Infinitely Many Solutions of Superlinear Elliptic Equation

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Jan 4, 2013 - Via the Fountain theorem, we obtain the existence of infinitely many solutions of the following superlinear elliptic boundary value problem:Β ...
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; [email protected] Received 4 January 2013; Revised 27 April 2013; Accepted 28 April 2013 Academic Editor: Wenming Zou Copyright Β© 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: βˆ’Ξ”π‘’ = 𝑓(π‘₯, 𝑒) in Ξ©, 𝑒 = 0 on πœ•Ξ©, where Ξ© βŠ‚ 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: βˆ’Ξ”π‘’ = 𝑓 (π‘₯, 𝑒) 𝑒=0

in Ξ©,

on πœ•Ξ©,

(1)

which has been receiving much attention during the last several decades. Here Ξ© βŠ‚ R𝑁 (𝑁 > 2) is a bounded smooth domain and 𝑓 is a continuous function on Ξ© Γ— 𝑅 and odd in 𝑒. We make the following assumptions on 𝑓: (𝑆1 ) there exist constants π‘Ž1 > 0 and 2𝑁/(𝑁 βˆ’ 2) = 2βˆ— > ] > 2 such that 󡄨 󡄨󡄨 ]βˆ’1 󡄨󡄨𝑓 (π‘₯, 𝑒)󡄨󡄨󡄨 ≀ π‘Ž1 (1 + |𝑒| ) ,

βˆ€π‘₯ ∈ Ξ©, 𝑒 ∈ 𝑅;

(2)

𝐹 (π‘₯, 𝑒) = ∞, |𝑒| β†’ ∞ 𝑒2

uniformly for π‘₯ ∈ Ξ©,

(3)

βˆ’Ξ”π‘’ = πœ†π‘’ + 𝑓 (π‘₯, 𝑒)

in Ξ©, 𝑒 = 0 on πœ•Ξ©,

(5)

where Ξ© βŠ‚ 𝑅𝑁 is a bounded smooth domain, and assumed

𝑒

(𝑓1 ) 𝑓 ∈ 𝐢1 (Ξ© Γ— 𝑅, 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 βˆ’ 2𝐹(π‘₯, 𝑒) lim sup < 𝑏, 𝑒2 + 1 |𝑒| β†’ ∞

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) β‰₯ 0, for all (π‘₯, 𝑒) ∈ Ξ© Γ— 𝑅, and lim

Note that Costa and Magalh˜aes 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‘₯ ∈ Ξ©. (4)

(𝑓3 ) |𝑓(π‘₯, 𝑒)| ≀ 𝐢(1 + |𝑒|π‘βˆ’1 ), 2 < 𝑝 < 2βˆ— , (𝑓4 ) βˆƒπœ‡ > 2, 𝑀 > 0, s.t. π‘₯ ∈ Ξ©,

|𝑒| β‰₯ 𝑀 󳨐⇒ 0 < πœ‡πΉ (π‘₯, 𝑒) ≀ 𝑒𝑓 (π‘₯, 𝑒) ,

(6)

2

Abstract and Applied Analysis (𝑓5 ) 𝐹(π‘₯, 𝑒) β‰₯ 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) βˆ’ ( βˆ’ 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) β‰₯ 𝑐|𝑒|πœƒ βˆ’π‘‘,

𝑐, 𝑑 > 0, a.e. π‘₯ ∈ Ξ©, 𝑒 ∈ 𝑅, πœƒ > 2. (9)

In [12], Willem and Zou gave one weaker condition 𝑐|𝑒|πœƒ ≀ 𝑒𝑓 (π‘₯, 𝑒)

for |𝑒| β‰₯ 𝑅0 , a.e. π‘₯ ∈ Ξ©, 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 β†’ ∞ 𝑒 β†’ βˆ’βˆž 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|π›Ύβˆ’2 𝑒+(π›Ύβˆ’1)|𝑒|π›Ύβˆ’3 𝑒 sin2 𝑒+|𝑒|π›Ύβˆ’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.βˆ— ) 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 (Ξ©) equipped with the norm ‖𝑒‖ = (∫ |βˆ‡π‘’|2 𝑑π‘₯) Ξ©

1/2

.

