On Standing Wave Solutions for Discrete Nonlinear Schrödinger Equations
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 [2–5]. 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 [6–10]. 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 [12–14]. 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].
where |n| = |n1| + |n2| + ⋯+|nm| is the length of multi-index n.
(f2)lim|u|→0f(n, u)/u = 0 uniformly for n ∈ ℤm.
(f4)u ↦ f(n, u)/|u| is strictly increasing on (−∞, 0) and (0, ∞).
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).
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(ℤm) is compact,
- (2)
the spectrum σ(L) is discrete and consists of simple eigenvalues accumulating to +∞.
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.
Remark 3. In [20], the author considered the following DNLS equation:
In [20], the nonlinearity f ∈ C1(ℝ) satisfies the following condition:
Remark 4. In [16], the authors also considered (18) and assumed that the nonlinearity f ∈ C1(ℝ) 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
To prove the multiplicity results, we need the following lemma.
Lemma 5 (see [21].)Let S = {w ∈ E : ∥w∥ = 1}. If E is a infinite-dimensional Hilbert space, Φ ∈ C1(S, ℝ) 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.
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 u ∈ 𝒩.
Proof. (1) From (f2) and (f4), it is easy to get that
(2) For all u ∈ 𝒩, 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)
s ↦ I′(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 W ⊂ E∖{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)⇀u ∈ E∖{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 w ∈ E∖{0}, there exists a unique sw > 0 such that sww ∈ 𝒩.
Proof. Let g(s) : = J(sw),s > 0. Note that
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 s ↦ sw (s > 0) which intersects with 𝒩. That is, u ∈ 𝒩 is the unique maximum of J on the ray. Therefore, we may define the mapping and m : S → 𝒩 by setting
Lemma 10. For each compact subset 𝒱 ⊂ S, there exists a constant C𝒱 such that sw ≤ C𝒱 for all w ∈ 𝒱.
Proof. Suppose that, by contradiction, as k → ∞. By Lemma 6 and (f3), we have
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 wn → w ≠ 0. Since for each t > 0, we may assume that wn ∈ S 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
According to Lemma 7(3), we have
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
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
The proof is complete.
Lemma 13. (1) , and
(2) Ψ ∈ C1(S, ℝ), 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 w ∈ E∖{0} and z ∈ E. By Remark 9 and the mean value theorem, we obtain
(2) follows from (1). Note only that since w ∈ S, .
(3) Let {wn} be a Palais-Smale sequence for Ψ, and let un = m(wn) ∈ 𝒩. Since for every wn ∈ S we have an orthogonal splitting , using (2) we have
(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, ω ≤ λ1, we suppose that (4) has a nontrivial solution u ∈ E. Then u is a nonzero critical point of J in E and J′(u) = 0. But
(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 n ∈ ℤm, 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).