Uniform Attractor for the Fractional Nonautonomous Long-Short Wave Equations
Abstract
We firstly proved the existence and the uniqueness of the solution for the 2π-periodic fractional nonautonomous long-short wave equations with translation compact force by using Galerkin method and then obtained the compact uniform attractor of the system.
1. Introduction
We all know that the long-short wave resonance equations play an important role in fluid mechanics and have rich physical and mathematical properties. There are more and more resent papers treating the long-short wave resonance equations. Guo studied the global solution for one class of the system of LS nonlinear wave interaction in [1] and the periodic initial value problems and initial value problems for one class of generalized long-short type equations in [2]. The papers [3–5] studied the existence of a global attractor of it. Cui et al. developed the weakly compact uniform attractor for the nonautonomous long-short wave equations with translation compact forces in [6].
The Schrödinger type equation has been of great importance describing nonrelativistic quantum mechanical behavior. It is well known that Feynman and Hibbs derive the standard (nonfractional) Schrödinger type equation by applying path integrals over Brownian paths in [7]. Recently Laskin generalized the Schrödinger equation to space fractional cases using path integrals over Lévy trajectories in [8, 9]. In [10], the authors discussed the models and numerical methods of the fractional calculus. The fractional Schrödinger type equation is used to describe better physical phenomenon and has attracted more and more attention of researchers. Guo and Xu studied some applications of the Schrödinger equation in physics (see [11]). In [12], the authors obtained the approximate analytical solutions of the fractional nonlinear Schrödinger equations by using the homotopy perturbation method. Eid et al. studied the α-dimensional fractional Schrödinger equation and obtained its exact solutions in [13]. Guo et al. investigated the fractional nonlinear Schrödinger equation and showed the existence and uniqueness of its global smooth solution by using energy method in [14]. Goubet [15] studied regularity of the attractor for a weakly damped nonlinear Schrödinger equation in .
The rest of this paper is arranged as follows. In Section 2, we recall some basic definitions, introduce preparation results, and analyse some fractional calculation laws which depend heavily on 2π-period. In Section 3, we introduce some preparation lemma and give the uniform a priori estimates (uniform in initial data and symbol in the symbol space and large time). In Section 4, we show the existence and uniqueness of the solution of the system. In Section 5, we prove the existence of strong compact uniform attractor of the system.
Through the paper, we denote the norm of with the usual inner product (·, ·) by ∥·∥. We denote the norm of for all 1 < p ⩽ ∞ by . For simplicity and convenience, the letter C represents a constant, which may be different from one to others. C(·, ·) represents the constant C expressed by the parameters appearing in the parentheses.
2. Preliminaries
In this section, we introduce notations definition and preliminary facts. We firstly recall the following known definitions (see [6, 16–18]) and some main lemmas (see [16, 19, 20]).
Definition 1. Suppose X is a Banach space, is a function, and T(·) is the translation operator. The hull of f is defined by
- (i)
f is said to be translation bounded in if is bounded in which
()Then consists of all the translation bounded functions in . - (ii)
f is called translation compact in if is compact in , where the convergence is taken in the sense of local quadratic mean convergence topology of . The collection of all the translation compact functions in is denoted by .
Let (X, ∥·∥X) be a Banach space, and the following definitions are common.
Definition 2. Let Σ be a parameter set. , σ ∈ Σ is said to be a family of processes in X, if, for each σ ∈ Σ, Uσ(t, τ) is a process; that is, the two-parameter mapping Uσ(t, τ) from X to X satisfies
- (i)
,
- (ii)
,
Definition 3. A closed set is called the uniform attractor of the family of processes {Uσ(t, τ)} σ∈Σ if it is uniformly attracting (attracting property) and it is contained in any closed uniformly attracting set of the family of processes (minimality property).
Definition 4. {Uσ∈Σ(t, τ)}, a family of processes in X, is said to be (X × Σ, X)-continuous, if, for any fixed T and τ, T⩾τ, projection (uτ, σ) → Uσ(T, τ)uτ is continuous from X × Σ to X.
Definition 5. The space Lp(0, T; X) denotes all measurable functions f : [0, T] → X with the norm
Lemma 6. Let ∑ be a compact metric space and suppose {T(h)∣h⩾0} is a family of operators defined on ∑ , satisfying
- (i)
()
- (ii)
translation identity:
()
Remark 7. Assumption (11) holds if the system has a unique solution.
Lemma 8. Let (X, ∥·∥X) be a uniform convex Banach space (particularly, a Hilbert space), and let be a sequence in X. If xk⇀x0 and ∥xk∥X → ∥x0∥X, then xk → x0.
