Abstract

By applying Mountain Pass Theorem in critical point theory, two existence results are obtained for the following asymptotically 𝑝-linear 𝑝-Laplacian discrete system Δ(|Δ𝑢(𝑡1)|𝑝2Δ𝑢(𝑡1))+[𝐾(𝑡,𝑢(𝑡))+𝑊(𝑡,𝑢(𝑡))]=0. The results obtained generalize some known works.

1. Introduction

Consider the periodic solutions of the following ordinary 𝑝-Laplacian discrete system Δ||||Δ𝑢(𝑡1)𝑝2Δ𝑢(𝑡1)+𝐹(𝑡,𝑢(𝑡))=0,(1.1) where Δ is the forward difference operator defined by Δ𝑢(𝑡)=𝑢(𝑡+1)𝑢(𝑡), Δ2𝑢(𝑡)=Δ(Δ𝑢(𝑡)), 𝑝(1,+),𝑡,𝑢𝑁, 𝐹×𝑁,𝐹(𝑡,𝑥) is continuously differentiable in 𝑥 for every 𝑡 and 𝑇-periodic in 𝑡 for all 𝑥𝑁, and 𝐹 satisfies (𝐹) 𝐹(𝑡,𝑥)=𝐾(𝑡,𝑥)+𝑊(𝑡,𝑥), and 𝐾 and 𝑊 are 𝑇-periodic in 𝑡 for all 𝑥𝑁 with 𝑇>1.

Difference equations provide a natural description of many discrete models in real world. Discrete models exist in various fields of science and technology such as statistics, computer science, electrical circuit analysis, biology, neural network, and optimal control; so it is very important to study the solutions of difference equations. For more details about difference equations, we refer the readers to the books [13].

In some recent papers [417], the authors investigated the existence of periodic solutions and subharmonic solutions of difference equations by applying critical point theory. These papers imply that the critical point theory is a useful method to the study of periodic solutions for difference equations. Motivated by the above papers and the paper [18], we will generalize the results of [18] to 𝑝-Laplacian systems (1.1). Here are our main results.

Theorem 1.1. Assume that 𝐹 satisfies (𝐹) and 𝐾 and 𝑊 satisfy the following conditions:
(A1) there exist constants 𝑎1>0 and 𝛾(𝑝1,𝑝] such that 𝐾(𝑡,0)=0,𝐾(𝑡,𝑥)𝑎1|𝑥|𝛾[],(𝑡,𝑥)1,𝑇×𝑁;(1.2)
(A2)  (𝐾(𝑡,𝑥),𝑥)𝑝𝐾(𝑡,𝑥) for all (𝑡,𝑥)[1,𝑇]×𝑁, where [𝑎,𝑏]=[𝑎,𝑏] for every 𝑎,𝑏 with 𝑎𝑏;
(A3)  𝑊(𝑡,0)=0, limsup|𝑥|0(𝑊(𝑡,𝑥)/|𝑥|𝑝)<𝑎1 uniformly for 𝑡[1,𝑇];
(A4) there exists a function 𝑔𝑙1([1,𝑇],) such that (𝑊(𝑡,𝑥),𝑥)𝑝𝑊(𝑡,𝑥)𝑔(𝑡)for[](𝑡,𝑥)1,𝑇×𝑁,(1.3)lim|𝑥|[][];(𝑊(𝑡,𝑥),𝑥)𝑝𝑊(𝑡,𝑥)=+𝑡1,𝑇(1.4)
(A5) there exist constants 𝑎2>0 and 𝑑>0 such that 𝑊(𝑡,𝑥)𝑎2|𝑥|𝑝[]+𝑑,(𝑡,𝑥)1,𝑇×𝑁;(1.5)
(A6) there exists 𝑥0𝑁 such that 𝑇𝑡=1𝐾𝑡,𝑥0𝑊𝑡,𝑥0𝑔(𝑡)𝑝<0.(1.6)
Then problem (1.1) possesses one nontrivial periodic solution.

Corollary 1.2. Assuming that 𝐹 satisfies (𝐹) and that 𝐾 and 𝑊 satisfy (A1)(A4) and
(A7) there exists a function 𝑉𝑙([1,𝑇],) such that lim|𝑥|||𝑊(𝑡,𝑥)𝑉(𝑡)|𝑥|𝑝2𝑥|||𝑥|𝑝1=0uniformlyfor[],𝑡1,𝑇(1.7)𝑇𝑡=1max|𝑥|=1𝑉𝐾(𝑡,𝑥)(𝑡)𝑝<0.(1.8)
Then problem (1.1) possesses one nontrivial periodic solution.

