• 検索結果がありません。

A Class of p-q-Laplacian Type Equation with Potentials Eigenvalue Problem in R

N/A
N/A
Protected

Academic year: 2022

シェア "A Class of p-q-Laplacian Type Equation with Potentials Eigenvalue Problem in R"

Copied!
19
0
0

読み込み中.... (全文を見る)

全文

(1)

Volume 2009, Article ID 185319,19pages doi:10.1155/2009/185319

Research Article

A Class of p-q-Laplacian Type Equation with Potentials Eigenvalue Problem in R

N

Mingzhu Wu

1

and Zuodong Yang

1, 2

1School of Mathematics Science, Institute of Mathematics, Nanjing Normal University, Jiangsu, Nanjing 210097, China

2College of Zhongbei, Nanjing Normal University, Jiangsu, Nanjing 210046, China

Correspondence should be addressed to Zuodong Yang,zdyang [email protected] Received 20 October 2009; Accepted 6 December 2009

Recommended by Wenming Zou

The nonlinear elliptic eigenvalue problem −div|∇u|p−2∇u −div|∇u|q−2∇u λax|u|p−2u λbx|u|q−2ufx, u, uW1,pW1,qRN, where 2≤qp < NandaxLN/pRN, bx∈ LN/qRN, ax, bx > 0 are studied. The key ingredient is a special constrained minimization method.

Copyrightq2009 M. Wu and Z. Yang. 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.

1. Introduction

In this paper, we are interested in finding nontrivial weak solutions for the nonlinear eigenvalue problem

−div

|∇u|p−2∇u

−div

|∇u|q−2∇u

ax|u|p−2ubx|u|q−2ufx, u, uW1,pW1,q

RN

, u /0,

1.1

where 2 ≤ qp < N and axLN/pRN, bxLN/qRN, ax, bx > 0, infax,infbx/0,fx, usatisfy the following conditions:

AfCRN×R,R, limt→0fx, t/|t|p−1 0,and lim|t| → ∞fx, t/|t|p−1p2/N 0 uniformly inxRN,

Blim|x| → ∞fx, t ftuniformly fortin bounded subsets ofR.

(2)

Remark 1.1. We can see ifaxLN/pRN, bxLN/qRN, then

RNax|u|pdx <

RNaxN/p

1−p/p

RNup p/p

<∞,

RNbx|u|qdx <

RNbxN/q

1−q/q

RNuq q/q

<∞,

1.2

wherepNp/NpandqNq/Nq.

Problem1.1comes, for example, from a general reaction-diffusion system:

utdivDu∇u cx, u, 1.3

whereDu |∇u|p−2|∇u|q−2. This system has a wide range of applications in physics and related sciences such as biophysics, plasma physics, and chemical reaction design. In such applications, the functionudescribes a concentration, the first term on the right-hand side of 1.3corresponds to the diffusion with a diffusion coefficientDu; whereas the second one is the reaction and relates to source and loss processes. Typically, in chemical and biological applications, the reaction termcx, uis a polynomial ofuwith variable coefficients.

When p q 2, problem1.1is a normal Schrodinger equation which has been extensively studied, for example,1–8. The authors used many different methods to study the equation. In8, the authors established some embedding results of weighted Sobolev spaces of radially symmetric functions which are used to obtain ground state solutions. In 6, the authors studied the equation depending upon the local behavior ofV near its global minimum. In3, the authors used spectral properties of the Schrodinger operator to study nonlinear Schrodinger equations with steep potential well. In9, the author imposed on functionskandKconditions ensuring that this problem can be written in a variational form.

We know thatW1,pRNis not a Hilbert space for 1 < p < N, except for p 2. The space W1,pRNwithp /2 does not satisfy the Lieb lemmae.g., see9. AndRNresults in the loss of compactness. So there are many difficulties to study equation1.1ofpq /2 by the usual methods. There seems to be little work on the casep q /2 for problem1.1, to the best of our knowledge. In this paper, we overcome these difficulties and study1.1ofpq≥2.

Recently, whenp q, ax bx,andfx, u 0 then the problem is the following eigenvalue problem has been studied by many authors:

−div

|∇u|p−2∇u

Vx|u|p−2u,

uD1,p0 Ω, u /0, 1.4

whereΩ ⊆RN. We can see10–13. In13, Szulkin and Willem generalized several earlier results concerning the existence of an infinite sequence of eigenvalues.

