Rotating Spirals in segregated reaction-diffusion systems

Abstract

We give a complete characterization of the boundary traces ${\phi }_i$ ($i=1,\dots ,K$) supporting spiraling waves, rotating with a given angular speed $\omega$, which appear as singular limits of competition-diffusion systems of the type \[ \frac{\partial}{\partial t} u_i -Δu_i = μu_i -βu_i \sum_{j \neq i} a_{ij} u_j \text{ in } Ω\times\mathbb{R}^+, \qquad u_i = φ_i \text{ on $\partial \Omega \times {\mathbb{R}}^{+}$}, \qquad u_i(\mathbf{x},0) = u_{i,0}(\mathbf{x}) \text{ for $\mathbf{x}\in \Omega$} \] as $\beta \to +\infty$. Here $\Omega$ is a rotationally invariant planar set and $a_{ij}>0$ for every $i$ and $j$. We tackle also the homogeneous Dirichlet and Neumann boundary conditions, as well as entire solutions in the plane. As a byproduct of our analysis we detect explicit families of eternal, entire solutions of the pure heat equation, parameterized by $\omega \in \mathbb{R}$, which reduce to homogeneous harmonic polynomials for $\omega =0$.

References in corpus (3)

• Spiraling asymptotic profiles of competition-diffusion systems
• A spiral interface with positive Alt-Caffarelli-Friedman limit at the origin
• On the limit configuration of four species strongly competing systems