Volume 2013, Issue 1 436919
Research Article
Open Access

On Standing Wave Solutions for Discrete Nonlinear Schrödinger Equations

Guowei Sun

Corresponding Author

Guowei Sun

Department of Applied Mathematics, Yuncheng University, Yuncheng, Shanxi 044000, China ycu.edu.cn

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First published: 31 July 2013
Citations: 4
Academic Editor: Juan J. Nieto

Abstract

The purpose of this paper is to study a class of discrete nonlinear Schrödinger equations. Under a weak superlinearity condition at infinity instead of the classical Ambrosetti-Rabinowitz condition, the existence of standing waves of the equations is obtained by using the Nehari manifold approach.

1. Introduction

The discrete nonlinear Schrödinger (DNLS) equation was first derived in the context of nonlinear optics by Christodoulides and Joseph [1]; see also [25]. DNLS equation is one of the most important inherently discrete models, having a crucial role in the modeling of a great variety of phenomena, ranging from solid state and condensed matter physics to biology [610]. For example, Davydov [6] studied the equation in molecular biology and Su et al. [10] considered the equation in condensed matter physics. Eilbeck et al. [11] firstly pointed out the universal nature of the discrete nonlinear Schrödinger equation and reported a number of applications.

For the analytical study, many authors studied the existence results of standing wave solutions for DNLS equations. Much of the works concerns the periodic DNLS equations [1214]. Recently, some authors considered the DNLS equations with infinitely growing potential. Zhang and Pankov [15, 16] devoted their efforts to the case of infinitely growing potential and power-like nonlinearity. In all these results, the nonlinearity is supposed to be either positive (self-focusing), or negative (defocusing). Pankov [17] studied the DNLS equatifvons with infinitely growing potential and sign-changing nonlinearity (a mixture of self-focusing and defocusing ones). Pankov and Zhang were concerned with the DNLS equations with infinitely growing potential and saturable nonlinearity in [18].

In this paper, we consider higher-dimensional generalizations of DNLS equation
()
where
()
and σ = ±1. The parameter σ characterizes the focusing properties of the following equation: if σ = 1, the equation is self-focusing, while σ = −1 corresponds to the defocusing equation.
We assume that the nonlinearity f(n, u) is gauge invariant, that is,
()
Then we can consider the special solutions of the form ϕn = eiωtun, for any ω. These solutions are called breather solutions or standing waves, due to their periodic time behavior. Inserting the ansatz of a breather solution into (1), it follows that ϕn satisfies the nonlinear system of algebraic equations
()
We need the following assumptions.
(V1) The discrete potential satisfies
()

where |n| = |n1| + |n2| + ⋯+|nm| is the length of multi-index n.

(f1)  fC(m × , ), and there exists a > 0, p ∈ (2, ) such that
()

(f2)lim|u|→0f(n, u)/u = 0 uniformly for nm.

(f3)  lim|u|→F(n, u)/u2 = + uniformly for nm, where F(n, u) is the  primitive function of f(n, u), that is,
()

  (f4)uf(n, u)/|u| is strictly increasing on (−, 0) and (0, ).

We are concerned with the existence of ground state solutions, that is, solutions corresponding to the least positive critical value of the variational functional. To obtain the existence of ground states, usually besides the growth condition on the nonlinearity and a Nehari type condition, the following classical Ambrosetti-Rabinowitz superlinear condition (see, e.g., [19]) is assumed:
()
It is easy to see that (8) implies that F(n, u) ≥ C | u|μ, for some constant C > 0 and |u | ≥ 1.
In this paper, instead of (8) we assume the super-quadratic condition (f3). It is easy to see that (8) implies (f3). It is well known that many nonlinearities such as
()
do not satisfy (8). A crucial role that (8) plays is to ensure the boundedness of Palais-Smale sequences.

This paper is organized as follows. In Section 2, we establish the variational framework associated with (4). We then present the main results of this paper and compare them with the existing ones. Section 3 is devoted to prove some useful lemmas, and the proof of the main results is completed in Section 4.

2. Preliminaries

In order to apply the critical point theory, we will establish the corresponding variational framework associated with (4).

For some positive integer m, we consider the real sequence spaces
()
Then the following embedding between lp spaces holds:
()
Let
()
which is a self-adjoint operator defined on lp(m) (see [20]).
Define the space
()
Then E is a Hilbert space equipped with the norm
()
Now we consider the variational functional J defined on E by
()
where (·, ·) is the inner product in l2. Then JC1(E, ). And for the derivative of J, we have the following formula:
()
Equation (16) implies that (4) is the corresponding Euler-Lagrange equation for J. Thus, we have reduced the problem of finding a nontrivial solution of (4) to that of seeking a nonzero critical point of the functional J on E.

The following lemma plays an important role in this paper; it was established in [20].