(13)

Lemma 4. 𝐸 embeds continuously into 𝐿𝑝 , for all 0 < 𝑝 ≀ 2βˆ— , and compactly into 𝐿𝑝 , for all 1 ≀ 𝑝 < 2βˆ— ; hence there exists πœπ‘ > 0 such that |𝑒|𝑝 ≀ πœπ‘ ‖𝑒‖ , where |𝑒|𝑝 = (∫Ω |𝑒|𝑝 𝑑π‘₯)

1/𝑝

βˆ€π‘’ ∈ 𝐸,

(14)

.

Define the Euler-Lagrange functional associated to problem (1), given by 𝑒 ∈ 𝐸,

(15)

where Ξ¨(𝑒) = ∫Ω 𝐹(π‘₯, 𝑒)𝑑π‘₯. Note that (𝑆1 ) implies that

βˆƒ 𝑒0 > 0,

𝑓 (π‘₯, 𝑒) s.t. is increasing in 𝑒 β‰₯ 𝑒0 𝑒

(1) 𝑓(π‘₯, 𝑒) = 2𝑒 ln 𝑒 + 𝑒,

1 𝐼 (𝑒) = ‖𝑒‖2 βˆ’ Ξ¨ (𝑒) , 2

(𝑆1 ) and (𝑆2 ) hold, and |𝑒| β†’ 0

Remark 2. To show that our assumptions (𝑆2 ) and (𝑆3 ) are weaker than (𝑓4 ), we give two examples:

(12)

and decreasing in 𝑒 ≀ βˆ’π‘’0 , βˆ€π‘₯ ∈ Ξ©, 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|] ) ,

βˆ€ (π‘₯, 𝑒) ∈ Ξ© Γ— 𝑅.

(16)

In view of (16) and Sobolev embedding theorem, πΌπœ‡ and Ξ¨ are well defined. Furthermore, we have the following. Lemma 5 (see [15] or [16]). Suppose that (𝑆1 ) is satisfied. Then Ξ¨ ∈ 𝐢1 (𝐸, 𝑅) and Ξ¨σΈ€  : 𝐸 β†’ πΈβˆ— is compact and hence 𝐼 ∈ 𝐢1 (𝐸, 𝑅). Moreover Ξ¨σΈ€  (𝑒) V = ∫ 𝑓 (π‘₯, 𝑒) V 𝑑π‘₯, Ξ©

𝐼󸀠 (𝑒) V = ∫ βˆ‡π‘’βˆ‡V 𝑑π‘₯ βˆ’ Ξ¨σΈ€  (𝑒)V,

(17)

Ξ©

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 |Ξ©| < ∞, 1 ≀ 𝑝, π‘Ÿ ≀ ∞, 𝑓 ∈ 𝐢(Ξ© Γ— 𝑅), and |𝑓(π‘₯, 𝑒)| ≀ 𝑐(1 + |𝑒|𝑝/π‘Ÿ ). Then for every 𝑒 ∈ 𝐿𝑝 (Ξ©), 𝑓(π‘₯, 𝑒) ∈ πΏπ‘Ÿ (Ξ©), and the operator 𝐴 : 𝐿𝑝 (Ξ©) 󳨃→ πΏπ‘Ÿ (Ξ©) : 𝑒 󳨃→ 𝑓(π‘₯, 𝑒) is continuous.

3. Proof of Theorem 1

Let 𝐸 be a Banach space equipped with the norm β€– β‹… β€– and 𝐸 = β¨π‘—βˆˆπ‘π‘‹π‘— , 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‘˜ β†’ ∞ as π‘˜ β†’ ∞ such that

1 π‘Œπ‘˜ = β¨π‘˜π‘—=1 𝑋𝑗 and π‘π‘˜ = ⨁∞ 𝑗=π‘˜ 𝑋𝑗 . Consider the following 𝐢 functional Ξ¦πœ† : 𝐸 β†’ 𝑅 defined by

