Research Article Infinitely Many Solutions of Superlinear Elliptic Equation

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Hindawi Publishing Corporation
Abstract and Applied Analysis
Volume 2013, Article ID 769620, 6 pages
http://dx.doi.org/10.1155/2013/769620
Research Article
Infinitely Many Solutions of Superlinear Elliptic Equation
Anmin Mao and Yang Li
School of Mathematical Sciences, Qufu Normal University, Jining, Shandong 273165, China
Correspondence should be addressed to Anmin Mao; maoam@163.com
Received 4 January 2013; Revised 27 April 2013; Accepted 28 April 2013
Academic Editor: Wenming Zou
Copyright © 2013 A. Mao and Y. Li. This is an open access article distributed under the Creative Commons Attribution License,
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Via the Fountain theorem, we obtain the existence of infinitely many solutions of the following superlinear elliptic boundary value
problem: −Δ𝑒 = 𝑓(π‘₯, 𝑒) in Ω, 𝑒 = 0 on πœ•Ω, where Ω ⊂ R𝑁 (𝑁 > 2) is a bounded domain with smooth boundary and f is odd in
u and continuous. There is no assumption near zero on the behavior of the nonlinearity f, and f does not satisfy the AmbrosettiRabinowitz type technical condition near infinity.
1. Introduction
Consider the following nonlinear problem:
−Δ𝑒 = 𝑓 (π‘₯, 𝑒)
𝑒=0
in Ω,
on πœ•Ω,
(1)
which has been receiving much attention during the last several decades. Here Ω ⊂ R𝑁 (𝑁 > 2) is a bounded smooth
domain and 𝑓 is a continuous function on Ω × π‘… and odd in
𝑒. We make the following assumptions on 𝑓:
(𝑆1 ) there exist constants π‘Ž1 > 0 and 2𝑁/(𝑁 − 2) = 2∗ >
] > 2 such that
󡄨
󡄨󡄨
]−1
󡄨󡄨𝑓 (π‘₯, 𝑒)󡄨󡄨󡄨 ≤ π‘Ž1 (1 + |𝑒| ) ,
∀π‘₯ ∈ Ω, 𝑒 ∈ 𝑅;
(2)
𝐹 (π‘₯, 𝑒)
= ∞,
|𝑒| → ∞
𝑒2
uniformly for π‘₯ ∈ Ω,
(3)
−Δ𝑒 = πœ†π‘’ + 𝑓 (π‘₯, 𝑒)
in Ω, 𝑒 = 0 on πœ•Ω,
(5)
where Ω ⊂ 𝑅𝑁 is a bounded smooth domain, and assumed
𝑒
(𝑓1 ) 𝑓 ∈ 𝐢1 (Ω × π‘…, 𝑅),
(𝑓2 ) 𝑓(π‘₯, 0) = 0 = 𝑓𝑒 (π‘₯, 0),
where 𝐹(π‘₯, 𝑒) = ∫0 𝑓(π‘₯, 𝑒)𝑑π‘₯;
(𝑆3 ) there exists a constant 𝑏 > 0 such that
𝑓 (π‘₯, 𝑒) 𝑒 − 2𝐹(π‘₯, 𝑒)
lim sup
< 𝑏,
𝑒2 + 1
|𝑒| → ∞
Theorem 1. Assume that (𝑆1 )–(𝑆3 ) hold and 𝑓(π‘₯, 𝑒) is odd in
𝑒. Then problem (1) possesses infinitely many solutions.
Problem (1) was studied widely under various conditions
on 𝑓(π‘₯, 𝑒); see, for example, [6–10]. In 2007, Rabinowitz et al.
[6] studied the problem
(𝑆2 ) 𝐹(π‘₯, 𝑒) ≥ 0, for all (π‘₯, 𝑒) ∈ Ω × π‘…, and
lim
Note that Costa and Magalhães in [1] introduced a
condition similar to (𝑆3 ), which also appeared in [2].
In this paper, we will study the existence of infinitely many
nontrivial solutions of (1) via a variant of Fountain theorems
established by Zou in [3]. Fountain theorems and their dual
form were established by Bartsch in [4] and by Bartsch and
Willem in [5], respectively. They are effective tools for studying the existence of infinitely many large or small energy
solutions. It should be noted that the P.S. condition and its
variants play an important role for these theorems and their
applications.
We state our main result as follows.
uniformly for π‘₯ ∈ Ω.
(4)
(𝑓3 ) |𝑓(π‘₯, 𝑒)| ≤ 𝐢(1 + |𝑒|𝑝−1 ), 2 < 𝑝 < 2∗ ,
(𝑓4 ) ∃πœ‡ > 2, 𝑀 > 0, s.t.
π‘₯ ∈ Ω,
|𝑒| ≥ 𝑀 󳨐⇒ 0 < πœ‡πΉ (π‘₯, 𝑒) ≤ 𝑒𝑓 (π‘₯, 𝑒) ,
(6)
2
Abstract and Applied Analysis
(𝑓5 ) 𝐹(π‘₯, 𝑒) ≥ 0, for all π‘₯ and 𝑒, and 𝑒𝑓(π‘₯, 𝑒) > 0 for |𝑒| >
0 small.
