1. Introduction and Preliminaries
In this paper we consider the quasilinear Schrödinger equation of the form
()
where
h ∈
C(
RN ×
R,
R) and
V ∈
C(
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 [
1–
5]. 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 [
8–
11] 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:
Set
()
with the inner product
()
and the norm
()
Then both
H1(
RN) and
E are Hilbert spaces.
By the continuity of the embedding
E↪
Ls(
ℝN) 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 x ∈ RN,
-
(h3) there exist μ > 4 and r > 0 such that
()
for all
x ∈
RN and |
s | ≥
r, where
.
By Lemma 3.4 in [17] we know that, under the assumption (V), the embedding E↪Ls(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 t ∈ R;
-
(f3) |f(t)|≤|t| for all t ∈ R;
-
(f4) lim t→0 f(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 t ∈ R;
-
(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 t ∈ R;
-
(f11) for all t ∈ R;
-
(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 [8–11]. 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(2
t) ≤
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 {3
ξ2,
M(
ξ)/
m(
ξ)}.
After the change of variable,
J(
u) can be reduced to
()
From [
8,
9,
11] we know that if
v ∈
E is a critical point of
I, that is,
()
for all
φ ∈
E, then
u : =
f(
v) is a weak solution of (
1). Particularly, if
v ∈
H1(
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 Iθ ∈ C1(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
v ∈
R. By (
26) and the continuity of the embedding
E↪
Ls(
RN) (
s ∈ [2, 2
*]),
()
Hence
Iθ is well defined in
E.
Now, we prove that Iθ ∈ C1(E, R). It suffices to prove that
()
For any v, ϕ ∈ E 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
ϕ ∈
E. Now, we show that
,
i = 1,2, are continuous. Indeed, if
vn →
v in
E, then
vn →
v 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
yn ∈
L2(
RN) and
zn ∈
Lr(
RN), one has
()
Hence
()
and hence
()
as
n →
∞. Therefore, Ψ
1 ∈
C1(
E,
R).
Define
()
with the norm
. On the space
, we define the norm
()
On the space
, we define the norm
()
From
vn →
v 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, Ψ
2 ∈
C1(
E,
R). This completes the proof.
Lemma 2. Assume that 1 ≤ p, q, r, s < +∞, g ∈ C(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/
r ≤
q/
s. Hence
()
for all (
x,
v) ∈
RN ×
R. Assume
vn →
v in
. Then
vn →
v 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.
x ∈
RN. 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 E↪Ls(RN) (2 ≤ s < 2*), passing to a subsequence, one has vn⇀v in E, vn → v in Ls(RN) for all 2 ≤ s < 2*, and vn(x) → v(x) for a.e. x ∈ RN. 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 vn ∈ E be a critical point of with for some constant c independent of n. Then, up to subsequence, one has vn → v 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
ϕ ∈
E. 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 : R → R is a smooth function satisfying b(s) = s for |s | ≤ T − 1, b(−s) = −b(s); b′(s) = 0 for s ≥ T, 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 ≤ CT ≤ T.
Let ; then ϕ ∈ E. 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
*/(8
N/(4
N − (
p − 4)(
N − 2))) = 2
*/2 −
p/4 + 1 > 1. Set
q = 8
N/(4
N − (
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
Ck →
C∞ > 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
vn⇀
v in
E,
vn →
v in
Ls(
RN) for
s ∈ [2, 2
*), and
vn(
x) →
v(
x) a.e.
x ∈
RN.
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 |∇(
vn −
v)|
2ψexp (−
f(
vn))
f′(
vn) ≥ 0, one has
()
Since
θn → 0, by (
63)
()
as
n →
∞. Moreover, notice that
vn⇀
v in
E,
vn →
v in
Ls(
RN) for
s ∈ [2, 2
*), and
vn(
x) →
v(
x) a.e.
x ∈
RN; by Hölder inequality and Lebesgue theorem, we have
()
Hence, from (
87), we have
()
For any
φ ∈
E 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
ψn →
ζ and
ψn(
x) →
ζ(
x) for a.e.
x ∈
RN. 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
v ∈
E 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 : =
vn −
v ∈
E. By (
f8), (
f12), and (
85), one has
()
Consequently, by (
f9), (
98), and Lemma
4, one has
()
as
n →
∞. Therefore,
vn →
v 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
v ∈
Sρ,
()
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
x ∈
RN. Consequently, there exist constants
τ > 1 such that
()
for all
x ∈
RN. 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 ∥
e∥
E = 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 E↪L2(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
φn ∈
E. Set
En = span {
φ1,
φ2, …,
φn}. Then we can decompose the space
E as
E =
En ⊕
Wn 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 n ≥ j, then B∩∂Qρ∩Wj−1 ≠ ∅.
-
Fact (2). There exist constants αj ≤ βj 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 x ∈ ℝN,
-
(h5) there exist μ > 4 and τ > 0 such that
()
for all
x ∈
ℝN 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
x ∈
ℝN 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).