Ξ¦πœ† (𝑒) := 𝐴 (𝑒) βˆ’ 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 Ξ¦πœ† defined above satisfies the following: (𝐹1 ) Ξ¦πœ† maps bounded sets to bounded sets uniformly for πœ† ∈ [1, 2]; furthermore, Ξ¦πœ† (βˆ’π‘’) = Ξ¦πœ† (𝑒) for all (πœ†, 𝑒) ∈ [1, 2] Γ— 𝐸; (𝐹2 ) 𝐡(𝑒) β‰₯ 0 for all 𝑒 ∈ 𝐸; moreover, 𝐴(𝑒) β†’ ∞ or 𝐡(𝑒) β†’ ∞ as ‖𝑒‖ β†’ ∞; (𝐹3 ) there exists π‘Ÿπ‘˜ > πœŒπ‘˜ > 0 such that π›Όπ‘˜ (πœ†) := :=

inf

π‘’βˆˆπ‘π‘˜ , ‖𝑒‖=πœŒπ‘˜

max

π‘’βˆˆπ‘Œπ‘˜ , ‖𝑒‖=π‘Ÿπ‘˜

Ξ¦πœ† (𝑒) > π›½π‘˜ (πœ†)

Ξ¦πœ† (𝑒) ,

βˆ€πœ† ∈ [1, 2] .

βˆ€π‘˜ β‰₯ π‘˜1 ,

(25)

max πΌπœ† (𝑒) < 0,

βˆ€π‘˜ ∈ 𝑁,

(26)

π‘’βˆˆπ‘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) β‰₯ ‖𝑒‖2 βˆ’ 2 ∫ π‘Ž1 (|𝑒| + |𝑒|] ) 𝑑π‘₯ 2 Ξ© 1 = ‖𝑒‖2 βˆ’ 2π‘Ž1 (|𝑒|1 + |𝑒|]] ) , 2

(27)

where π‘Ž1 is the constant in (16). Let 𝜎] (π‘˜) =

(19)

|𝑒|] ,

sup

π‘’βˆˆπ‘π‘˜ ,‖𝑒‖=1

βˆ€π‘˜ ∈ 𝑁.

(28)

Then

Then π›Όπ‘˜ (πœ†) ≀ πœπ‘˜ (πœ†) := inf max Ξ¦πœ† (𝛾 (𝑒)) , βˆ€πœ† ∈ [1, 2] , π›ΎβˆˆΞ“π‘˜ π‘’βˆˆπ΅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΅„© < ∞, Ξ¦σΈ€ πœ† (π‘’π‘š (πœ†)) 󳨀→ 0, π‘š (21) π‘˜ Ξ¦π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‘₯, Ξ©

(24)

and the corresponding system of eigenfunctions {𝑒𝑗 : 𝑗 ∈ 𝑁}(βˆ’Ξ”π‘’π‘— = 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† β‰₯ ‖𝑒‖2 βˆ’ 2π‘Ž1 𝜏1 ‖𝑒‖ βˆ’ 2π‘Ž1 𝜎]] (π‘˜) ‖𝑒‖] , 2

(30)

βˆ€ (πœ†, 𝑒) ∈ [1, 2] Γ— π‘π‘˜ . By (29), there exists a positive integer π‘˜1 > 0 such that πœŒπ‘˜ := (16π‘Ž1 𝜎]] (π‘˜))

1/(2βˆ’])

> 16π‘Ž1 𝜏1 ,

βˆ€π‘˜ β‰₯ π‘˜1 ,

(31)

since ] > 2. Evidently, πœŒπ‘˜ 󳨀→ ∞ as π‘˜ 󳨀→ ∞.

(22)

1 πΌπœ† (𝑒) = 𝐴 (𝑒) βˆ’ πœ†π΅ (𝑒) = ‖𝑒‖2 βˆ’ πœ† ∫ 𝐹 (π‘₯, 𝑒) 𝑑π‘₯, (23) 2 Ξ© 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 βˆ’Ξ” is a selfadjoint operator with a sequence of eigenvalues (counted with multiplicity) 0 < πœ† 1 < πœ† 2 ≀ πœ† 3 ≀ β‹… β‹… β‹… ≀ πœ† 𝑗 ≀ β‹… β‹… β‹… 󳨀→ ∞,

𝜎] (π‘˜) 󳨀→ 0

(20)

where π΅π‘˜ = {𝑒 ∈ π‘Œπ‘˜ : ‖𝑒‖ ≀ π‘Ÿπ‘˜ } and Ξ“π‘˜ := {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

π‘’βˆˆπ‘π‘˜ ,‖𝑒‖=πœŒπ‘˜

(32)

Combining (30) and (31), direct computation shows π›Όπ‘˜ :=

inf

π‘’βˆˆπ‘π‘˜ ,‖𝑒‖=πœŒπ‘˜

πΌπœ† (𝑒) β‰₯

πœŒπ‘˜2 > 0, 4

βˆ€π‘˜ β‰₯ π‘˜1 .

