earlier work on periodic switching. In the absence of dispersal symmetry, we demonstrate that $Λ(ω)$ can be non-monotonic in $ω$. In conclusion, our results show how population growth rates depend on the tempo ($ω$) and mode (random versus deterministic) of the environmental fluctuations.

q-bio.PE↗

A note on the top Lyapunov exponent of linear cooperative systems

In a recent paper [Asymptotic of the largest Floquet multiplier for cooperative matrices Annales de la Faculté des Sciences de Toulouse, Tome XXXI, no 4 (2022)] P. Carmona gives an asymptotic formulae for the top Lyapunov exponent of a linear T-periodic cooperative differential equation, in the limit T goes to infinity. This short note discusses and extends this result.

math.DS↗

Large population asymptotics for a multitype stochastic SIS epidemic model in randomly switched environment

We consider an epidemic SIS model described by a multitype birth-and-death process in a randomly switched environment. That is, the infection and cure rates of the process depend on the state of a finite Markov jump process (the environment), whose transitions also depend on the number of infectives. The total size of the population is constant and equal to some K $\in$ N * , and the number of infectives vanishes almost surely in finite time. We prove that, as K $\rightarrow$ $\infty$, the process composed of the proportions of infectives of each type X^K and the state of the environment $Ξ$^K , converges to a piecewise deterministic Markov process (PDMP) given by a system of randomly switched ODEs. The long term behaviour of this PDMP has been previously investigated by Bena{ï}m and Strickler, and depends only on the sign of the top Lyapunov exponent $Λ$ of the linearised PDMP at 0: if $Λ$ < 0, the proportion of infectives in each group converges to zero, while if $Λ$ > 0, the disease becomes endemic. In this paper, we show that the large population asymptotics of X^K also strongly depend on the sign of $Λ$: if negative, then from fixed initial proportions of infectives the disease disappears in a time of order at most log(K), while if positive, the typical extinction time grows at least as a power of K. We prove that in the situation where the origin is accessible for the linearised PDMP, the mean extinction time of X^K is logarithmically equivalent to K^p * , where p * > 0 is fully characterised. We also investigate the quasi-stationary distribution $μ$^K of (X^K , $Ξ$^K) and show that, when $Λ$ < 0, weak limit points of ($μ$^K), K>0 are supported by the extinction set, while when $Λ$ > 0, limit points belong to the (non empty) set of stationary distributions of the limiting PDMP which do not give mass to the extinction set.

math.PR↗