Lemma 1. If V satisfies the condition (V1), then

  • (1)

    for any 2 ≤ p, the embedding map from E into lp(m) is compact,

  • (2)

    the spectrum σ(L) is discrete and consists of simple eigenvalues accumulating to +.

By Lemma 1, we may assume that λ1 is the smallest eigenvalue of L, that is
()

Now we are ready to state the main results.

Theorem 2. Suppose that conditions (V1) and (f1)–(f4) are satisfied. Then one has the following conclusions.

  • (1)

    If σ = −1, ωλ1, (4) has no nontrivial solution.

  • (2)

    If σ = 1, ω < λ1, (4) has a nontrivial ground state solution.

  • (3)

    If σ = 1, ω < λ1, and f(n, u) is odd in u for each nm, (4) has infinitely many pairs of solutions ±u(k) in E.

Remark 3. In [20], the author considered the following DNLS equation:

()
where there exists a positive constant , such that for any nm, . Clearly, (18) corresponds (4) if we let f(n, u) = γnf(u). Therefore, (18) is a special case of (4).

In [20], the nonlinearity fC1() satisfies the following condition:

()
which implies (8). So it is a stronger condition than (f3). Therefore, our results generalize the corresponding ones.

Remark 4. In [16], the authors also considered (18) and assumed that the nonlinearity fC1() satisfies the classical Ambrosetti-Rabinowitz superlinear condition (8). Clearly, it is a stronger condition than (f3).

Since ω < λ1, we may introduce an equivalent norm in E by setting

()
and then the functional J can be rewritten as
()

To prove the multiplicity results, we need the following lemma.

Lemma 5 (see [21].)Let S = {wE : ∥w∥ = 1}. If E is a infinite-dimensional Hilbert space, Φ ∈ C1(S, ) is even and bounded below and satisfies the Palais-Smale condition. Then Φ has infinitely many pairs of critical points.

3. Some Lemmas

In this section, we always assume that σ = 1.

We define the Nehari manifold
()

To prove the main results, we need some lemmas.

Lemma 6. Suppose that conditions (V1) and (f1)–(f4) are satisfied. Then one has

  • (1)

    F(n, u) > 0 and (1/2)f(n, u)u > F(n, u) for all u ≠ 0,

  • (2)

    J(u) > 0, for all u𝒩.

Proof. (1) From (f2) and (f4), it is easy to get that

()
By (f4), we have
()
So (1/2)f(n, u)u > F(n, u) for all u ≠ 0.

(2) For all u𝒩, by (1), we have

()

Lemma 7. Suppose that conditions (V1) and (f1)–(f4) are satisfied, and let Then one has the following.

  • (1)

    I(u) = o(∥u∥) as u → 0.

  • (2)

    sI(su)u/s is strictly increasing for all u ≠ 0 and s > 0.

  • (3)

    I(su)/s2 uniformly for u on the weakly compact subsets of E∖{0}, as s.

Proof. (1) and (2) are easy to be shown from (f2) and (f4), respectively. Next, we verify (3). Let WE∖{0} be weakly compact and let {u(k)} ⊂ W. It suffices to show that if s(k) as k, then so does a subsequence of I(s(k)u(k))/(s(k)) 2. Passing to a subsequence if necessary, u(k)uE∖{0} and for every n, as k.

Since and u(k) ≠ 0, by (f3) and (23), we have

()

Lemma 8. Under the assumptions (V1) and (f1)–(f4), for each wE∖{0}, there exists a unique sw > 0 such that sww𝒩.

Proof. Let g(s) : = J(sw),s > 0. Note that

()
and from (2) of Lemma 7, then there exists a unique sw, such that g(s) > 0 whenever 0 < s < sw, g(s) < 0 whenever s > sw, and g(sw) = J(sww)w = 0. So sww𝒩.

Remark 9. By (1) and (3) of Lemma 7, g(s) > 0 for s > 0 small and g(s) < 0 for s > 0 large. Together with Lemma 8, we have that sw is a unique maximum of g(s) and sww is the unique point on the ray ssw (s > 0) which intersects with 𝒩. That is, u𝒩 is the unique maximum of J on the ray. Therefore, we may define the mapping and m : S𝒩 by setting

()
where S = {uE : ∥u∥ = 1}.

Lemma 10. For each compact subset 𝒱S, there exists a constant C𝒱 such that swC𝒱 for all w𝒱.

Proof. Suppose that, by contradiction, as k. By Lemma 6 and (f3), we have

()
This is a contradiction.

Lemma 11. (1) The mapping is continuous.

(2) The mapping m is a homeomorphism between S and 𝒩, and the inverse of m is given by m−1(u) = u/∥u∥.

Proof. (1) Suppose that wnw ≠ 0. Since for each t > 0, we may assume that wnS for all n. Write . By Lemmas 8 and 10, is bounded, and hence after passing to a subsequence if needed. Since 𝒩 is closed and . Hence by the uniqueness of sw of Lemma 8. (2) This is an immediate consequence of (1).

