2008
DOI: 10.1007/bf03167516
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Dynamics of front solutions in a specific reaction-diffusion system in one dimension

Abstract: In this paper, two component reaction-diffusion systems with a specific bistable nonlinearity are concerned. The systems have the bifurcation structure of pitch-fork type of traveling front solutions with opposite velocities, which is rigorously proved and the ordinary differential equations describing the dynamics of such traveling front solutions are also derived explicitly. It enables us to know rigorously precise information on the dynamics of traveling front solutions. As an application of this result, th… Show more

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Cited by 18 publications
(12 citation statements)
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“…The fast reduced system (FRS) of (2.2) is obtained in the limit ε → 0, 6) and (v, q, w, r) = (v * , q * , w * , r * ) constants. It is independent of γ(ξ), therefore, this FRS coincides with the FRS of (2.2) 1 and (2.2) 2 .…”
Section: Existence Of Pinned 1-front Solutionsmentioning
confidence: 99%
See 1 more Smart Citation
“…The fast reduced system (FRS) of (2.2) is obtained in the limit ε → 0, 6) and (v, q, w, r) = (v * , q * , w * , r * ) constants. It is independent of γ(ξ), therefore, this FRS coincides with the FRS of (2.2) 1 and (2.2) 2 .…”
Section: Existence Of Pinned 1-front Solutionsmentioning
confidence: 99%
“…In [9] pinning, rebound and penetration phenomena are studied in a system that is assumed to be close to a drift bifurcation, i.e., the bifurcation at which a traveling front bifurcates from the standing front. The analysis is based on a center manifold approach that has been developed to describe the weak interactions of fronts [6]. From the analytical point of view, the main differences between the present work and [9,10,11] is that (i), we use geometrical singular perturbation theory to explicitly construct the leading order profile of 1-front and 1-pulse, or 2-front, solutions and determine explicit stability conditions (in a three-component model), see Theorems 2.1, 3.1, and 4.1; (ii), our methods enable us to go beyond the setting of weak interactions and thus to consider N -front patterns (N > 1) that interact in a semi-strong fashion [3,22], see also section 5.…”
Section: Introductionmentioning
confidence: 99%
“…[25]). For spatially extended systems on the infinite line, it is then often possible to perform a centre manifold reduction, valid near the Hopf bifurcation point, to develop a weakly nonlinear normal form theory for large-scale oscillatory drift instabilities (see [9], [8] and the references therein). In contrast to this normal form theory, we emphasize that our Stefan problem with moving sources provides a description of large-scale oscillatory drift instabilities for values of τ 0 not necessarily close to the Hopf bifurcation point.…”
Section: In the Subregime O(1)mentioning
confidence: 99%
“…For the analysis, we do not deal with the original PDEs of (1), but with finite-dimensional ODEs that describe the pulse motion. Our study is inspired in part by the work of Ei et al [11] [32]. In [11], they employed the following nonlinearities for f and g of (1):…”
Section: Historical Background To the Present Studymentioning
confidence: 99%
“…Our study is inspired in part by the work of Ei et al [11] [32]. In [11], they employed the following nonlinearities for f and g of (1):…”
Section: Historical Background To the Present Studymentioning
confidence: 99%