They got the existence of at least three nontrivial solutions. (𝑓4 ) was given by Ambrosetti and Rabinowitz [11] to
ensure that some compactness and the Mountain Pass setting
hold.
However, there are many functions which are superlinear
but do not necessarily need to satisfy (𝑓4 ). For example,
1
1 𝑒2
𝐹 (π‘₯, 𝑒) = 𝑒2 ln (1 + 𝑒) − ( − 𝑒 + ln (1 + 𝑒)) .
2
2 2
(7)
It is easy to check that (𝑓4 ) does not hold. On the other
hand, in order to verify (𝑓4 ), it is usually an annoying task
to compute the primitive function of 𝑓 and sometimes it is
almost impossible, for example,
𝛼
𝑓 (π‘₯, 𝑒) = |𝑒| 𝑒 (1 + 𝑒(1+|sin 𝑒|) + |cos 𝑒|𝛼 ) ,
𝑒 ∈ 𝑅, 𝛼 > 0.
(8)
More examples are presented in Remark 2.
We recall that (𝑓4 ) implies a weaker condition
𝐹 (π‘₯, 𝑒) ≥ 𝑐|𝑒|πœƒ −𝑑,
𝑐, 𝑑 > 0, a.e. π‘₯ ∈ Ω, 𝑒 ∈ 𝑅, πœƒ > 2.
(9)
In [12], Willem and Zou gave one weaker condition
𝑐|𝑒|πœƒ ≤ 𝑒𝑓 (π‘₯, 𝑒)
for |𝑒| ≥ 𝑅0 , a.e. π‘₯ ∈ Ω, πœƒ > 2.
(10)
Note that (𝑆2 ) is much weaker than the above conditions.
In [13], Schechter and Zou proved that under the hypotheses that
(𝑆1 ) holds and
𝐹 (π‘₯, 𝑒)
𝐹 (π‘₯, 𝑒)
= +∞ or lim
= +∞,
2
𝑒
→
∞
𝑒 → −∞
𝑒
𝑒2
(11)
either lim
problem (1) has a nontrivial weak solution.
Recently, Miyagaki and Souto in [2] proved that problem
(1) has a nontrivial solution via the Mountain Pass theorem
under the following conditions:
lim
𝑓 (π‘₯, 𝑒)
= 0,
𝑒
(2) 𝑓(π‘₯, 𝑒) = 𝛾|𝑒|𝛾−2 𝑒+(𝛾−1)|𝑒|𝛾−3 𝑒 sin2 𝑒+|𝑒|𝛾−1 sin 2𝑒,
𝑒 ∈ 𝑅 \ {0}, 𝛾 > 2,
which do not satisfy (𝑓4 ). Example (2) can be found in [3].
So the case considered here cannot be covered by the cases
mentioned in [6, 11].
Remark 3. Compared with papers [11, 12], we do not assume
any superlinear conditions near zero. Compared with paper
[2], we do not impose any kind of monotonic conditions. In
addition, although we do not assume (𝑓4 ) holds, we are able
to check the boundedness of P.S. (or P.S.∗ ) sequences. So, our
result is different from those in the literature.
Our argument is variational and close to that in [2, 3,
13, 14]. The paper is arranged as follows. In Section 2 we
formulate the variational setting and recall some critical point
theorems required. We then in Section 3 complete the proof
of Theorem 1.
2. Variational Setting
In this section, we will first recall some related preliminaries and establish the variational setting for our problem.
Throughout this paper, we work on the space 𝐸 = 𝐻01 (Ω)
equipped with the norm
‖𝑒‖ = (∫ |∇𝑒|2 𝑑π‘₯)
Ω
1/2
.
(13)
Lemma 4. 𝐸 embeds continuously into 𝐿𝑝 , for all 0 < 𝑝 ≤ 2∗ ,
and compactly into 𝐿𝑝 , for all 1 ≤ 𝑝 < 2∗ ; hence there exists
πœπ‘ > 0 such that
|𝑒|𝑝 ≤ πœπ‘ ‖𝑒‖ ,
where |𝑒|𝑝 = (∫Ω |𝑒|𝑝 𝑑π‘₯)
1/𝑝
∀𝑒 ∈ 𝐸,
(14)
.