(33)

Step 2. We then verify (26). We claim that for any finite-dimensional subspace 𝐹 βŠ‚ 𝐸, there exists a constant πœ– > 0 such that π‘š ({π‘₯ ∈ Ξ© : |𝑒 (π‘₯)| β‰₯ πœ– ‖𝑒‖}) β‰₯ πœ–,

βˆ€π‘’ ∈ 𝐹 \ {0} .

(34)

Here and in the sequel, π‘š(β‹…) 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‘₯ ∈ Ξ© : 󡄨󡄨󡄨𝑒𝑛 (π‘₯)󡄨󡄨󡄨 β‰₯ 󡄩󡄩󡄩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 βˆ’ ∫ 3 2 Ξ›π‘˜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‘₯ ∈ Ξ© : 󡄨󡄨󡄨V𝑛 (π‘₯)󡄨󡄨󡄨 β‰₯ }) < , 𝑛 𝑛

βˆ€π‘› ∈ 𝑁.

1 1 ≀ ‖𝑒‖2 βˆ’ 3 πœ–π‘˜2 ‖𝑒‖2 π‘š (Ξ›π‘˜π‘’ ) 2 πœ–π‘˜

(36)

1 ≀ ‖𝑒‖2 βˆ’ ‖𝑒‖2 2

Passing to a subsequence if necessary, we may assume V𝑛 β†’ 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 βˆ’ V0 󡄨󡄨󡄨 𝑑π‘₯ 󳨀→ 0 as 𝑛 󳨀→ ∞, Ξ©

(37)

and |V0 |∞ > 0. By the definition of norm | β‹… |∞ , there exists a constant 𝛿0 > 0 such that 󡄨 󡄨 π‘š ({π‘₯ ∈ Ξ© : 󡄨󡄨󡄨V0 (π‘₯)󡄨󡄨󡄨 β‰₯ 𝛿0 }) β‰₯ 𝛿0 . (38) For any 𝑛 ∈ 𝑁, let 󡄨 1 󡄨 Ξ› 𝑛 = {π‘₯ ∈ Ξ© : 󡄨󡄨󡄨V𝑛 (π‘₯)󡄨󡄨󡄨 < } , 𝑛 Λ𝑐𝑛

󡄨 1 󡄨 = Ξ© \ Ξ› 𝑛 = {π‘₯ ∈ Ξ© : 󡄨󡄨󡄨V𝑛 (π‘₯)󡄨󡄨󡄨 β‰₯ } . 𝑛

(39)

π‘š (Ξ› 𝑛 ∩ Ξ› 0 ) = π‘š (Ξ› 0 \ Λ𝑐𝑛 ) 1 𝛿0 β‰₯ . 𝑛 2

(40)

Consequently, for 𝑛 large enough, there holds 󡄨 󡄨 ∫ 󡄨󡄨󡄨V𝑛 βˆ’ V0 󡄨󡄨󡄨 𝑑π‘₯ β‰₯ ∫ Ξ©

Ξ› 𝑛 βˆ©Ξ› 0

β‰₯∫

Ξ› 𝑛 βˆ©Ξ› 0

β‰₯

βˆ€ |𝑒| β‰₯ π‘†π‘˜ .

then (44) implies π›½π‘˜ (πœ†) :=

max πΌπœ† (𝑒) ≀ βˆ’

π‘’βˆˆπ‘Œπ‘˜ ,‖𝑒‖=π‘Ÿπ‘˜

π‘Ÿπ‘˜2 < 0, 2

βˆ€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† (βˆ’π‘’) = πΌπœ† (𝑒) for all (πœ†, 𝑒) ∈ [1, 2] Γ— 𝐸. Thus the condition (𝐹1 ) of Theorem 7 holds. Besides, 𝐴(𝑒) = (1/2)‖𝑒‖2 β†’ ∞ as ‖𝑒‖ β†’ ∞ and 𝐡(𝑒) β‰₯ 0 since 𝐹(π‘₯, 𝑒) β‰₯ 0. Thus the condition (𝐹2 ) of Theorem 7 holds. And Lemma 8 shows that the condition (𝐹3 ) holds for all π‘˜ β‰₯ π‘˜1 . Therefore, by Theorem 7, for any π‘˜ β‰₯ π‘˜1 and a.e. πœ† ∈ [1, 2], there exists ∞ π‘˜ (πœ†)}π‘š=1 βŠ‚ 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„ŽβˆˆΞ“π‘˜ π‘’βˆˆπ΅π‘˜