Remark 1.3. As far as we know, similar results of discrete system (1.1) which satisfies (𝐹) and is asymptotically 𝑝-linear at infinity cannot be found in the literature. From this point, our results are new.

2. Preliminaries

Let 𝐸𝑇 be the Sobolev space defined by𝐸𝑇=𝑢𝑁,𝑢(𝑡+𝑇)=𝑢(𝑡),𝑡(2.1) with the norm𝑢=𝑇𝑡=1||||Δ𝑢(𝑡)𝑝+||||𝑢(𝑡)𝑝1/𝑝,𝑢𝐸𝑇,(2.2) where || denote the usual norm in 𝑁. It is easy to see that (𝐸𝑇,) is a finite dimensional Banach space and linear homeomorphic to 𝑁𝑇. As usual, let 𝑢||𝑢||[]=sup(𝑡)𝑡1,𝑇,𝑢𝑙[]1,𝑇,𝑁.(2.3) Since 𝐸𝑇 is finite dimensional Banach space, there exists a positive constant 𝐶0 such that𝑢𝐶0𝑢.(2.4)

For any 𝑢𝐸𝑇, let 1𝜑(𝑢)=𝑝𝑇𝑡=1||||Δ𝑢(𝑡)𝑝+𝑇𝑡=1[].𝐾(𝑡,𝑢(𝑡))𝑊(𝑡,𝑢(𝑡))(2.5) We can compute the Fréchet derivative of (2.5) as 𝜕𝜑(𝑢)||||𝜕𝑢=ΔΔ𝑢(𝑡1)𝑝2[][].Δ𝑢(𝑡1)+𝐾(𝑡,𝑢(𝑡))𝑊(𝑡,𝑢(𝑡)),𝑡1,𝑇(2.6) Hence, 𝑢 is a critical point of 𝜑 on 𝐸𝑇 if and only ifΔ||||Δ𝑢(𝑡1)𝑝2[][]Δ𝑢(𝑡1)+𝐾(𝑡,𝑢(𝑡))𝑊(𝑡,𝑢(𝑡))=0,𝑡1,𝑇,𝑢𝑁.(2.7) So, the critical points of 𝜑 are classical solutions of (1.1). We will use the following lemma to prove our main results.

Lemma 2.1 (see [19]). Let 𝐸 be a real Banach space and 𝜑𝐶1(𝐸,) satisfying the (PS) condition. Suppose 𝜑(0)=0 and (a)there exist constants 𝜌,𝛼>0 such that 𝜑|𝜕𝐵𝜌(0)𝛼;(b)there exists an 𝑒𝐸𝐵𝜌(0) such that 𝜑(𝑒)0.Then 𝜑 possesses a critical value 𝑐𝛼 which can be characterized as 𝑐=infΓmax𝑠[0,1]𝜑((𝑠)), where Γ={𝐶([0,1],𝐸)(0)=0,(1)=𝑒} and 𝐵𝜌(0) is an open ball in 𝐸 of radius 𝜌 centered at 0.
It is well known that a deformation lemma can be proved with the weaker condition (C) replacing the usual (PS) condition. So Lemma 2.1 holds true under condition (C).