Lemma 12. J satisfies the Palais-Smale condition on 𝒩.

Proof. Let {u(k)} ⊂ 𝒩 be a sequence such that J(u(k)) ≤ d for some d > 0 and J(u(k)) → 0 as k.

Firstly, we prove that {u(k)} is bounded. In fact, if not, we may assume by contradiction that ∥u(k)∥ → as k. Let v(k) = u(k)/∥u(k)∥. Then there exists a subsequence, still denoted by the same notation, such that v(k)v in  E as k.

Suppose that v = 0. For every s > 0, from Remark 9, we have

()
This is a contradiction if . Therefore, v ≠ 0.

According to Lemma 7(3), we have

()
a contradiction again. Thus, {u(k)} is bounded.

Finally, we show that there exists a convergent subsequence of {u(k)}. Actually, there exists a subsequence, still denoted by the same notation, such that u(k)u. By Lemma 1, for any 2 ≤ q, then

()
Note that
()

The first term (J(u(k)) − J(u), (u(k)u)) → 0 as k because of the weak convergence.

By (f1) and (f2), it is easy to show that for any ε > 0, there exists cε > 0, such that

()
Then,
()
Combining (32) and the boundedness of {u(k)}, the above inequality implies
()
It follows from (33) that u(k)u in E; that is, J satisfies Palais-Smale condition.

The proof is complete.

Now we define the functional and Ψ : S by
()

Lemma 13. (1) , and

()

(2) Ψ ∈ C1(S, ), and

()

(3) {wn} is a Palais-Smale sequence for Ψ if and only if {m(wn)} is a Palais-Smale sequence for J.

(4) w is a critical point of Ψ if and only if m(w) is a nontrivial critical point of J. Moreover, the corresponding values of Ψ and J coincide and inf SΨ = inf 𝒩J.

Proof. (1) Let wE∖{0} and zE. By Remark 9 and the mean value theorem, we obtain

()
where |t| is small enough and τt ∈ (0,1). Similarly,
()
where ηt ∈ (0,1). From the proof of Lemma 11, the function wsw is continuous, combining these two inequalities that
()
Hence the Gâteaux derivative of is bounded linear in z and continuous in w. It follows that is a class of C1 (see [19, Proposition 1.3]).

(2) follows from (1). Note only that since wS,    .

(3) Let {wn} be a Palais-Smale sequence for Ψ, and let un = m(wn) ∈ 𝒩. Since for every wnS we have an orthogonal splitting , using (2) we have

()
Using (2) again, then
()
Therefore,
()
According to Lemma 6, for un𝒩, J(un) > 0, so there exists a constant c > 0 such that J(un) > c. And since , . Together with Lemma 12, . Hence {wn} is a Palais-Smale sequence for Ψ if and only if {un} is a Palais-Smale sequence for J.

(4) By (45), Ψ(w) = 0 if and only if J(m(w)) = 0. The other part is clear.

4. Proof of Main Results

Proof of Theorem 2. (1) If σ = −1, ωλ1, we suppose that (4) has a nontrivial solution uE. Then u is a nonzero critical point of J in E and J(u) = 0. But

()
This is a contradiction.

(2) If σ = 1, ω < λ1. We firstly show that Ψ satisfies the Palais-Smale condition.

Let {w(k)} be a Palais-Smale sequence for Ψ; then {u(k)} is a Palais-Smale sequence for J by Lemma 13(3), where u(k): = m(w(k)) ∈ 𝒩. From Lemma 12, u(k)u after passing to a subsequence and w(k)m−1(u), so Ψ satisfies the Palais-Smale condition.

Let {w(k)} ⊂ S be a minimizing sequence for Ψ. By Ekeland′s variational principle, we may assume that Ψ(w(k)) → 0 as k, so {w(k)} is a Palais-Smale sequence for Ψ. By Palais-Smale condition, w(k)w after passing to a subsequence if needed. Hence w is a minimizer for Ψ and therefore a critical point of Ψ, and then u = m(w) is a critical point of J and is also a minimizer for J by Lemma 13. Therefore, u is a ground state solution of (4).

(3) If σ = 1, ω < λ1, and f(n, u) is odd in u for each nm, then J is even and so is Ψ. Since inf SΨ = inf 𝒩J > 0 and Ψ satisfies the Palais-Smale condition, Ψ has infinitely many pairs of critical points by Lemma 5. It follows that (4) has infinitely many pairs of solutions ±u(k) in E from Lemma 13.

This completes Theorem 2.

Acknowledgments

This work is supported by Program for the National Natural Science Foundation of China (no. 11071283) and Yuncheng University Science Foundation (nos. JY-2011026, JY-2011038, JY-2011039, and JC-2009024).

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