After the book [1] had been published, the theory of random dynamical systems became a convenient technique for the analysis of random and stochastic differential equations. In the framework of this theory, there arises a natural notion of random attractor as a random set attracting the trajectories from −∞ [2]. This notion was generalized in [3] to the multivalued case. In the present paper, we use the theory of random attractors of multivalued random dynamical systems to analyze the qualitative behavior of the evolution equation perturbed by additive white noise:Here the multimapping F does not necessarily satisfy the Lipschitz condition.In Section 1, we refine and extend the results from [3] to problems of the form (1). The conditions obtained will be verified in Section 2.
MULTIVALUED RANDOM DYNAMICAL SYSTEMSbe the set of all nonempty closed (respectively, bounded) subsets of X, let σ(X) be the Borel σ-algebra, let (Ω, Φ, P ) be a probability space, and let θ t : Ω → Ω be a measure-preserving one-parameter transformation group of Ω such that the mapping (t, w) → θ t w is (σ(R) × Φ)-measurable. Definition 1. A mapping G : R + × Ω × X → C(X) is called a multivalued random dynamical system if G is measurable [4] and the following conditions are valid for w ∈ Ω :By [4], if (Y, Φ) is a measurable space and F : Y → C(X), then F is measurable provided that F −1 (C) ∈ Φ for every closed C ⊂ X.A random set D(w) is defined as a measurable mapping D : Ω → C(X).
Definition 2. A compact random set A(w)is referred to as a global random attractor (an attractor in what follows) if the following conditions are satisfied for P -almost all w ∈ Ω :Note that property (A2) characterizes attraction with probability 1 "from −∞" (pullback attraction). If property (A2) takes place, then the dynamics in "forward time" (forward attraction) is described by the following convergence in probability [2]:Suppose that we have an m-semiflow G : R + × X → C(X) describing the dynamics of a deterministic autonomous evolution equation without uniqueness [5]. Let the equation be perturbed by a stochastic additional term depending on the parameter ε ∈ [0, 1]. Let the resulting stochastic equation generate a multivalued random dynamical system G ε with attractor A ε (w). The dependence of the random attractor A ε (w) on the parameter ε is described in the following easy-to-verify assertion.