3. Proofs of Main Results

Proof of Theorem 1.1. The proof is divided into three steps.
Step 1. The functional 𝜑 satisfies condition (C). Let {𝑢𝑛}𝐸𝑇 satisfying (1+𝑢𝑛)𝜑(𝑢𝑛)0 as 𝑛 and 𝜑(𝑢𝑛) is bounded. Hence, there exists a positive constant 𝐶1 such that ||𝜑𝑢𝑛||𝐶1,𝑢1+𝑛𝜑𝑢𝑛𝐶1.(3.1) We prove {𝑢𝑛} is bounded by contradiction. If {𝑢𝑛} is unbounded, without loss of generality, we can assume that 𝑢𝑛 as 𝑛. Let 𝑧𝑛=𝑢𝑛/𝑢𝑛, then we have 𝑧𝑛=1. Going to a subsequence if necessary, we may assume that 𝑧𝑛𝑧 weakly in 𝐸𝑇 and so 𝑧𝑛𝑧 strongly in 𝑙1([1,𝑇],). It follows from (3.1) and (A2) that (𝑝+1)𝐶1𝑢𝑝𝜑𝑛𝜑𝑢𝑛,𝑢𝑛=𝑇𝑡=1𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛+𝑇𝑡=1𝑝𝐾𝑡,𝑢𝑛𝐾𝑡,𝑢𝑛,𝑢𝑛𝑇𝑡=1𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛.(3.2) From (A1) and (A5), we obtain 𝜑𝑢𝑛=1𝑝𝑇𝑡=1||Δ𝑢𝑛||(𝑡)𝑝+𝑇𝑡=1𝐾𝑡,𝑢𝑛(𝑡)𝑊𝑡,𝑢𝑛1(𝑡)𝑝𝑇𝑡=1||Δ𝑢𝑛||(𝑡)𝑝𝑎2𝑇𝑡=1||𝑢𝑛||(𝑡)𝑝=1𝑑𝑇𝑝𝑢𝑛1𝑝+𝑎2𝑇𝑡=1||𝑢𝑛||(𝑡)𝑝𝑑𝑇.(3.3) Hence, we have 𝜑𝑢𝑛𝑢𝑛𝑝1𝑝1𝑝+𝑎2𝑇𝑡=1||𝑧𝑛||(𝑡)𝑝𝑑𝑇𝑢𝑛𝑝.(3.4) Passing to the limit in the above inequality, by using the fact that 𝜑(𝑢𝑛) is bounded and {𝑧𝑛(𝑡)} converges uniformly to 𝑧(𝑡) on [1,𝑇], we obtain 1𝑝+𝑎2𝑇𝑡=1||||𝑧(𝑡)𝑝1𝑝,(3.5) which implies that 𝑧0. Let Ω[1,𝑇] be the set on which 𝑧0, then the measure of Ω is positive. Moreover, |𝑢𝑛(𝑡)| as 𝑛 for 𝑡Ω. Thus, from (A4), we get 𝑇𝑡=1𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛=Ω𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛+[1,𝑇]Ω𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛Ω𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛+[]1,𝑇Ω𝑔(𝑡).(3.6) It follows from Fatou’s lemma and (A4) that lim𝑇𝑛𝑡=1𝑊𝑡,𝑢𝑛,𝑢𝑛𝑝𝑊𝑡,𝑢𝑛=+,(3.7) which contradicts with (3.2). Therefore, {𝑢𝑛} is bounded in 𝐸𝑇. Hence, there exists a subsequence, still denoted by {𝑢𝑛}, such that 𝑢𝑛𝑢0weaklyin𝐸𝑇.(3.8) Since 𝐸𝑇 is finite dimensional space, we have 𝑢𝑛𝑢0 in 𝐸𝑇. Therefore, the functional 𝜑 satisfies condition (C).Step 2. From (A3) and (A5), there exist constants 0<𝜀<1/𝑝,𝑞>𝑝 and 𝐶2>1/𝑇𝐶𝑝0 such that 𝑊𝑎(𝑡,𝑢)1𝜀|𝑢|𝑝+𝐶2|𝑢|𝑞for𝑢𝑁[].,𝑡1,𝑇(3.9) Let 𝛿=𝑝𝜀𝑞𝑇𝐶2𝐶𝑝01/(𝑞𝑝).(3.10) Then 0<𝛿<1. If 𝑢𝐸𝑇 and 𝑢=𝛿/𝐶0=𝜌, then it follows from (2.4) that |𝑢(𝑡)|𝛿 for 𝑡[1,𝑇]. Set 𝛼=(𝑞𝑝)𝜀𝑞𝜌𝑝.(3.11) Then from (A1), (2.4), (3.9), (3.10), and (3.11), we have1𝜑(𝑢)=𝑝𝑇𝑡=1||||Δ𝑢(𝑡)𝑝+𝑇𝑡=1𝐾(𝑡,𝑢(𝑡))𝑇𝑡=11𝑊(𝑡,𝑢(𝑡))𝑝𝑇𝑡=1||||Δ𝑢(𝑡)𝑝+𝑎1𝑇𝑡=1||𝑢||(𝑡)𝛾𝑎1𝜀𝑇𝑡=1||𝑢||(𝑡)𝑝𝐶2𝑇𝑡=1||𝑢||(𝑡)𝑞1𝑝𝑇𝑡=1||||Δ𝑢(𝑡)𝑝+𝜀𝑇𝑡=1||||𝑢(𝑡)𝑝𝐶2𝑇𝑡=1||||𝑢(𝑡)𝑞𝜀𝑇𝑡=1||||Δ𝑢(𝑡)𝑝+𝑇𝑡=1||||𝑢(𝑡)𝑝𝐶2𝑇𝑢𝑞𝜀𝑢𝑝𝐶2𝑇𝐶𝑞0𝑢𝑞=(𝑞𝑝)𝜀𝑞𝜌𝑝=𝛼𝑢𝐸𝑇with𝑢=𝜌.(3.12)Step 3. Set 𝑓(𝑠)=𝑠𝑝𝑊(𝑡,𝑠𝑥0) for 𝑠>0. Then it follows from (A4) that 𝑓(𝑠)=𝑠𝑝1𝑝𝑊𝑡,𝑠𝑥0+𝑊𝑡,𝑠𝑥0,𝑠𝑥0𝑠𝑝1[]𝑔(𝑡)𝑡1,𝑇,𝑠>0.(3.13) Integrating the above inequality from 1 to 𝜉>1, we have 𝑊𝑡,𝜉𝑥0𝜉𝑝𝑊𝑡,𝑥0+𝑔(𝑡)𝑝(𝜉𝑝[]1)𝑡1,𝑇,𝜉>1.(3.14) From (A2), it is easy to see that 𝐾𝑡,𝜉𝑥0𝜉𝑝𝐾𝑡,𝑥0[]𝑡1,𝑇,𝜉>1.(3.15) From (3.14), (3.15), and (A6), we have 𝜑𝜉𝑥0=𝑇𝑡=1𝐾𝑡,𝜉𝑥0𝑊𝑡,𝜉𝑥0𝜉𝑝𝑇𝑡=1𝐾𝑡,𝑥0𝑊𝑡,𝑥0𝑔(𝑡)𝑝+1𝑝𝑇𝑡=1𝑔(𝑡)0forlargeenough𝜉>1.(3.16) Choose 𝜉1>1 such that 𝑇1/𝑝|𝜉1𝑥0|>𝜌 and 𝜑(𝜉1𝑥0)0. Let 𝑒=𝜉1𝑥0, then 𝑒=𝑇1/𝑝|𝜉1𝑥0|>𝜌 and 𝜑(𝑒)0. It is easy to see that 𝜑(0)=0. Hence, by Lemma 2.1, there exists 𝑢𝐸𝑇 such that 𝜑(𝑢)=𝑐,𝜑(𝑢)=0.(3.17) Then the function 𝑢 is a desired nontrivial 𝑇-periodic solution of (1.1). The proof is complete.