Define the Euler-Lagrange functional associated to problem (1), given by
𝑒 ∈ 𝐸,
(15)
where Ψ(𝑒) = ∫٠𝐹(π‘₯, 𝑒)𝑑π‘₯. Note that (𝑆1 ) implies that
∃ 𝑒0 > 0,
𝑓 (π‘₯, 𝑒)
s.t.
is increasing in 𝑒 ≥ 𝑒0
𝑒
(1) 𝑓(π‘₯, 𝑒) = 2𝑒 ln 𝑒 + 𝑒,
1
𝐼 (𝑒) = ‖𝑒‖2 − Ψ (𝑒) ,
2
(𝑆1 ) and (𝑆2 ) hold, and
|𝑒| → 0
Remark 2. To show that our assumptions (𝑆2 ) and (𝑆3 ) are
weaker than (𝑓4 ), we give two examples:
(12)
and decreasing in 𝑒 ≤ −𝑒0 , ∀π‘₯ ∈ Ω,
and they adapted some monotonicity arguments used by
Schechter and Zou [13]. This approach is interesting, but
many powerful variational tools such as the Fountain theorem and Morse theory are not directly applicable. In addition,
the monotonicity assumption on 𝐹(π‘₯, 𝑒)/𝑒2 is weaker than
the monotonicity assumption on 𝑓(π‘₯, 𝑒)/𝑒.
As to the case in the current paper, we make some
concluding remarks as follows.
𝐹 (π‘₯, 𝑒) ≤ π‘Ž1 (|𝑒| + |𝑒|] ) ,
∀ (π‘₯, 𝑒) ∈ Ω × π‘….
(16)
In view of (16) and Sobolev embedding theorem, πΌπœ‡ and
Ψ are well defined. Furthermore, we have the following.
Lemma 5 (see [15] or [16]). Suppose that (𝑆1 ) is satisfied. Then
Ψ ∈ 𝐢1 (𝐸, 𝑅) and ΨσΈ€  : 𝐸 → 𝐸∗ is compact and hence 𝐼 ∈
𝐢1 (𝐸, 𝑅). Moreover
ΨσΈ€  (𝑒) V = ∫ 𝑓 (π‘₯, 𝑒) V 𝑑π‘₯,
Ω
𝐼󸀠 (𝑒) V = ∫ ∇𝑒∇V 𝑑π‘₯ − ΨσΈ€  (𝑒)V,
(17)
Ω
for all 𝑒, V ∈ 𝐸, and critical points of 𝐼 on 𝐸 are solutions of (1).
Abstract and Applied Analysis
3
Lemma 6 (see [17]). Assume that |Ω| < ∞, 1 ≤ 𝑝, π‘Ÿ ≤
∞, 𝑓 ∈ 𝐢(Ω × π‘…), and |𝑓(π‘₯, 𝑒)| ≤ 𝑐(1 + |𝑒|𝑝/π‘Ÿ ). Then for every
𝑒 ∈ 𝐿𝑝 (Ω), 𝑓(π‘₯, 𝑒) ∈ πΏπ‘Ÿ (Ω), and the operator 𝐴 : 𝐿𝑝 (Ω) 󳨃→
πΏπ‘Ÿ (Ω) : 𝑒 󳨃→ 𝑓(π‘₯, 𝑒) is continuous.
3. Proof of Theorem 1
Let 𝐸 be a Banach space equipped with the norm β€– ⋅ β€–
and 𝐸 = ⨁𝑗∈𝑁𝑋𝑗 , where dim𝑋𝑗 < ∞ for any 𝑗 ∈ 𝑁. Set
π›Όπ‘˜ (πœ†) :=
Lemma 8. Assume that (𝑆1 )-(𝑆2 ) hold. Then there exists a
positive integer π‘˜1 and two sequences π‘Ÿπ‘˜ > πœŒπ‘˜ → ∞ as
π‘˜ → ∞ such that
1
π‘Œπ‘˜ = β¨π‘˜π‘—=1 𝑋𝑗 and π‘π‘˜ = ⨁∞
𝑗=π‘˜ 𝑋𝑗 . Consider the following 𝐢
functional Φπœ† : 𝐸 → 𝑅 defined by
Φπœ† (𝑒) := 𝐴 (𝑒) − πœ†π΅ (𝑒) ,
πœ† ∈ [1, 2] .
(18)
The following variant of the Fountain theorems was established in [3].
Theorem 7 (see [3, Theorem 2.1]). Assume that the functional
Φπœ† defined above satisfies the following:
(𝐹1 ) Φπœ† maps bounded sets to bounded sets uniformly for
πœ† ∈ [1, 2]; furthermore, Φπœ† (−𝑒) = Φπœ† (𝑒) for all
(πœ†, 𝑒) ∈ [1, 2] × πΈ;
(𝐹2 ) 𝐡(𝑒) ≥ 0 for all 𝑒 ∈ 𝐸; moreover, 𝐴(𝑒) → ∞ or
𝐡(𝑒) → ∞ as ‖𝑒‖ → ∞;
(𝐹3 ) there exists π‘Ÿπ‘˜ > πœŒπ‘˜ > 0 such that
π›Όπ‘˜ (πœ†) :=
:=
inf
𝑒∈π‘π‘˜ , ‖𝑒‖=πœŒπ‘˜
max
𝑒∈π‘Œπ‘˜ , ‖𝑒‖=π‘Ÿπ‘˜
Φπœ† (𝑒) > π›½π‘˜ (πœ†)
Φπœ† (𝑒) ,
∀πœ† ∈ [1, 2] .
