We prove that if the initial condition of the Swift-Hohenberg equation $\partial_t u(x,t)=\bigl(\epsilon^2-(1+\partial_ x^2)^2\bigr) u(x,t) -u^3(x,t)$ is bounded in modulus by $Ce^{ -\beta x}$ as $x\to+\infty $, the solution cannot propagate to the right with a speed greater than $\sup_{ 0<\gamma\le\beta}\gamma^{ -1}(\epsilon ^2+4\gamma^2+8\gamma^4).$ This settles a long-standing conjecture about the possible asymptotic propagation speed of the Swift-Hohenberg equation. The proof does not use the maximum principle and is simple enough to generalize easily to other equations. We illustrate this with an example of a modified Ginzburg-Landau equation, where the minimal speed is not determined by the linearization alone.
Categories: nlin.PS math-ph math.MP physics.flu-dyn