Volume 2013, Issue 1 256324
Research Article
Open Access

Existence of Nontrivial Solutions and High Energy Solutions for a Class of Quasilinear Schrödinger Equations via the Dual-Perturbation Method

Yu Chen

Yu Chen

Department of Mathematics, Honghe University, Mengzi, Yunnan 661100, China uoh.edu.cn

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Xian Wu

Corresponding Author

Xian Wu

Department of Mathematics, Yunnan Normal University, Kunming, Yunnan 650092, China ynnu.edu.cn

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First published: 29 October 2013
Citations: 5
Academic Editor: Mihai Mihǎilescu

Abstract

We study the quasilinear Schrödinger equation of the form −Δu + V(x)u − Δ(u2)u = h(x, u), xRN. Under appropriate assumptions on V(x) and h(x, u), existence results of nontrivial solutions and high energy solutions are obtained by the dual-perturbation method.

1. Introduction and Preliminaries

In this paper we consider the quasilinear Schrödinger equation of the form
()
where hC(RN × R, R) and VC(RN, R). Solutions of (1) are standing waves of the following quasilinear Schrödinger equation:
()
where V(x) is a given potential, k is a real constant, and α and g are real functions. The quasilinear Schrödinger equations (2) are derived as models of several physical phenomena; for example, see [15]. Several methods can be used to solve (1). For instance, the existence of a positive ground state solution has been proved in [6, 7] by using a constrained minimization argument; the problem is transformed to a semilinear one in [811] by a change of variables (dual approach); Nehari method is used to get the existence results of ground state solutions in [12, 13].

Recently, some new methods have been applied to these equations. In [14], the authors prove that the critical points are L functions by the Moser’s iteration; then the existence of multibump type solutions is constructed for this class of quasilinear Schrödinger equations. In [15], by analysing the behavior of the solutions for subcritical case, the authors pass to the limit as the exponent approaches to the critical exponent in order to establish the existence of both one-sign and nodal ground state solutions. Another new method which works for these equations is perturbations. In [16] 4-Laplacian perturbations are led into these equations; then high energy solutions are obtained on bounded smooth domain.

In this paper, the perturbation, combined with dual approach, is applied to search the existence of nontrivial solution and sequence of high energy solutions of (1) on the whole space RN. For simplicity we call this method the dual-perturbation method.

We need the following several notations. Let be the collection of smooth functions with compact support. Let
()
with the inner product
()
and the norm
()
Let the following assumption (V) hold:
  • (V) VC(RN, R) satisfies and lim |x|→V(x) = +.

Set
()
with the inner product
()
and the norm
()
Then both H1(RN) and E are Hilbert spaces.
By the continuity of the embedding  ELs(N) for s ∈ [2, 2*] we know that, for each s ∈ [2, 2*], there exists constant as > 0 such that
()
where ∥·∥s denotes the Ls-norm. In the following, we use C or Ci to denote various positive constants. Moreover, we need the following assumptions:
  • (h1) there exist  4 < p < 2(2*) if N ≥ 3 and 4 < p < if N = 2 such that

    ()

  • (h2) lim s→0h(x, s)/s = 0 uniformly in xRN,

  • (h3) there exist μ > 4 and r > 0 such that

    ()

for all xRN and |s | ≥ r, where .

By Lemma 3.4 in [17] we know that, under the assumption (V), the embedding ELs(RN) is compact for each 2 ≤ s < 2*.

Equation (1) is the Euler-Lagrange equation of the energy functional
()
where . Due to the presence of the term , J(u) is not well defined in E. To overcome this difficulty, a dual approach is used in [9, 10]. Following the idea from these papers, let f be defined by
()
on [0, +), f(0) = 0 and f(−t) = −f(t) on (−, 0]. Then f has the following properties:
  • (f1) f is uniquely defined C function and invertible;

  • (f2) 0 < f(t) ≤ 1 for all tR;

  • (f3) |f(t)|≤|t| for all tR;

  • (f4) lim t→0f(t)/t = 1;

  • (f5) , ;

  • (f6) (1/2)f(t) ≤ tf(t) ≤ f(t) for all t ≥ 0 and f(t) ≤ tf(t)≤(1/2)f(t) for all t ≤ 0;

  • (f7) for all tR;

  • (f8) the function f2(t) is strictly convex;

  • (f9) there exists a positive C such that

    ()

  •   (f10) there exist positive constants C1 and C2 such that

    ()
    for all tR;

  • (f11) for all tR;

  • (f12) for each ξ > 0, there exists C(ξ) > 0 such that f2(ξt) ≤ C(ξ)f2(t).