(47)

βˆ€πœ† ∈ [1, 2] ,

(48)

with π΅π‘˜ = {𝑒 ∈ π‘Œπ‘˜ : ‖𝑒‖ ≀ π‘Ÿπ‘˜ } and Ξ“π‘˜ := {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 Ξ›π‘˜π‘’ := {π‘₯ ∈ Ξ© : |𝑒(π‘₯)| β‰₯ 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 β†’ ∞, 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) β‰₯

π‘†π‘˜ }, πœ–π‘˜

π‘˜ πΌπœ† (π‘’π‘š (πœ†)) 󳨀→ πœπ‘˜ (πœ†)

󡄨 󡄨 󡄨 󡄨 (󡄨󡄨󡄨V0 󡄨󡄨󡄨 βˆ’ 󡄨󡄨󡄨V𝑛 󡄨󡄨󡄨) 𝑑π‘₯

βˆ€π‘’ ∈ π‘Œπ‘˜ \ {0} ,

π‘Ÿπ‘˜ > max {πœŒπ‘˜ ,

π‘š

𝛿02 > 0. 4

π‘š (Ξ›π‘˜π‘’ ) β‰₯ πœ–π‘˜ ,

with ‖𝑒‖ β‰₯ 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 βˆ’ V0 󡄨󡄨󡄨 𝑑π‘₯

1 β‰₯ (𝛿0 βˆ’ ) π‘š (Ξ› 𝑛 ∩ Ξ› 0 ) 𝑛

1 = βˆ’ ‖𝑒‖2 2

ending the proof.

Set Ξ› 0 = {π‘₯ ∈ Ξ© : |V0 (π‘₯)| β‰₯ 𝛿0 }. Then for 𝑛 large enough, by (36) and (38), we have

β‰₯ π‘š (Ξ› 0 ) βˆ’ π‘š (Λ𝑐𝑛 ) β‰₯ 𝛿0 βˆ’

(44)

(43)

πœπ‘˜ (πœ†) ∈ [π›Όπ‘˜ , πœπ‘˜ ] ,

βˆ€π‘˜ β‰₯ π‘˜1 ,

(49)

where πœπ‘˜ := maxπ‘’βˆˆπ΅π‘˜ πΌπœ† (𝑒) and π›Όπ‘˜ := πœŒπ‘˜2 /4 β†’ ∞ as π‘˜ β†’ ∞ by (32). ∞

π‘˜ Claim 1. {π‘’π‘š (πœ†)}π‘š=1 βŠ‚ 𝐸 possesses a strong convergent subsequence in 𝐸, for βˆ€πœ† ∈ [1, 2] and π‘˜ β‰₯ 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 β†’ ∞, 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 Ξ© =ΜΈ = {π‘₯ ∈ Ξ© : V(π‘₯) =ΜΈ 0}. If π‘₯ ∈ Ξ© =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]/(]βˆ’1) .

(52)

Observe that σ΅„©σ΅„©σ΅„©π‘’π‘˜ (πœ†) βˆ’ π‘’π‘˜ (πœ†)σ΅„©σ΅„©σ΅„©2 σ΅„©σ΅„© σ΅„©σ΅„© π‘š

Ξ©

π‘˜ (𝑓 (π‘₯, π‘’π‘š

π‘˜

(53)

(πœ†)) βˆ’ 𝑓 (π‘₯, 𝑒 (πœ†)))

∫

𝐹 (π‘₯, 𝑒𝑛 (π‘₯)) 𝑒𝑛 (π‘₯)2

as π‘š 󳨀→ ∞.