Proof of Corollary 1.2. Let 𝐶3=(1/3𝑇)𝑇𝑡=1[max|𝑥|=1𝐾(𝑡,𝑥)(𝑉(𝑡)/𝑝)]. Then it follows from (A7) that 𝐶3>0 and there exists a positive constant 𝐶4>0 such that ||𝑊(𝑡,𝑥)𝑉(𝑡)|𝑥|𝑝2𝑥||𝐶3|𝑥|𝑝1for[]𝑡1,𝑇,|𝑥|𝐶4.(3.18) For any 𝑥𝑁{0}, let 𝑥=𝐶4𝑥/|𝑥|. Then it follows from (3.18) that for all 𝑡[1,𝑇] and 𝑥𝑁 with |𝑥|>𝐶4𝑉𝑊(𝑡,𝑥)(𝑡)𝑝|𝑥|𝑝=𝑊𝑡,𝑥1𝑝𝑉||𝑥(𝑡)||𝑝+10𝑊𝑡,𝑥+𝑠𝑥𝑥𝑉𝑥(𝑡)+𝑠𝑥𝑥,𝑥𝑥𝑑𝑠𝑊𝑡,𝑥𝐶𝑝4𝑝𝑉(𝑡)+𝐶310||𝑥+𝑠𝑥𝑥||||𝑥𝑥||𝑑𝑠𝑊𝑡,𝑥𝐶𝑝4𝑝𝑉(𝑡)+2𝐶3|𝑥|𝑝,(3.19) which implies that 𝑉𝑊(𝑡,𝑥)(𝑡)𝑝+2𝐶3|𝑥|𝑝+𝑊𝑡,𝑥𝐶𝑝4𝑝𝑉(𝑡)for[]𝑡1,𝑇,|𝑥|>𝐶4,(3.20) which together with (A3) shows that (A5) holds. Similarly, we have 𝑉𝑊(𝑡,𝑥)(𝑡)𝑝2𝐶3|𝑥|𝑝+𝑊𝑡,𝑥𝐶𝑝4𝑝𝑉(𝑡)for[]𝑡1,𝑇,|𝑥|>𝐶4.(3.21) From (A2), it is easy to show that 𝑥𝐾(𝑡,𝑥)𝐾𝑡,|𝑥||𝑥|𝑝for[]𝑡1,𝑇,|𝑥|>1.(3.22) Choose 𝑥0𝑁 such that |𝑥0|>𝐶4+1 and 𝐶3𝑇||𝑥0||𝑝+𝑇𝑡=1min|𝑥|=𝐶4𝑊(𝑡,𝑥)+𝑔(𝑡)𝑝𝐶𝑝4𝑝𝑉(𝑡)>0.(3.23) It follows from (3.21), (3.22), and (3.23) that 𝑇𝑡=1𝐾𝑡,𝑥0𝑊𝑡,𝑥0𝑔(𝑡)𝑝||𝑥0||𝑝𝑇𝑡=1𝐾𝑥𝑡,0||𝑥0||𝑉(𝑡)𝑝+2𝐶3𝑇𝑡=1𝑊𝑡,𝑥+𝑔(𝑡)𝑝𝐶𝑝4𝑝𝑉||𝑥(𝑡)0||𝑝𝑇𝑡=1max|𝑥|=1𝑉𝐾(𝑡,𝑥)(𝑡)𝑝+2𝐶3𝑇𝑡=1min|𝑥|=𝐶4𝑊(𝑡,𝑥)+𝑔(𝑡)𝑝𝐶𝑝4𝑝𝑉(𝑡)𝐶3𝑇||𝑥0||𝑝𝑇𝑡=1min|𝑥|=𝐶4𝑊(𝑡,𝑥)+𝑔(𝑡)𝑝𝐶𝑝4𝑝𝑉(𝑡)<0.(3.24) This implies that (A6) holds. By Theorem 1.1, the conclusion of Corollary 1.2 holds true. The proof is complete.

