2009
DOI: 10.1016/j.jde.2008.12.005
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Entire solutions of reaction–advection–diffusion equations with bistable nonlinearity in cylinders

Abstract: This paper deals with entire solutions and the interaction of traveling wave fronts of bistable reaction-advection-diffusion equation with infinite cylinders. Assume that the equation admits three equilibria: two stable equilibria 0 and 1, and an unstable equilibrium θ . It is well known that there are different wave fronts connecting any two of those three equilibria. By considering a combination of any two of those different traveling wave fronts and constructing appropriate subsolutions and supersolutions, … Show more

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Cited by 24 publications
(8 citation statements)
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“…These solutions can not only describe the interaction of traveling waves but also characterize new dynamics of diffusion equations. For the study of such entire solutions, we refer to [4,[14][15][16]19,23,27] for reaction-diffusion equations without delay, [22,35,37,42] for reaction-diffusion equations with nonlocal delay, [38,39] for delayed lattice differential equations with nonlocal interaction, [21,34] for nonlocal dispersal equations without delay ((1.9) below), [28,40,44] for reaction-diffusion systems, and [43] for periodic lattice dynamical systems. However, to the best of our knowledge, the issues on entire solutions for nonlocal dispersal equations with spatio-temporal delay have not been addressed, especially for infinite delay equations.…”
Section: Introductionmentioning
confidence: 99%
“…These solutions can not only describe the interaction of traveling waves but also characterize new dynamics of diffusion equations. For the study of such entire solutions, we refer to [4,[14][15][16]19,23,27] for reaction-diffusion equations without delay, [22,35,37,42] for reaction-diffusion equations with nonlocal delay, [38,39] for delayed lattice differential equations with nonlocal interaction, [21,34] for nonlocal dispersal equations without delay ((1.9) below), [28,40,44] for reaction-diffusion systems, and [43] for periodic lattice dynamical systems. However, to the best of our knowledge, the issues on entire solutions for nonlocal dispersal equations with spatio-temporal delay have not been addressed, especially for infinite delay equations.…”
Section: Introductionmentioning
confidence: 99%
“…By using a similar argument to that of [19, Proofs of Theorems 1.3 and 1.4], the problem (3.9) is well posed and the maximum principle holds (see also [8,22]). Let u n (t, x, y) denote the unique classical solution of (3.9) that satisfies 0 < u n (t, x, y) < 1 for any (t, x, y) ∈ [−n, −T ) ×Σ and n > T (n ∈ N).…”
Section: Existence Of Entire Solutionsmentioning
confidence: 98%
“…In our previous paper [22], an amazingly rich class of entire solutions is obtained for the bistable nonlinearity, by splicing the traveling fronts which connect 0 and α, α and 1, and 0 and 1, respectively. However, the global uniqueness and the stability of such an entire solution under the heterogeneous bistable assumption remain open.…”
Section: Introductionmentioning
confidence: 99%
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“…Recently, many types of front-like entire solutions have been observed for various evolution equations by mixing the traveling wave solutions and some spatially independent solutions, see [11][12][13][15][16][17]20,21,25,[27][28][29][30][31][32][33]. For examples, Hamel and Nadirashvili [12] established three-, four-and five-dimensional manifolds of entire solutions for the Fisher-KPP equation.…”
Section: Introductionmentioning
confidence: 99%