Ξ©

π‘›β†’βˆž

< lim sup

󡄨 󡄨 π‘˜ ≀ 󡄨󡄨󡄨󡄨𝑓 (π‘₯, π‘’π‘š (πœ†)) βˆ’ 𝑓 (π‘₯, π‘’π‘˜ (πœ†))󡄨󡄨󡄨󡄨]/(]βˆ’1)

as π‘š β†’ ∞. Thus by (53), (54), and (55), we have proved that σ΅„©σ΅„©σ΅„©π‘’π‘˜ (πœ†) βˆ’ 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†) β†’ π‘’π‘˜ (πœ†) in 𝐸. Thus, for each π‘˜ β‰₯ π‘˜1 , we can choose πœ† 𝑛 β†’ 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‘˜ ] ,

βˆ€π‘› ∈ 𝑁, π‘˜ β‰₯ π‘˜1 . (58)

∞

Claim 2. {π‘’π‘›π‘˜ }𝑛=1 is bounded in 𝐸 for all π‘˜ β‰₯ 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] (Ξ©) ,

V𝑛 (π‘₯) 󳨀→ V (π‘₯)

a.e. in Ξ©.

(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‘˜ β‰₯ π‘˜1 . In fact, by Claim 2, without loss of generality, we have assume π‘’π‘›π‘˜ ⇀ π‘’π‘˜

(55)

in 𝐸, βˆ€π‘› ∈ 𝑁, π‘˜ β‰₯ π‘˜1 .

𝑏 (𝑒𝑛2 + 1)

π‘›β†’βˆž

󡄨 󡄨󡄨 σ΅„¨σ΅„¨βˆ« (𝑓 (π‘₯, π‘’π‘˜ (πœ†)) βˆ’ 𝑓 (π‘₯, π‘’π‘˜ (πœ†))) (π‘’π‘˜ (πœ†) βˆ’ π‘’π‘˜ (πœ†)) 𝑑π‘₯󡄨󡄨󡄨 󡄨󡄨 󡄨󡄨 π‘š π‘š 󡄨 󡄨 Ξ© 󡄨 󡄨 π‘˜ Γ— σ΅„¨σ΅„¨σ΅„¨σ΅„¨π‘’π‘š (πœ†) βˆ’ π‘’π‘˜ (πœ†)󡄨󡄨󡄨󡄨] 󳨀→ 0

(1/2) 𝑓 (π‘₯, 𝑒𝑛 ) 𝑒𝑛 βˆ’ 𝐹 (π‘₯, 𝑒𝑛 ) 2 V𝑛 𝑒𝑛2

(54)

It follows from the H¨older inequality, (51), and (52) that

V𝑛 󳨀→ V

(61)

By (𝑆3 ),

π‘˜ π‘˜ (πΌπœ†σΈ€  (π‘’π‘š (πœ†)) βˆ’ πΌπœ†σΈ€  (π‘’π‘˜ (πœ†)) , π‘’π‘š (πœ†) βˆ’ π‘’π‘˜ (πœ†)) 󳨀→ 0

V𝑛 ⇀ V

1 V𝑛 (π‘₯)2 = . 2

πΌπœ† (𝑒𝑛 ) (1/2) 𝑓 (π‘₯, 𝑒𝑛 ) 𝑒𝑛 βˆ’ 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 Ξ© =ΜΈ has zero measure and V ≑ 0 a.e. in Ξ©. 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‘˜ Γ— (π‘’π‘š (πœ†) βˆ’ π‘’π‘˜ (πœ†)) 𝑑π‘₯.

lim π‘’π‘˜ π‘šβ†’βˆž π‘š

2

π‘›β†’βˆž Ξ©

π‘˜ π‘˜ = (πΌπœ†σΈ€  (π‘’π‘š (πœ†)) βˆ’ πΌπœ†σΈ€  (π‘’π‘˜ (πœ†)) , π‘’π‘š (πœ†) βˆ’ π‘’π‘˜ (πœ†))

+ πœ†βˆ«

𝐹 (π‘₯, 𝑒𝑛 (π‘₯))

π‘›β†’βˆž

as 𝑛 󳨀→ ∞.

(64)

By virtue of the Riesz Representation theorem, πΌπœ†σΈ€  : 𝐸 󳨃→ πΈβˆ— and Ξ¨σΈ€  : 𝐸 󳨃→ πΈβˆ— can be viewed as πΌπœ†σΈ€  : 𝐸 󳨃→ 𝐸 and Ξ¨σΈ€  : 𝐸 󳨃→ 𝐸, respectively, where πΈβˆ— is the dual space of 𝐸. Note that 0 = πΌπœ†σΈ€  𝑛 (π‘’π‘›π‘˜ ) = π‘’π‘›π‘˜ βˆ’ πœ† 𝑛 Ξ¨σΈ€  (π‘’π‘›π‘˜ ) ,

(65)

π‘’π‘›π‘˜ = πœ† 𝑛 Ξ¨σΈ€  (π‘’π‘›π‘˜ ) .

