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Reaction-Diffusion Processes and Evolution to Harmonic Maps

Jacob Rubinstein, Peter Sternberg, Joseph B. Keller

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Source: Crossref

Published: Dec 1, 1989

DOI: 10.1137/0149104

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Source abstract

Initial-boundary value problems are considered for the reaction-diffusion equation u1=εΔu−ε−1f(u)u_1 = \varepsilon \Delta u - \varepsilon ^{ - 1} f( u ) with x in a domain Ω\Omega in R′′R'' and u in R′′′R'''. First the asymptotic behavior of u is determined for ε\varepsilon small when f(u)=0f( u ) = 0 on a connected manifold M of stable equilibrium points. It is found that a tends rapidly to M, being driven by reaction. Then u evolves slowly by diffusion restricted toM. It tends ultimately to a limit that is a harmonic map of Ω\Omega into M Next, the case where f(u)f( u ) has stable equilibrium points on two manifolds M1M_1 and M2M_2 is treated. In this case a front develops in Ω\Omega , It separates the regions where u is close to M1M_1 , from the regions whereu is close to M2M_2 . For f(u)=Vn(u)f( u ) = V_n ( u ) a boundary layer solution is constructed for u near the front, and the velocity of the front is found to be proportional to the jump in V across it, to leading order in ε\varepsilon . When V(u)V( u ) has the same value on M1M_1 and M2M_2 , this term is zero and the front velocity isε\varepsilon times its mean curvature. The case of a spherically symmetric potential V(∣u∣)V( {| u |} ) and the case M=S1M = S^1 are presented to illustrate the results.

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Reaction-Diffusion Processes and Evolution to Harmonic Maps — Mathematical Frontier Network