The properties (f1)–(f11) have been proved in [811]. It suffices to prove (f12).

Indeed, by (f1), (f4), and (f5), there exist δ > 0 and M > 0 such that, for |t | ≤ δ,
()
and for |t | ≥ M,
()
Since there exists a C0 > 0 such that f2(2t) ≤ C0f2(t) (see [10]), we can assume that 0 < ξ < 1. For |t | ≤ δ, we have |ξt | ≤ δ, and hence
()
for |t | ≥ M/ξ > M, one has |ξt | ≥ M, and hence
()
and for δ≤|t | ≤ M/ξ, there exist m(ξ) > 0 and M(ξ) > 0 such that f2(ξt) ≤ M(ξ) and f2(t) ≥ m(ξ). Then we have
()
Hence f2(ξt) ≤ C(ξ)f2(t), where C(ξ) = max {3ξ2, M(ξ)/m(ξ)}.
After the change of variable, J(u) can be reduced to
()
From [8, 9, 11] we know that if vE is a critical point of I, that is,
()
for all φE, then u : = f(v) is a weak solution of (1). Particularly, if vH1(RN)∩C2(RN) is a critical point of I, then u : = f(v) is a classical solution of (1).

A sequence {un} ⊂ E is called a Cerami sequence of J if {J(un)} is bounded and (1 + ∥un∥)J(un) → 0 in E*. We say that J satisfies the Cerami condition if every Cerami sequence possesses a convergent subsequence.

2. Some Lemmas

Consider the following perturbation functional Iθ defined by
()
where θ ∈ (0,1]. We have the following lemmas.

Lemma 1. If assumptions (V), (h1), and (h2) hold, then the functional Iθ is well defined on E and IθC1(E, R).

Proof. By conditions (h1) and (h2), the properties (f2), (f3), (f7), and (f11) imply that there exists δ > 0 such that

()
Hence
()
()
for all vR. By (26) and the continuity of the embedding ELs(RN) (s ∈ [2, 2*]),
()
Hence Iθ is well defined in E.

Now, we prove that IθC1(E, R). It suffices to prove that

()

For any v, ϕE and 0<|t | < 1, by the mean value theorem, (25) and (f2)-(f3), we have

()
The Hölder inequality implies that
()
Hence, by the Lebesgue theorem, we have
()
for all ϕE. Now, we show that , i = 1,2, are continuous. Indeed, if vnv in E, then vnv in Ls(RN) for all s ∈ [2, 2*].

On the space , we define the norm

()
Then
()
Moreover, on the space , we define the norm
()
By (25), we have
()
where q = p/2 and r = p/(p − 2). Then Theorem A.4 in [18] implies
()
as n → +. If h(x, f(vn))f(vn) − h(x, f(v))f(v) = yn + zn with ynL2(RN) and znLr(RN), one has
()
Hence
()
and hence
()
as n. Therefore, Ψ1C1(E, R).

Define

()
with the norm . On the space , we define the norm
()
On the space , we define the norm
()
From vnv in E, one has and
()
as n. Since |f(v)f(v)|≤|v|, by the following Lemma 2, we have
()
If f(vn)f(vn) − f(v)f(v) = yn + zn with and , one has
()
Hence
()
and hence
()
as n. Therefore, Ψ2C1(E, R). This completes the proof.

Lemma 2. Assume that 1 ≤ p, q, r, s < +, gC(RN × R) and

()
Then, for every , , and the operator
()
is continuous.

Proof. Let η(s) be a smooth cut-off function such that η(s) = 1 for |s | ≤ 1 and η(s) = 0 for |s | ≥ 2. Define

()
We can assume that p/rq/s. Hence
()
for all (x, v) ∈ RN × R. Assume vnv in . Then vnv in and g(·, vn) → g(·, v) in . As in the proof of Lemma A.1 in [18], there exists a subsequence {wn} of {vn} and such that wn(x) → v(x) and |v(x)|, |wn(x)| ≤ α(x) for a.e. xRN. Hence, from (51), one has
()
a.e. on RN. It follows from the Lebesgue theorem that g1(·, wn) → g1(·, v) in . Consequently, g1(·, vn) → g1(·, v) in . Similarly, we can prove g2(·, vn) → g2(·, v) in . Since
()
it follows that g(·, vn) → g(·, v) in . This completes the proof.

Lemma 3. Let (V), (h1), and (h2) hold. Then every bounded sequence {vn} ⊂ E with possesses a convergent subsequence.