∀π‘˜ ≥ π‘˜1 ,
(25)
max πΌπœ† (𝑒) < 0,
∀π‘˜ ∈ 𝑁,
(26)
𝑒∈π‘Œπ‘˜ ,‖𝑒‖=π‘Ÿπ‘˜
where π‘Œπ‘˜ = β¨π‘˜π‘—=1 𝑋𝑗 = span{𝑒1 , . . . , π‘’π‘˜ } and π‘π‘˜ = ⨁∞
𝑗=π‘˜ 𝑋𝑗 =
span{π‘’π‘˜ , . . .}, for all π‘˜ ∈ 𝑁.
Proof
Step 1. We first prove (25).
By (16) and (23), for all πœ† ∈ [1, 2] and 𝑒 ∈ 𝐸, we have
1
πΌπœ† (𝑒) ≥ ‖𝑒‖2 − 2 ∫ π‘Ž1 (|𝑒| + |𝑒|] ) 𝑑π‘₯
2
Ω
1
= ‖𝑒‖2 − 2π‘Ž1 (|𝑒|1 + |𝑒|]] ) ,
2
(27)
where π‘Ž1 is the constant in (16). Let
𝜎] (π‘˜) =
(19)
|𝑒|] ,
sup
𝑒∈π‘π‘˜ ,‖𝑒‖=1
∀π‘˜ ∈ 𝑁.
(28)
Then
Then
π›Όπ‘˜ (πœ†) ≤ πœπ‘˜ (πœ†) := inf max Φπœ† (𝛾 (𝑒)) , ∀πœ† ∈ [1, 2] ,
𝛾∈Γπ‘˜ 𝑒∈π΅π‘˜
∞
π‘˜
πœ† ∈ [1, 2], there exists a sequence {π‘’π‘š
(πœ†)}π‘š=1 such that
σ΅„©σ΅„©
σ΅„©σ΅„© π‘˜
π‘˜
sup σ΅„©σ΅„©σ΅„©π‘’π‘š (πœ†)σ΅„©σ΅„©σ΅„© < ∞, ΦσΈ€ πœ† (π‘’π‘š
(πœ†)) 󳨀→ 0,
π‘š
(21)
π‘˜
Φπœ† (π‘’π‘š (πœ†)) 󳨀→ πœπ‘˜ (πœ†) as m 󳨀→ ∞.
In order to apply the above theorem to prove our main
results, we define the functionals 𝐴, 𝐡, and πΌπœ† on our working
space 𝐸 by
𝐡 (𝑒) = ∫ 𝐹 (π‘₯, 𝑒) 𝑑π‘₯,
Ω
(24)
and the corresponding system of eigenfunctions {𝑒𝑗 : 𝑗 ∈
𝑁}(−Δ𝑒𝑗 = πœ† 𝑗 𝑒𝑗 ) forming an orthogonal basis in 𝐸. Let
𝑋𝑗 = span{𝑒𝑗 }, for all 𝑗 ∈ 𝑁.
as π‘˜ 󳨀→ ∞,
(29)
since 𝐸 is compactly embedded into 𝐿] . Combining (14), (27),
and (28), we have
1
πΌπœ† ≥ ‖𝑒‖2 − 2π‘Ž1 𝜏1 ‖𝑒‖ − 2π‘Ž1 𝜎]] (π‘˜) ‖𝑒‖] ,
2
(30)
∀ (πœ†, 𝑒) ∈ [1, 2] × π‘π‘˜ .
By (29), there exists a positive integer π‘˜1 > 0 such that
πœŒπ‘˜ := (16π‘Ž1 𝜎]] (π‘˜))
1/(2−])
> 16π‘Ž1 𝜏1 ,
∀π‘˜ ≥ π‘˜1 ,
(31)
since ] > 2. Evidently,
πœŒπ‘˜ 󳨀→ ∞ as π‘˜ 󳨀→ ∞.
(22)
1
πΌπœ† (𝑒) = 𝐴 (𝑒) − πœ†π΅ (𝑒) = ‖𝑒‖2 − πœ† ∫ 𝐹 (π‘₯, 𝑒) 𝑑π‘₯, (23)
2
Ω
for all 𝑒 ∈ 𝐸 and πœ† ∈ [1, 2]. Note that 𝐼1 = 𝐼, where 𝐼 is the
functional defined in (15).
From Lemma 5, we know that πΌπœ† ∈ 𝐢1 (𝐸, 𝑅), for all
πœ† ∈ [1, 2]. It is known that −Δ is a selfadjoint operator with a
sequence of eigenvalues (counted with multiplicity)
0 < πœ† 1 < πœ† 2 ≤ πœ† 3 ≤ ⋅ ⋅ ⋅ ≤ πœ† 𝑗 ≤ ⋅ ⋅ ⋅ 󳨀→ ∞,
𝜎] (π‘˜) 󳨀→ 0
(20)
where π΅π‘˜ = {𝑒 ∈ π‘Œπ‘˜ : ‖𝑒‖ ≤ π‘Ÿπ‘˜ } and Γπ‘˜ := {𝛾 ∈
𝐢(π΅π‘˜ , 𝐸) | 𝛾 is odd, 𝛾|πœ•π΅π‘˜ = 𝑖𝑑}. Moreover, for a.e.
