“…1 Typical examples to which the theory developed in the paper is applicable are non-linear, stochastic heat equations: ∂u ∂t (t, ξ) = ∆ ξ u(t, ξ) + f (u(t, ξ)) + g(u(t, ξ)) ∂β ∂t , (1.6) u(0, ξ) = x(ξ), ξ ∈ O, u(t, ξ) = 0, t > 0, ξ ∈ ∂O, (1. 7) and strongly damped, non-linear, stochastic wave equations: ∂ 2 u ∂t 2 (t, ξ) = ∆ ξ u(t, ξ) + ρ∆ ξ ∂u ∂t (t, ξ) + f (u(t, ξ)) + g(u(t, ξ)) ∂β ∂t (1.8) u(t, ξ) = 0, t > 0, ξ ∈ ∂O, (1.9) u(0, ξ) = x 0 (ξ), ∂u ∂t (0, ξ) = x 1 (ξ), ξ ∈ O.…”