Proof. Since {vn} ⊂ E is bounded, then, by the compactness of the embedding ELs(RN) (2 ≤ s < 2*), passing to a subsequence, one has vnv in E, vnv in Ls(RN) for all 2 ≤ s < 2*, and vn(x) → v(x) for a.e. xRN. By (25)

()
as n. Similarly, as n. Hence, by the property of (f8), we have
()
where on(1) → 0 as n. This shows that as n. This completes the proof.

The following Lemma 4 has been proved in [10] (see Proposition 2.1(3) in [10]).

Lemma 4. If vn(x) → v(x) a.e. in RN and , then as n.

3. Main Results

Theorem 5. Assume conditions (V), (h1)–(h3) hold. Let {θn}⊂(0,1] be such that θn → 0. Let vnE be a critical point of with for some constant c independent of n. Then, up to subsequence, one has vnv in E, and v is a critical point of I.

Proof. By (h2), for 0 < ε0 < (1/4)(1/2 − 1/μ)a0, there exists δ0 > 0 such that

()
By (h1), for δ0≤|s | ≤ r (r is the constant appearing in condition (h3)), we have
()
where C is the constant appearing in condition (h1). Hence
()
Since lim |x|→V(x) = +, there exists ρ0 > 0 such that
()
for all |x | ≥ ρ0. Hence
()
Since vn is a critical point of ,
()
for all ϕE. Consequently, taking ϕ = f(vn)/f(vn) ∈ E, by (h3) and (f6) we have
()
and hence
()
for some constant C independent of n. By the boundedness of , there exists C2 > 0 such that
()
for all n. Hence, by the Sobolev embedding theorem, one has
()

Next, we prove that f(vn) ∈ L(RN) and , where the positive constant C is independent of n. Setting T > 2, r > 0, define , where b : RR is a smooth function satisfying b(s) = s for |s | ≤ T − 1, b(−s) = −b(s); b(s) = 0 for sT, and b(s) is decreasing in [T − 1, T].

This means that , for |vn | ≤ T − 1; , for T − 1≤|vn | ≤ T; , for |vn | ≥ T, where T − 1 ≤ CTT.

Let ; then ϕE. By (61) 〈I(vn), ϕ〉 = 0. Hence

()
where
()
()
For T − 1≤|vn | ≤ T, . By the properties of f and b, the mean value theorem implies
()
Hence
()
Consequently,
()
Combining (67) and (68), we have
()
For any ε > 0, by (h1) and (h2), there exists C(ε) > 0 such that
()
Combining (66), (72), and (73), one has
()
By the Hölder inequality and (65),
()
Moreover,
()
Hence
()
Since 4 < p < 2(2*), d = 2*/(8N/(4N − (p − 4)(N − 2))) = 2*/2 − p/4 + 1 > 1. Set q = 8N/(4N − (p − 4)(N − 2)). Then
()
Take r = r0 such that (2 + r0)q = 2(2*). Since , . Hence, from (65), we have
()
Since as T → +, taking T → + in (78) with r = r0, we have
()
Set 2 + r1 = (2 + r0)d. Then
()
Inductively, we have
()
where (2 + ri) = di(2 + r0)  (i = 0,1, …, k), and
()
is convergent as k. Let . Then CkC > 0 as k. Hence
()
Let k; by (65), we have
()
Hence, by (f9) and (85), we have
()
By (63) we know that is bounded, and hence {vn} is bounded in E. Up to subsequence, one has vnv in E, vnv in Ls(RN) for s ∈ [2, 2*), and vn(x) → v(x) a.e. xRN.

Now, we show that v is a critical point of I. For any with ψ ≥ 0, by (85), we know that ϕ = ψexp (−f(vn)) ∈ E. Take ϕ = ψexp (−f(vn)) as the test function in (61); we have

()
By |∇(vnv)|2ψexp (−f(vn))f(vn) ≥ 0, one has
()
Since θn → 0, by (63)
()
as n. Moreover, notice that vnv in E, vnv in Ls(RN) for s ∈ [2, 2*), and vn(x) → v(x) a.e. xRN; by Hölder inequality and Lebesgue theorem, we have
()
Hence, from (87), we have
()
For any φE with φ ≥ 0, by (85) we know that ζ : = φexp (f(v)) ∈ E. By Theorem 2.8 in [19], there exists a sequence such that ψn ≥ 0 and ψnζ and ψn(x) → ζ(x) for a.e. xRN. Take ψ = ψn in (91), and let n; we have
()
The opposite inequality can be obtained by taking ϕ = ψexp (f(vn)) and ζ = φexp (−f(v)). Consequently,
()
This shows that vE is a critical point of I, and by taking φ = f(v)/f(v) ∈ E, one has
()

Finally, taking ϕ = f(vn)/f(vn) as the test function in (61), we have

()
Since
()
by Fatou’s Lemma, (63), (94), (95), up to subsequence, one has
()
()
Hence as n. Set wn : = vnvE. By (f8), (f12), and (85), one has
()
Consequently, by (f9), (98), and Lemma 4, one has
()
as n. Therefore, vnv in E. This completes the proof.

