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Non-linear noise excitation and intermittency under high disorder

Consider the semilinear heat equation $\partial_t u = \partial^2_x u + λσ(u)ξ$ on the interval $[0\,,1]$ with Dirichlet zero boundary condition and a nice non-random initial function, where the forcing $ξ$ is space-time white noise and $λ>0$ denotes the level of the noise. We show that, when the solution is intermittent [that is, when $\inf_z|σ(z)/z|>0$], the expected $L^2$-energy of the solution grows at least as $\exp\{cλ^2\}$ and at most as $\exp\{cλ^4\}$ as $λ\to\infty$. In the case that the Dirichlet boundary condition is replaced by a Neumann boundary condition, we prove that the $L^2$-energy of the solution is in fact of sharp exponential order $\exp\{cλ^4\}$. We show also that, for a large family of one-dimensional randomly-forced wave equations, the energy of the solution grows as $\exp\{cλ\}$ as $λ\to\infty$. Thus, we observe the surprising result that the stochastic wave equation is, quite typically, significantly less noise-excitable than its parabolic counterparts.