1
𝐴 (𝑒) = ‖𝑒‖2 ,
2
π›½π‘˜ (πœ†) :=
πΌπœ† (𝑒) > 0,
inf
𝑒∈π‘π‘˜ ,‖𝑒‖=πœŒπ‘˜
(32)
Combining (30) and (31), direct computation shows
π›Όπ‘˜ :=
inf
𝑒∈π‘π‘˜ ,‖𝑒‖=πœŒπ‘˜
πΌπœ† (𝑒) ≥
πœŒπ‘˜2
> 0,
4
∀π‘˜ ≥ π‘˜1 .
(33)
Step 2. We then verify (26).
We claim that for any finite-dimensional subspace 𝐹 ⊂ 𝐸,
there exists a constant πœ– > 0 such that
π‘š ({π‘₯ ∈ Ω : |𝑒 (π‘₯)| ≥ πœ– ‖𝑒‖}) ≥ πœ–,
∀𝑒 ∈ 𝐹 \ {0} .
(34)
Here and in the sequel, π‘š(⋅) always denotes the Lebesgue
measure in 𝑅.
4
Abstract and Applied Analysis
If not, for any 𝑛 ∈ 𝑁, there exists 𝑒𝑛 ∈ 𝐹 \ {0} such that
1
󡄨 1σ΅„© σ΅„©
󡄨
π‘š ({π‘₯ ∈ Ω : 󡄨󡄨󡄨𝑒𝑛 (π‘₯)󡄨󡄨󡄨 ≥ 󡄩󡄩󡄩𝑒𝑛 σ΅„©σ΅„©σ΅„©}) < .
𝑛
𝑛
Combining (23), (42), (43), and (𝑆2 ), for any π‘˜ ∈ 𝑁 and πœ† ∈
[1, 2], we have
(35)
1
|𝑒|2
𝑑π‘₯
πΌπœ† (𝑒) ≤ ‖𝑒‖2 − ∫
3
2
Λπ‘˜π‘’ πœ–π‘˜
Let V𝑛 = 𝑒𝑛 /‖𝑒𝑛 β€– ∈ 𝐹, for all 𝑛 ∈ 𝑁. Then β€–V𝑛 β€– = 1, for all
𝑛 ∈ 𝑁, and
1
󡄨 1
󡄨
π‘š ({π‘₯ ∈ Ω : 󡄨󡄨󡄨V𝑛 (π‘₯)󡄨󡄨󡄨 ≥ }) < ,
𝑛
𝑛
∀𝑛 ∈ 𝑁.
1
1
≤ ‖𝑒‖2 − 3 πœ–π‘˜2 ‖𝑒‖2 π‘š (Λπ‘˜π‘’ )
2
πœ–π‘˜
(36)
1
≤ ‖𝑒‖2 − ‖𝑒‖2
2
Passing to a subsequence if necessary, we may assume V𝑛 →
V0 in 𝐸, for some V0 ∈ 𝐹, since 𝐹 is of finite dimension.
Evidently, β€–V0 β€– = 1. In view of Lemma 4 and the equivalence
of any two norms on 𝐹, we have
󡄨
󡄨
∫ 󡄨󡄨󡄨V𝑛 − V0 󡄨󡄨󡄨 𝑑π‘₯ 󳨀→ 0 as 𝑛 󳨀→ ∞,
Ω
(37)
and |V0 |∞ > 0.
By the definition of norm | ⋅ |∞ , there exists a constant
𝛿0 > 0 such that
󡄨
󡄨
π‘š ({π‘₯ ∈ Ω : 󡄨󡄨󡄨V0 (π‘₯)󡄨󡄨󡄨 ≥ 𝛿0 }) ≥ 𝛿0 .
(38)
For any 𝑛 ∈ 𝑁, let
󡄨 1
󡄨
Λ π‘› = {π‘₯ ∈ Ω : 󡄨󡄨󡄨V𝑛 (π‘₯)󡄨󡄨󡄨 < } ,
𝑛
Λ𝑐𝑛
󡄨 1
󡄨
= Ω \ Λ π‘› = {π‘₯ ∈ Ω : 󡄨󡄨󡄨V𝑛 (π‘₯)󡄨󡄨󡄨 ≥ } .
𝑛
(39)
π‘š (Λ π‘› ∩ Λ 0 ) = π‘š (Λ 0 \ Λ𝑐𝑛 )
1 𝛿0
≥ .