Theorem 6. Assume conditions (V), (h1)–(h3) hold; then (1) has a weak solution.

Proof. First, we prove that, for each θ ∈ (0,1], Iθ satisfy the Cerami condition. Indeed, let {vn} ⊂ E be an arbitrary Cerami sequence of Iθ. Set ϕ = f(vn)/f(vn). Then . Similar to the proof of (63), we can prove that {vn} is bounded in E. Hence, by Lemma 3, the sequence {vn} possesses a convergent subsequence in E. This shows that Iθ satisfy the Cerami condition.

Next, for any ε > 0, by (h1), (h2), (f3), and (f7), there exists C(ε) > 0 such that

()
for all (x, t) ∈ RN × R. For small 0 < ρ ≪ 1, set
()
Then, from (101), for vSρ,
()
for small ε > 0 and ρ > 0. Moreover, by (h3), for any (x, z) ∈ RN × R with |z | ≥ r, one has
()
Since μ > 4, there exists a constant 4 < α < min {μ, 2(2*)}. Hence, by (f5), we have
()
uniformly in xRN. Consequently, there exist constants τ > 1 such that
()
for all xRN. For any finite-dimensional subspace , by the equivalency of all norms in the finite-dimensional space, there is a constant a > 0 such that
()
By (h1), (h2), and (106), there exists a positive constant C > 0 such that
()
Since 4 < α < 2(2*), by (f3), (107), and (108), we have
()
for all . Hence there exists a large R > 0 such that Iθ < 0 on . Set a fixed with ∥eE = 1. For any fixed T > ρ, define the path by hT(t) = tTe. Then for large T > 0, by (109), one has
()
Hence by Theorem 2.2 with the Cerami condition in [20], Iθ possesses a critical value
()
where
()
Consequently, by Theorem 5, we know that (1) has a weak solution. This completes the proof of Theorem 6.

Remark 7. Let v+ = max {v, 0} and v = max {−v, 0}. Set

()
instead of I(u) and Iθ(u), respectively. Then, under the conditions of Theorem 6, we can obtain the existence of a positive solution and a negative solution for (1).

Theorem 8. Assume conditions (V), (h1)–(h3) hold. If h(x, s) is odd in s, then (1) has a sequence {vm} of solutions such that I(vm)→+.

Proof. Consider the eigenvalue of the operate L = −Δ + V. By assumption (V) and the compactness of the embedding EL2(RN), we know that the spectrum σ(L) = {λ1, λ2, …, λn⋯} of L with

()
and λn → + as n → + (see page 3820 in [21]). Let φn be the eigenfunction corresponding to λn. By regularity argument we know that φnE. Set En = span {φ1, φ2, …, φn}. Then we can decompose the space E as E = EnWn for n = 1,2, …, where Wn is orthogonal to En in E. For ρ > 0, set
()
By (109) there exists rn > 0 independent of θ such that
()
Set
()
where γ(·) is the genus. Let
()
We have the following three facts (we refer the reader to [16] for their proofs).
  •   

    Fact (1). For each B ∈ Γj, if 0 < ρ < rn for all nj, then BQρWj−1.

  •   

    Fact (2). There exist constants αjβj such that cj(θ)∈[αj, βj] and αj → + as j → +.

  •   

    Fact (3).  cj(θ), j = 1,2, … are critical values of Iθ.

Consequently, Theorem 8 follows from Theorem 5 and the above Facts (2)-(3). This completes the proof.

Corollary 9. If the following conditions (h4) and (h5) are used in place of (h3); then the conclusions of Theorem 5, Theorem 6, and Theorem 8 hold:

  • (h4) lim |s|→+inf H(x, s) > 0 uniformly in xN,

  • (h5) there exist μ > 4 and τ > 0 such that

    ()

for all xN and |s | ≥ τ.

Proof. By (h4), there are constants λ > 0 and r1 > 0 such that whenever |s | ≥ r1, one has

()
Set r = max {τ, r1}. Then, by (h5),
()
for all xN and |s | ≥ r. Therefore, condition (h3) holds. This completes the proof.

Acknowledgment

This work was supported partially by the National Natural Science Foundation of China (11261070).

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