Transition asymptotics for reaction-diffusion in random media

We describe a universal transition mechanism characterizing the passage to an annealed behavior and to a regime where the fluctuations about this behavior are Gaussian, for the long time asymptotics of the empirical average of the expected value of the number of random walks which branch and annihilate on ${\mathbb{Z}}^d$, with stationary random rates. The random walks are independent, continuous time rate $2d\kappa$, simple, symmetric, with $\kappa \ge 0$\mathrm{.}Arandomwalkat$x\in{\mathbb Z}^d$,binarybranchesatrate$v_+(x)$, and annihilates at rate $v_{-}(x)$. The random environment $w$ has coordinates $w(x)=(v_{-}(x),v_{+}(x))$ which are i.i.d. We identify a natural way to describe the annealed-Gaussian transition mechanism under mild conditions on the rates. Indeed, we introduce the exponents $F_{\theta }(t):=\frac{H_1((1+\theta )t)-(1+\theta )H_1(t)}{\theta }$, and assume that $\frac{F_{2\theta }(t)-F_{\theta }(t)}{\theta \log (\kappa t+e)}\to \mathrm{\infty }$ for $\mathrm{\mid }\theta \mathrm{\mid }>0$ small enough, where $H_1(t):=\log <m(0,t)>$ and $<m(0,t)>$ denotes the average of the expected value of the number of particles $m(0,t,w)$ at time $t$ and an environment of rates $w$, given that initially there was only one particle at 0. Then the empirical average of $m(x,t,w)$ over a box of side $L(t)$ has different behaviors: if $ L(t)\ge e^{\frac{1}{d} F_\epsilon(t)}$forsome$\epsilon >0$andlargeenough$t$, a law of large numbers is satisfied; if $L(t)\ge e^{\frac{1}{d}{F}_{ϵ}(2t)}$ for some $ϵ>0$ and large enough $t$, a CLT is satisfied. These statements are violated if the reversed inequalities are satisfied for some negative $ϵ$. Applications to potentials with Weibull, Frechet and double exponential tails are given.