4. An Example

In this section, we give an example to illustrate our results.

Example 4.1. In problem (1.1), let 𝑝=4/3 and 𝑊(𝑡,𝑥)=𝑎(𝑡)|𝑥|4/311ln(𝑒+|𝑥|),𝐾(𝑡,𝑥)=𝑏|𝑥|𝜃+𝑐(𝑡)|𝑥|𝜎,(4.1) where 𝑏>0,𝑎,𝑐𝑙1(,[0,+)),1<𝜃<𝜎4/3,𝑎(𝑡+𝑇)=𝑎(𝑡),𝑐(𝑡+𝑇)=𝑐(𝑡). It is easy to check that (𝐹), (A1)–(A3), and (A5) hold. On the one hand, we have 4(𝑊(𝑡,𝑥),𝑥)3𝑊(𝑡,𝑥)=(4/3)𝑎(𝑡)|𝑥|7/3(𝑒+|𝑥|)(ln(𝑒+|𝑥|))2.(4.2) Then, it is easy to check that condition (A4) holds. On the other hand, we have 𝑇𝑡=1𝐾(𝑡,𝑥)𝑊(𝑡,𝑥)𝑔(𝑡)𝑝=𝑇𝑡=1𝑏|𝑥|𝜃+𝑐(𝑡)|𝑥|𝜎𝑎(𝑡)|𝑥|4/311ln(𝑒+|𝑥|)𝑔(𝑡)𝑝=𝑏𝑇|𝑥|𝜃+|𝑥|𝜎𝑇𝑡=1𝑐(𝑡)𝑔𝑙1𝑝|𝑥|4/311ln(𝑒+|𝑥|)𝑇𝑡=1𝑎(𝑡),(4.3) which implies that there exists 𝑥0𝑁 such that (A6) holds if 𝑇𝑡=1𝑎(𝑡)>𝑇𝑡=1𝑐(𝑡).(4.4) Hence, from Theorem 1.1, problem (1.1) with 𝑊 and 𝐾 as in (4.1) has one nontrivial 𝑇-periodic solution if (4.4) holds.

Acknowledgment

This work is partially supported by Scientific Research Foundation of Guilin University of Technology and Scientific Research Foundation of Guangxi Education Office of China (200911MS270).