𝑛
2
(40)
Consequently, for 𝑛 large enough, there holds
󡄨
󡄨
∫ 󡄨󡄨󡄨V𝑛 − V0 󡄨󡄨󡄨 𝑑π‘₯ ≥ ∫
Ω
Λ π‘› ∩Λ 0
≥∫
Λ π‘› ∩Λ 0
≥
∀ |𝑒| ≥ π‘†π‘˜ .
then (44) implies
π›½π‘˜ (πœ†) :=
max πΌπœ† (𝑒) ≤ −
𝑒∈π‘Œπ‘˜ ,‖𝑒‖=π‘Ÿπ‘˜
π‘Ÿπ‘˜2
< 0,
2
∀π‘˜ ∈ 𝑁,
(46)
Proof of Theorem 1. It follows from (16), (23), and Lemma 5
that πΌπœ† maps bounded sets to bounded sets uniformly for
πœ† ∈ [1, 2]. In view of the evenness of 𝐹(π‘₯, 𝑒) in 𝑒, it holds that
πΌπœ† (−𝑒) = πΌπœ† (𝑒) for all (πœ†, 𝑒) ∈ [1, 2] × πΈ. Thus the condition
(𝐹1 ) of Theorem 7 holds. Besides, 𝐴(𝑒) = (1/2)‖𝑒‖2 → ∞
as ‖𝑒‖ → ∞ and 𝐡(𝑒) ≥ 0 since 𝐹(π‘₯, 𝑒) ≥ 0. Thus
the condition (𝐹2 ) of Theorem 7 holds. And Lemma 8 shows
that the condition (𝐹3 ) holds for all π‘˜ ≥ π‘˜1 . Therefore, by
Theorem 7, for any π‘˜ ≥ π‘˜1 and a.e. πœ† ∈ [1, 2], there exists
∞
π‘˜
(πœ†)}π‘š=1 ⊂ 𝐸 such that
a sequence {π‘’π‘š
π‘˜
πΌπœ†σΈ€  (π‘’π‘š
(πœ†)) 󳨀→ 0,
πœπ‘˜ (πœ†) := inf max πΌπœ† (β„Ž (𝑒)) ,
β„Ž∈Γπ‘˜ 𝑒∈π΅π‘˜
(47)
∀πœ† ∈ [1, 2] ,
(48)
with π΅π‘˜ = {𝑒 ∈ π‘Œπ‘˜ : ‖𝑒‖ ≤ π‘Ÿπ‘˜ } and Γπ‘˜ := {β„Ž ∈ 𝐢(π΅π‘˜ , 𝐸) |
β„Ž is odd, β„Ž|πœ•π΅π‘˜ = 𝑖𝑑}.
Furthermore, it follows from the proof of Lemma 8 that
(42)
where Λπ‘˜π‘’ := {π‘₯ ∈ Ω : |𝑒(π‘₯)| ≥ πœ–π‘˜ ‖𝑒‖}, for all π‘˜ ∈ 𝑁, and
𝑒 ∈ π‘Œπ‘˜ \ {0}. By (𝑆2 ), for any π‘˜ ∈ 𝑁, there exists a constant
π‘†π‘˜ > 0 such that
|𝑒|2
,
πœ–π‘˜3
(45)
as π‘š → ∞, where
(41)
This is in contradiction to (37). Therefore (34) holds.
Consequently, for any π‘˜ ∈ 𝑁, there exists a constant πœ–π‘˜ >
0 such that
𝐹 (π‘₯, 𝑒) ≥
π‘†π‘˜
},
πœ–π‘˜
π‘˜
πΌπœ† (π‘’π‘š
(πœ†)) 󳨀→ πœπ‘˜ (πœ†)
󡄨 󡄨 󡄨 󡄨
(󡄨󡄨󡄨V0 󡄨󡄨󡄨 − 󡄨󡄨󡄨V𝑛 󡄨󡄨󡄨) 𝑑π‘₯
∀𝑒 ∈ π‘Œπ‘˜ \ {0} ,
π‘Ÿπ‘˜ > max {πœŒπ‘˜ ,
π‘š
𝛿02
> 0.
4
π‘š (Λπ‘˜π‘’ ) ≥ πœ–π‘˜ ,
with ‖𝑒‖ ≥ π‘†π‘˜ /πœ–π‘˜ . Now for any π‘˜ ∈ 𝑁, if we choose
σ΅„©
σ΅„© π‘˜
sup σ΅„©σ΅„©σ΅„©σ΅„©π‘’π‘š
(πœ†)σ΅„©σ΅„©σ΅„©σ΅„© < ∞,
󡄨󡄨
󡄨
󡄨󡄨V𝑛 − V0 󡄨󡄨󡄨 𝑑π‘₯
1
≥ (𝛿0 − ) π‘š (Λ π‘› ∩ Λ 0 )
𝑛
1
= − ‖𝑒‖2
2
ending the proof.
Set Λ 0 = {π‘₯ ∈ Ω : |V0 (π‘₯)| ≥ 𝛿0 }. Then for 𝑛 large enough, by
(36) and (38), we have
≥ π‘š (Λ 0 ) − π‘š (Λ𝑐𝑛 ) ≥ 𝛿0 −
(44)
(43)
πœπ‘˜ (πœ†) ∈ [π›Όπ‘˜ , πœπ‘˜ ] ,
∀π‘˜ ≥ π‘˜1 ,
(49)
where πœπ‘˜ := max𝑒∈π΅π‘˜ πΌπœ† (𝑒) and π›Όπ‘˜ := πœŒπ‘˜2 /4 → ∞ as π‘˜ → ∞
by (32).
