“…√ 5 2 , 2 only the slow diffusion is possible under the condition m > p. In the case of the fast diffusion and superlinear growth in u, v of the right hand sides, the solutions may blow up or vanish in some finite time depending on the initial conditions as illustrated in [11], [40], [41], [46] and the references therein for the simple equation obtained from the first of system (1.1) by letting p = 2, a > 0 constant and all the kernels K i ≡ 0 (observe that in the case when p = q = 2 no restriction on m, n are required, see Remark 2.2). If Ω = R N for such equation we have that the solution blows up for any initial condition in the case when the superlinear growth in u is less than a certain critical exponent, see [46], and the same occurs for doubly degenerate parabolic equations, see [47].…”