Random Attractors for the Stochastic Discrete Long Wave-Short Wave Resonance Equations
Abstract
We prove the existence of the random attractor for the stochastic discrete long wave-short wave resonance equations in an infinite lattice. We prove the asymptotic compactness of the random dynamical system and obtain the random attractor.
1. Introduction
There has been considerable progress in the study of infinite-dimensinal dynamical systems in the past few decades (see [1–5]). Recently, the dynamics of infinite lattice systems has attracted a great deal of attention from mathematicians and physicists; see [6–11] and the references therein. Various properties of solutions for lattice dynamical systems (LDSs) have been extensively investigated. For example, the long-time behavior of LDSs was studied in [5, 10]. Lattice dynamical systems play an important role in their potential application such as biology, chemical reaction, pattern recognition and image processing, electrical engineering, and laser systems. However, a system in reality is usually affected by external perturbations within many cases that are of great uncertainty or random influence. These random effects are introduced not only to compensate for the defects in some deterministic models but also to explain the intrinsic phenomena. Therefore, there is much work concerning stochastic lattice dynamical systems. The study of random attractors gained considerable attention during the past decades; see [12] for a comprehensive survey. Bates et al. [13] first investigated the existence of global random attractor for a kind of first-order dynamic systems driven by white noise on lattice ℤ; then, Lv and Sun [14] extended the results of Bates to the dimensional lattices. Stochastic complex Ginzburg-Landau equations, FitzHugh-Nagumo equation, and KGS equations in an infinite lattice are studied by Lv and Sun [15], Huang [16], and Yan et al. [17], respectively.
The long wave-short wave (LS) resonance system is an important model in nonlinear science. Long wave-short wave resonance equations arise in the study of the interaction of surface waves with both gravity and capillary modes present and also in the analysis of internal waves as well as Rossby waves as in [18]. In the plasma physics they describe the resonance of the high-frequency electron plasma oscillation and the associated low-frequency ion density perturbation in [19].
This paper is organized as follows. In the next section, we recall some basic concepts and already know results to random dynamical system and random attractors. In Section 3, we prove the existence of the global random attractor for stochastic LS lattice dynamical systems (1.4)–(1.6).
2. Preliminaries
In this section, we first introduce the definitions of the random dynamical systems and random attractor, which are taken from [13]. Let (H, ∥·∥H) be a Hilbert space and (Ω, ℱ, ℙ) a probability space.
Definition 2.1. (Ω, ℱ, ℙ, (θt) t∈ℝ) are called metric dynamical systems; if θ : ℝ × Ω → Ω is (𝔹(ℝ) × ℱ, ℱ)-measurable, θ0 = 𝕀, θt+s = θt∘θs for all t, s ∈ ℝ, and θtℙ = ℙ for all t ∈ ℝ.
Definition 2.2. A stochastic process ϕ(t, ω) is called a continuous random dynamical system (RDS) over (Ω, ℱ, ℙ, (θt) t∈ℝ) if ϕ is (𝔹(ℝ+) × ℱ × 𝔹(H), 𝔹(H))-measurable, and for all ω ∈ Ω
- (i)
the mapping ϕ : ℝ+ × Ω × H → H is continuous;
- (ii)
ϕ(0, ω) = 𝕀 on H;
- (iii)
ϕ(t + s, ω, χ) = ϕ(t, θsω, ϕ(s, ω, χ)) for all t, s ≥ 0 and χ ∈ H (cocycle property).
Definition 2.3. A random bounded set B(ω) ⊂ H is called tempered with respect to (θt) t∈ℝ if for a.e. ω ∈ Ω and all ϵ > 0
Consider a continuous random dynamical system ϕ(t, w) over (Ω, ℱ, ℙ, (θt) t∈ℝ), and let 𝔻 be the collection of all tempered random sets of H.
Definition 2.4. A random set 𝕂(ω) is called an absorbing set in 𝔻 if for all B ∈ 𝔻 and a.e. ω ∈ Ω there exist tB(ω) > 0 such that
Definition 2.5. A random set 𝔸(ω) is a random 𝔻-attractor for RDS ϕ if
- (i)
𝔸(ω) is a random compact set, that is, ω → d(χ, 𝔸(ω)) is measurable for every χ ∈ H and 𝔸(ω) is compact for a.e. ω ∈ Ω;
- (ii)
𝔸(ω) is strictly invariant, that is, ϕ(t, ω, 𝔸(ω)) = 𝔸(θtω), for all t ≥ 0 and for a.e. ω ∈ Ω;
- (iii)
𝔸(ω) attracts all sets in 𝔻, that is, for all B ∈ 𝔻 and a.e. ω ∈ Ω we have
()where d(X, Y) = sup χ∈Xinf y∈Y∥χ−y∥H, X, Y ⊂ H.
The collection 𝔻 is called the domain of attraction of 𝔸.
Definition 2.6. Let ϕ be an RDS on Hilbert space H. ϕ is called asymptotically compact if, for any bounded sequence {χn} ⊂ H and tn → ∞, the set is precompact in H, for any ω ∈ Ω.
From [13], we have the following result.
Proposition 2.7. Let 𝕂 ∈ 𝔻 be an absorbing set for an asymptotically compact continuous RDS ϕ. Then ϕ has a unique global random 𝔻-attractor
Let and , where (an) n∈ℤ, (bn) n∈ℤ ∈ ℓ2. Here {en} denotes the standard complete orthonormal system in ℓ2, which means that the nth component of en is 1 and all other elements are 0. Then W1(·) and W2(·) are ℓ2-valued Q-Wiener processes. It is obvious that EW1(t) = EW2(t) = 0. For details we refer to [24].