∞
π‘˜
Claim 1. {π‘’π‘š
(πœ†)}π‘š=1 ⊂ 𝐸 possesses a strong convergent
subsequence in 𝐸, for ∀πœ† ∈ [1, 2] and π‘˜ ≥ π‘˜1 .
∞
π‘˜
In fact, by the boundedness of the {π‘’π‘š
(πœ†)}π‘š=1 , passing to
a subsequence, as π‘š → ∞, we may assume
π‘˜
π‘’π‘š
(πœ†) ⇀ π‘’π‘˜ (πœ†)
in 𝐸.
(50)
Abstract and Applied Analysis
5
By the Sobolev embedding theorem,
π‘˜
π‘’π‘š
(πœ†) 󳨀→ π‘’π‘˜ (πœ†)
in 𝐿] .
(51)
Let Ω =ΜΈ = {π‘₯ ∈ Ω : V(π‘₯) =ΜΈ 0}. If π‘₯ ∈ Ω =ΜΈ , from (𝑆2 ) it follows
that
lim
Lemma 6 implies that
π‘˜
𝑓 (π‘₯, π‘’π‘š
(πœ†)) 󳨀→ 𝑓 (π‘₯, π‘’π‘˜ (πœ†))
in 𝐿]/(]−1) .
(52)
Observe that
σ΅„©σ΅„©σ΅„©π‘’π‘˜ (πœ†) − π‘’π‘˜ (πœ†)σ΅„©σ΅„©σ΅„©2
σ΅„©σ΅„©
σ΅„©σ΅„© π‘š
Ω
π‘˜
(𝑓 (π‘₯, π‘’π‘š
π‘˜
(53)
(πœ†)) − 𝑓 (π‘₯, 𝑒 (πœ†)))
∫
𝐹 (π‘₯, 𝑒𝑛 (π‘₯))
𝑒𝑛 (π‘₯)2
as π‘š 󳨀→ ∞.
Ω
𝑛→∞
< lim sup
󡄨
󡄨
π‘˜
≤ 󡄨󡄨󡄨󡄨𝑓 (π‘₯, π‘’π‘š
(πœ†)) − 𝑓 (π‘₯, π‘’π‘˜ (πœ†))󡄨󡄨󡄨󡄨]/(]−1)
as π‘š → ∞. Thus by (53), (54), and (55), we have proved that
σ΅„©σ΅„©σ΅„©π‘’π‘˜ (πœ†) − π‘’π‘˜ (πœ†)σ΅„©σ΅„©σ΅„© 󳨀→ 0 as π‘š 󳨀→ ∞,
(56)
σ΅„©σ΅„©
σ΅„©σ΅„© π‘š
π‘˜
that is, π‘’π‘š
(πœ†) → π‘’π‘˜ (πœ†) in 𝐸.
Thus, for each π‘˜ ≥ π‘˜1 , we can choose πœ† 𝑛 → 1
∞
π‘˜
(πœ† 𝑛 )}π‘š=1 obtained a convergent
such that the sequence {π‘’π‘š
subsequence; passing again to a subsequence, we may assume
(57)
This together with (47) and (49) yields
πΌπœ† 𝑛 (π‘’π‘›π‘˜ ) ∈ [π›Όπ‘˜ , πœπ‘˜ ] ,
∀𝑛 ∈ 𝑁, π‘˜ ≥ π‘˜1 .
(58)
∞
Claim 2. {π‘’π‘›π‘˜ }𝑛=1 is bounded in 𝐸 for all π‘˜ ≥ π‘˜1 .
For notational simplicity, we will set 𝑒𝑛 = π‘’π‘›π‘˜ for all 𝑛 ∈
𝑁 throughout this paragraph. If {𝑒𝑛 } is unbounded in 𝐸, we
define V𝑛 = 𝑒𝑛 /‖𝑒𝑛 β€–. Since β€–V𝑛 β€– = 1, without loss of generality
we suppose that there is V ∈ 𝐸 such that
in 𝐸,
in 𝐿] (Ω) ,
V𝑛 (π‘₯) 󳨀→ V (π‘₯)
a.e. in Ω.
(59)
2𝑒𝑛2
(63)
V𝑛2 = 0
which contradicts (62). Hence {𝑒𝑛 } is bounded.
Claim 3. {π‘’π‘›π‘˜ } possesses a convergent subsequence with the
limit π‘’π‘˜ ∈ 𝐸 for all π‘˜ ≥ π‘˜1 .
In fact, by Claim 2, without loss of generality, we have
assume
π‘’π‘›π‘˜ ⇀ π‘’π‘˜
(55)
in 𝐸, ∀𝑛 ∈ 𝑁, π‘˜ ≥ π‘˜1 .
