Admissible wavefront speeds for a single species reaction-diffusion equation with delay

preprint2006arXivOpen access

Abstract

We consider equation ut(t,x)=Δu(t,x)−u(t,x)+g(u(t−h,x))(∗)u_t(t,x) = Δu(t,x)- u(t,x) + g(u(t-h,x)) (*) , when g:R+→R+g:\R_+\to \R_+ has exactly two fixed points: x1=0x_1= 0 and x2=κ>0x_2=κ>0. Assuming that gg is unimodal and has negative Schwarzian, we indicate explicitly a closed interval C=C(h,g′(0),g′(κ))=[c∗,c∗]\mathcal{C} = \mathcal{C}(h,g'(0),g'(κ)) = [c_*,c^*] such that (∗)(*) has at least one (possibly, nonmonotone) travelling front propagating at velocity cc for every c∈Cc \in \mathcal{C}. Here c∗>0c_*>0 is finite and c∗∈R+∪{+∞}c^* \in \R_+ \cup \{+\infty\}. Every time when C\mathcal{C} is not empty, the minimal bound c∗c_* is sharp so that there are not wavefronts moving with speed c<c∗c < c_*. In contrast to reported results, the interval C\mathcal{C} can be compact, and we conjecture that some of equations (∗)(*) can indeed have an upper bound for propagation speeds of travelling fronts. As particular cases, Eq. (∗)(*) includes the diffusive Nicholson's blowflies equation and the Mackey-Glass equation with nonmonotone nonlinearity.

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