Remark 2.8. The special form of multiplicative noise in (2.5) is more suitable than the white noise “adW” and the additive noise “”, because it is more approximative to the perturbations of the short wave for this model.
Let θtω(·) = ω(·+t) − ω(t), t ∈ ℝ. Then (Ω, ℱ, ℙ, (θt) t∈ℝ) is a metric dynamical system with the filtration , where is the smallest σ-algebra generated by the random variable W(t2) − W(t1) for all t1, t2 such that s ≤ t1 ≤ t2 ≤ t; see [12] for more details.
3. The Existence of a Random Attractor
In this section, we study the dynamics of solutions for the stochastic LS (1.4)–(1.6). Then we apply Proposition 2.7 to prove the existence of a global random attractor for stochastic lattice LS equations.
Before proving the existence of global solution for (2.5)-(2.6), we need the following a priori estimate.
Lemma 3.1. Suppose that f(t) = (fn(t)) n∈ℤ ∈ CB(ℝ, ℓ2). Then, the solution of (1.4)–(1.6) satisfies
Proof. We write (1.4) in the form of vector as
By Lemma 3.1, we know that ∥u∥2 is bounded in any bounded subset of [0, ∞), that is, , for any fixed constant T > 0.
Remark 3.2. For the general multiplicative noise, we can also choose a suitable process and a change of variable to convert the stochastic equations into deterministic equations.
For each fixed ω ∈ Ω, (3.8) are deterministic equations, and we have the following result.
Theorem 3.3. For any T > 0, (2.5)-(2.6) are well posed and admit a unique solution (u(t), v(t)) ∈ 𝕃2(Ω; C([0, T]; E)). Moreover, the solution of (2.5)-(2.6) depends continuously on the initial data (u0, v0).
Proof. By standard existence theorem for ODEs, it follows that (3.8) possess a local solution , where [0, Tmax ] is the maximal interval of existence of the solution of (3.8). Now, we prove that this local solution is a global solution. Let ω ∈ Ω; from (3.8) it follows that
By the Young inequality and (1.8), direct computation shows that
Combining the above inequalities with Lemma 3.1, we obtain
Theorem 3.4. System (2.5)-(2.6) generates a continuous random dynamical system (ϕ(t, θ−tω)) t≥0 over (Ω, ℱ, ℙ, (θt) t∈ℝ).
The proof is similar to that of Theorem 3.2 in [13], so we omit it.
- (1)
the mapping t → zi(θtω), i = 1,2, is continuous for each ω ∈ Ω′,
- (2)
the random variables ∥zi(ω)∥, i = 1,2, are tempered.
Lemma 3.5. There exists a θt invariant set Ω′ ⊂ Ω of full ℙ measure and an absorbing random set 𝕂(ω), ω ∈ Ω′, for the random dynamical system (ϕ(t, θ−tω)) t≥0.
Proof. We use the estimates in Theorem 3.3. By (3.11), we have
By the Gronwall inequality, we have
Lemma 3.6. Let (u0, v0) ∈ 𝕂(ω), the absorbing set given in Lemma 3.5. Then, for every ɛ > 0 and ℙ-a.e. ω ∈ Ω, there exist T(ɛ, ω) > 0 and N(ɛ, ω) > 0 such that the solution (u, v) of system (2.5)-(2.6) satisfies
Proof. Let η(x) ∈ C(ℝ+, [0,1]) be a cut-off function satisfying
Taking the inner product of (3.8) with and , respectively, we get
We also use the estimates in Theorem 3.3. Similar to (3.11), it follows that
Replace ω by θ−tω in (3.22). Then, we estimate each term on the right-hand of (3.22); it follows that
Since f(t) ∈ CB(ℝ, ℓ2) and g(t) ∈ CB(ℝ, ℓ2), there exists N2(ɛ, ω) such that for M > N2(ɛ, ω)
Therefore, let
Then, for and , we obtain
Lemma 3.7. The random dynamical systems (ϕ(t, θ−tω)) t≥0 are asymptotically compact.
Proof. We use the method of [25]. Let ω ∈ Ω. Consider a sequence (tn) n∈ℕ with tn → ∞ as n → ∞. Since 𝕂(ω) is a bounded absorbing set, for large n, , where (u0, v0) ∈ 𝕂(ω). Then, there exist (u, v) ∈ E and a sequence (un, vn) (denoted by itself) such that
Next, we show that the above weak convergence is actually strong convergence in E.
From Lemma 3.6, for any ɛ > 0, there exist positive constants N3(ɛ, ω) and such that, for ,
Since (u, v) ∈ E, there exists N4(ɛ, ω) > 0 such that
Let , then, from (3.33), there exists such that, for ,
By (3.34)–(3.36), we obtain that, for ,
Now, combining Lemmas 3.5, 3.7 with Proposition 2.7, we can easily obtain the following result.
Theorem 3.8. The random dynamical systems (ϕ(t, θ−tω)) t≥0 possess a global random attractor in E.
Acknowledgments
The authors are grateful to the anonymous referees for their careful reading of the paper and precious comments. The authors also thank the editors for their kind help. They were supported by the NSF of China (nos. 11071162, 11001116), the NSF of Shandong Province, the Project of Shandong Province Higher Educational Science and Technology Program (nos. J10LA09, J11LA03), and the Project of Discipline Construction Foundation in Ludong University.