Lemma 9. Let be a sequence in B* space X. If xk⇀x0, then
Since the solution u(x, t), if it exists, is a 2π-periodic function, we have the Fourier expansion:
For brevity, we introduce W(x, t) = (u(x, t), n(x, t)) and Y(x, t) = (f(x, t), g(x, t)). We denote the space of functions W(x, t) = (u(x, t), n(x, t)) by with norm
Assumption 10. Suppose that the symbol Y(x, t) belongs to the symbol space ∑ , defined by
Remark 11. Due to the conception of translation compact/boundedness, we remark that
- (i)
∀Y1 ∈ ∑ , ;
- (ii)
, where T(t)φ(s) = φ(s + t) is a translation operator.
3. A Uniform A Priori Estimates
In this section, we will get some uniform a priori estimates which hold uniformly independently of initial data, time, and symbols in symbol space (Y ∈ Σ). In the following, we denote that ∫ · dx = ∫Ω · dx and H = L2(Ω), which will not cause any confusions.
We first recall the Gagliardo-Nirenberg and the Young inequalities (see [21]).
Lemma 12. Let . Then for 0 ⩽ j ⩽ m, j/m ⩽ a ⩽ 1, there exists a constant C such that
Lemma 13. Let a, b > 0. Then for each (p, q) satisfying 1 < p, q < ∞, 1/p + 1/q = 1, it holds that
Lemma 14. Assume that
Then there exist positive constants and such that
Proof. Taking the inner product of (1) with u, we have
Lemma 15. Assume that
Then there exist positive constants and such that
Proof. Taking the inner product of (1) with ut, we have
By (48),(53), and (55), we get
Lemma 16. Assume that
Then there exist positive constants and such that
Proof. Taking the inner product of (1) with (−Δ) αut, we have
4. Unique Existence of the Solution
In this section, we show the unique existence theorem of the solutions. Since uniform a priori estimates have been established in the above section, one can readily get the existence of the solution by ’s method (see [20, 22–24]). We show the theorem and prove it briefly for readers’ convenience.
Theorem 17. Set α⩾1, and Y(x, t) satisfy Assumption 10; for each Wτ ∈ E0, then system (1)–(4) has a unique global solution W(x, t) ∈ L∞(τ, T; E0), ∀T > τ.
Proof. We prove this theorem by two steps.
Step 1. The existence of solution.
By ’s method, we construct the approximate solution of the periodic initial value problem (1)~(4). We apply the following approximate solution:
Step 2. The uniqueness of solution.
Suppose W1(x, t) = (u1(x, t), n1(x, t)), W2(x, t) = (u2(x, t), n2(x, t)) are two solutions of problem (1)–(4). Let W(x, t) = W1(x, t) − W2(x, t), and then W(x, t) = (u(x, t), n(x, t)) satisfies
Taking the inner product of (74) with u and taking the imaginary part, we can get
5. Uniform Absorbing Set and Uniform Attractor
In this section, we will prove the existence of the strong compact uniform attractor of problem (1)~(4) applying Ball et al.’s idea (see [19, 22]). Firstly, we construct a bounded uniformly absorbing set. Next, we show the weak uniform attractor of the system. Lastly, we derive that the weak uniform attractor is actually the strong one.
Theorem 18. Under assumptions of Theorem 17, {Uσ∈∑ (t, τ)} admits a strong compact uniform attractor .
Proof. We prove this theorem by three steps.
Step 1. {Uσ∈∑ (t, τ)} possess a bounded uniformly absorbing set in E0.
Let . By Theorem 17, B0 is a bounded absorbing set of the process .
By Assumption 10, we know that, for each Y ∈ ∑ , holds. So the solution of (1)~(4) satisfies
Step 2. we prove the existence of weakly compact uniform attractor in E0.
From Lemma 6, Theorem 17, and Step 1, we only need to prove that {Uσ∈∑ (t, τ)} is (E0 × ∑ , E0)-continuous. We denote weak convergence by ⇀ and * weak convergence by .
For any fixed , let
Next, we will obtain that is a solution of problem (1)~(4).
For , by (91) we have that
For any with ψ(T) = 0, ψ(τ) = 1, by (91) we find that
Step 3. We show the weakly compact uniform attractor is actually the strong one.
From the proof of Lemma 16, we know each solution trajectory for problem (1)–(4) satisfies
From Step 2, we can see that the point if and only if there exist two sequences and such that for all σ(t) ∈ Σ, it uniformly satisfies that
Since , we can see the solution (w, m) as at h corresponding to the initial data (v, p) and the symbol σ*. Similarly to (122), we have
Conflict of Interests
The authors declare that they have no conflict of interests regarding the publication of this paper.
Acknowledgments
This work was supported by the NSF of China (nos. 11371183 and 11271050) and the NSF of Shandong Province (no. ZR2013AM004).