𝑏 (𝑒𝑛2 + 1)
𝑛→∞
󡄨
󡄨󡄨
󡄨󡄨∫ (𝑓 (π‘₯, π‘’π‘˜ (πœ†)) − 𝑓 (π‘₯, π‘’π‘˜ (πœ†))) (π‘’π‘˜ (πœ†) − π‘’π‘˜ (πœ†)) 𝑑π‘₯󡄨󡄨󡄨
󡄨󡄨
󡄨󡄨
π‘š
π‘š
󡄨
󡄨 Ω
󡄨
󡄨 π‘˜
× σ΅„¨σ΅„¨σ΅„¨σ΅„¨π‘’π‘š
(πœ†) − π‘’π‘˜ (πœ†)󡄨󡄨󡄨󡄨] 󳨀→ 0
(1/2) 𝑓 (π‘₯, 𝑒𝑛 ) 𝑒𝑛 − 𝐹 (π‘₯, 𝑒𝑛 ) 2
V𝑛
𝑒𝑛2
(54)
It follows from the Hölder inequality, (51), and (52) that
V𝑛 󳨀→ V
(61)
By (𝑆3 ),
π‘˜
π‘˜
(πΌπœ†σΈ€  (π‘’π‘š
(πœ†)) − πΌπœ†σΈ€  (π‘’π‘˜ (πœ†)) , π‘’π‘š
(πœ†) − π‘’π‘˜ (πœ†)) 󳨀→ 0
V𝑛 ⇀ V
1
V𝑛 (π‘₯)2 = .
2
πΌπœ† (𝑒𝑛 )
(1/2) 𝑓 (π‘₯, 𝑒𝑛 ) 𝑒𝑛 − 𝐹 (π‘₯, 𝑒𝑛 ) 2
V𝑛 𝑑π‘₯ = 𝑛󡄩 σ΅„©2 > 0. (62)
2
𝑒𝑛
πœ† 𝑛 󡄩󡄩󡄩𝑒𝑛 σ΅„©σ΅„©σ΅„©
lim sup
(πœ† 𝑛 ) = π‘’π‘›π‘˜
(60)
We conclude that Ω =ΜΈ has zero measure and V ≡ 0 a.e. in Ω.
Moreover, from (49) and (58)
By (47), it is clear that
πΌπœ†σΈ€  𝑛 (π‘’π‘›π‘˜ ) = 0,
𝑒𝑛 (π‘₯)
V𝑛 (π‘₯)2 = ∞.
On the other hand, after a simple calculation, we have
lim ∫
π‘˜
× (π‘’π‘š
(πœ†) − π‘’π‘˜ (πœ†)) 𝑑π‘₯.
lim π‘’π‘˜
π‘š→∞ π‘š
2
𝑛→∞ Ω
π‘˜
π‘˜
= (πΌπœ†σΈ€  (π‘’π‘š
(πœ†)) − πΌπœ†σΈ€  (π‘’π‘˜ (πœ†)) , π‘’π‘š
(πœ†) − π‘’π‘˜ (πœ†))
+ πœ†∫
𝐹 (π‘₯, 𝑒𝑛 (π‘₯))
𝑛→∞
as 𝑛 󳨀→ ∞.
(64)
By virtue of the Riesz Representation theorem, πΌπœ†σΈ€  : 𝐸 󳨃→ 𝐸∗
and ΨσΈ€  : 𝐸 󳨃→ 𝐸∗ can be viewed as πΌπœ†σΈ€  : 𝐸 󳨃→ 𝐸 and ΨσΈ€  : 𝐸 󳨃→
𝐸, respectively, where 𝐸∗ is the dual space of 𝐸. Note that
0 = πΌπœ†σΈ€  𝑛 (π‘’π‘›π‘˜ ) = π‘’π‘›π‘˜ − πœ† 𝑛 ΨσΈ€  (π‘’π‘›π‘˜ ) ,
(65)
π‘’π‘›π‘˜ = πœ† 𝑛 ΨσΈ€  (π‘’π‘›π‘˜ ) .
(66)
that is
By Lemma 5, ΨσΈ€  : 𝐸 󳨃→ 𝐸 is also compact. Due to the
compactness of ΨσΈ€  and (64), the right-hand side of (66)
converges strongly in 𝐸 and hence π‘’π‘›π‘˜ → π‘’π‘˜ in 𝐸.
Now for each π‘˜ ≥ π‘˜1 , by (58), the limit π‘’π‘˜ is just a critical
point of 𝐼1 = 𝐼 with 𝐼(π‘’π‘˜ ) ∈ [π›Όπ‘˜ , πœπ‘˜ ]. Since π›Όπ‘˜ → ∞ as
π‘˜ → ∞ in (49), we get infinitely many nontrivial critical
points of 𝐼. Therefore (1) possesses infinitely many nontrivial
solutions by Lemma 5.
Acknowledgments
The authors would like to thank the referee for valuable
comments and helpful suggestions. The first author would
like to acknowledge the hospitality of Professor Y. Ding of the
AMSS of the Chinese Academy of Sciences, where this paper
was written during his visit. Anmin Mao was supported by
NSFC (11101237) and ZR2012AM006.
6
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