2021
DOI: 10.3934/jcd.2021010
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On the influence of cross-diffusion in pattern formation

Abstract: In this paper we consider the Shigesada-Kawasaki-Teramoto (SKT) model to account for stable inhomogeneous steady states exhibiting spatial segregation, which describe a situation of coexistence of two competing species. We provide a deeper understanding on the conditions required on both the cross-diffusion and the reaction coefficients for non-homogeneous steady states to exist, by combining a detailed linearized analysis with advanced numerical bifurcation methods via the continuation software pde2path. We r… Show more

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Cited by 21 publications
(41 citation statements)
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References 51 publications
(87 reference statements)
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“…on a disk domain = {(x 1 , x 2 ) : x = x 2 1 + x 2 2 < R}, where = ∂ 2 x 1 + ∂ 2 x 2 is the Laplacian, with Neumann BCs ∂ n u = ∂ n u = 0, where n is the outer normal at x = R. Equations of type (6) (with various nonlinearities, for instance f (u) = νu 2 − u 3 instead of f (u) = νu 3 − u 5 in (6)) are prototypical examples for finite wave number (Turing) pattern formation, and are thus also studied as model problems in [68], over 1D, 2D and 3D boxes (intervals, rectangles and cuboids). The new feature in [81] is the disk domain.…”
Section: Introductionmentioning
confidence: 99%
“…on a disk domain = {(x 1 , x 2 ) : x = x 2 1 + x 2 2 < R}, where = ∂ 2 x 1 + ∂ 2 x 2 is the Laplacian, with Neumann BCs ∂ n u = ∂ n u = 0, where n is the outer normal at x = R. Equations of type (6) (with various nonlinearities, for instance f (u) = νu 2 − u 3 instead of f (u) = νu 3 − u 5 in (6)) are prototypical examples for finite wave number (Turing) pattern formation, and are thus also studied as model problems in [68], over 1D, 2D and 3D boxes (intervals, rectangles and cuboids). The new feature in [81] is the disk domain.…”
Section: Introductionmentioning
confidence: 99%
“…Here we should refer to a recent numerical result by Breden, Kuehn and Soresina [1], which numerically exhibits the bifurcation diagram of solutions of (1.1) with…”
Section: Resultsmentioning
confidence: 99%
“…and (5.22) that µ j (d) > 0 for any j ∈ N if d > d (1) . Then, for any d > d (1) , the number σ(d) of negative eigenvalues of I − L(d) is equal to that of negatives of Assume that C < A < B in addition to (3.6). We shall show that (3.2) admits at least one nonconstant solution when d ∈ (d (j+1) , d (j) ) ∩ [ε, ∞) and j is odd.…”
Section: Existence Of Nonconstant Solutions For the Full Cross-diffusion Limitmentioning
confidence: 99%
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