(66)

that is

By Lemma 5, Ξ¨σΈ€  : 𝐸 󳨃→ 𝐸 is also compact. Due to the compactness of Ξ¨σΈ€  and (64), the right-hand side of (66) converges strongly in 𝐸 and hence π‘’π‘›π‘˜ β†’ π‘’π‘˜ in 𝐸. Now for each π‘˜ β‰₯ 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‘˜ β†’ ∞ as π‘˜ β†’ ∞ 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

References [1] D. G. Costa and C. A. Magalh˜aes, β€œVariational elliptic problems which are nonquadratic at infinity,” Nonlinear Analysis. Theory, Methods & Applications, vol. 23, no. 11, pp. 1401–1412, 1994. [2] O. H. Miyagaki and M. A. S. Souto, β€œSuperlinear problems without Ambrosetti and Rabinowitz growth condition,” Journal of Differential Equations, vol. 245, no. 12, pp. 3628–3638, 2008. [3] W. Zou, β€œVariant fountain theorems and their applications,” Manuscripta Mathematica, vol. 104, no. 3, pp. 343–358, 2001. [4] T. Bartsch, β€œInfinitely many solutions of a symmetric Dirichlet problem,” Nonlinear Analysis. Theory, Methods & Applications, vol. 20, no. 10, pp. 1205–1216, 1993. [5] T. Bartsch and M. Willem, β€œOn an elliptic equation with concave and convex nonlinearities,” Proceedings of the American Mathematical Society, vol. 123, no. 11, pp. 3555–3561, 1995. [6] P. H. Rabinowitz, J. Su, and Z.-Q. Wang, β€œMultiple solutions of superlinear elliptic equations,” Rendiconti Lincei. Serie IX. Matematica e Applicazioni, vol. 18, no. 1, pp. 97–108, 2007. [7] L. Jeanjean, β€œOn the existence of bounded Palais-Smale sequences and application to a Landesman-Lazer-type problem set on R𝑁 ,” Proceedings of the Royal Society of Edinburgh A, vol. 129, no. 4, pp. 787–809, 1999. [8] Y. Ding and C. Lee, β€œMultiple solutions of SchrΒ¨odinger equations with indefinite linear part and super or asymptotically linear terms,” Journal of Differential Equations, vol. 222, no. 1, pp. 137–163, 2006. [9] H.-S. Zhou, β€œPositive solution for a semilinear elliptic equation which is almost linear at infinity,” Zeitschrift fΒ¨ur Angewandte Mathematik und Physik, vol. 49, no. 6, pp. 896–906, 1998. [10] M. Schechter, β€œSuperlinear elliptic boundary value problems,” Manuscripta Mathematica, vol. 86, no. 3, pp. 253–265, 1995. [11] A. Ambrosetti and P. H. Rabinowitz, β€œDual variational methods in critical point theory and applications,” Journal of Functional Analysis, vol. 14, pp. 349–381, 1973. [12] M. Willem and W. Zou, On a Semilinear Dirichlet Problem and a Nonlinear SchrΒ¨odinger Equation with Periodic Potential, vol. 305 of SΒ΄eminaire de MathΒ΄ematique, UniversitΒ΄e Catholique de Louvain, 2000. [13] M. Schechter and W. Zou, β€œSuperlinear problems,” Pacific Journal of Mathematics, vol. 214, no. 1, pp. 145–160, 2004. [14] Q. Y. Zhang and C. G. Liu, β€œInfinitely many periodic solutions for second order Hamiltonian systems,” Journal of Differential Equations, vol. 251, no. 4-5, pp. 816–833, 2011. [15] V. Benci and P. H. Rabinowitz, β€œCritical point theorems for indefinite functionals,” Inventiones Mathematicae, vol. 52, no. 3, pp. 241–273, 1979. [16] P. H. Rabinowitz, Minimax Methods in Critical Point Theory with Applications to Differential Equations, CBMS, 1986. [17] M. Willem, Minimax Theorems, BirkhΒ¨auser, Boston, Mass, USA, 1996.

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