(3)

Whenp qandax, bxis constant then the problem is the following quasilinear elliptic equation:

−div

|∇u|p−2∇u

λ|u|p−2ufx, u, inΩ,

uW01,pΩ, u /0, 1.5

where 1< p < N, N≥3,λis a parameter,Ωis an unbounded domain inRN. There are many results about it we can see14–18. Because of the unboundedness of the domain, the Sobolev compact embedding does not hold. There are many methods to overcome the difficulty. In 15, the authors used the concentration-compactness principle posed by P. L. Lions and the mountain pass lemma to solve problem1.5. In17,18, the authors studied the problem in symmetric Sobolev spaces which possess Sobolev compact embedding. By the result and a min-max procedure formulated by Bahri and Li16, they considered the existence of positive solutions of

−div

|∇u|p−2∇u

up−1qxuα inRN, 1.6

where qxsatisfies some conditions. We can see if λ is function, then it cannot easily be proved by the above methods.

Whenax, bxis positive constant, He and Li used the mountain pass theorem and concentration-compactness principle to study the following elliptic problem in19:

−div

|∇u|p−2∇u

−div

|∇u|q−2∇u

m|u|p−2un|u|q−2ufx, u inRN, uW1,pW1,q

RN

, 1.7

wherem, n > 0, N ≥ 3,and 1 < q < p < N,fx, u/up−1 tends to a positive constantl as u → ∞. The authors prove in this paper that the problem possesses a nontrivial solution even if the nonlinearityfx, tdoes not satisfy the Ambrosetti-Rabinowitz condition.

In20, Li and Liang used the mountain pass theorem to study the following elliptic problem:

−div

|∇u|p−2∇u

−div

|∇u|q−2∇u

|u|p−2u|u|q−2ufx, u inRN, uW1,pW1,q

RN

, 1.8

where 1< q < p < N. They generalized a similar result forp-Laplacian type equation in15.

It is our purpose in this paper to study the existence of ground state to the problem 1.1inRN. We call any minimizer a ground state for1.1. We inspired by9,16,21try to use constrained minimization method to study problem1.1. Let us point out that although the idea was used before for other problems, the adaptation to the procedure to our problem is not trivial at all. But since bothp- andq-Laplacian operators are involved, careful analysis is needed. A typical difficulty for problem1.1inRNis the lack of compactness of the Sobolev imbedding due to the invariance ofRN under the translations and rotations. However, our method has essential difference with the methods used in 19,20. In order to obtain the

(4)

results, we have to overcome two main difficulties; one is that RN results in the loss of compactness; the other is thatW1,pRN is not a Hilbert space for 1 < p < N and it does not satisfy the Lieb lemma, except forp2.

The paper is organized as follows. InSection 2, we state some condition and many lemmas which we need in the proof of the main theorem. InSection 3, we give the proof of the main result of the paper.

2. Preliminaries

Let

Fx, t t

0

fx, sds, Ft t

0

fsds 2.1

and we define variational functionalsI:W1,p∩W1,qRNRandI:W1,p∩W1,qRNR by

Iu 1 p

RN|∇u|pdx1 q

RN|∇u|qdx

RNFx, udx, Iu 1

p

RN|∇u|pdx1 q

RN|∇u|qdx

RNFudx.

2.2

Solutions to problem1.1will be found as minimizers of the variational problem

Iλinf Iu;uW1,p RN

,

RNax|u|pbx|u|qdxλ

, λ >0. Iλ

To find a solution of problemIλwe introduce thelimitvariational problem

Iλinf Iu;uW1,p RN

,

RNax|u|pbx|u|qdxλ

, λ >0. Iλ

Lemma 2.1. LetunW01,pΩa bounded sequence andp2. Going if necessary to a subsequence, one may assume thatun uinW01,pΩ,unualmost everywhere, whereΩ ⊆ RNis an open subset.

Then,

nlim→ ∞

Ω|∇un|pdx≥ lim

n→ ∞

Ω|∇un− ∇u|pdx lim

n→ ∞

Ω|∇u|pdx. 2.3

(5)

Proof. Whenp2 from Brezis-Lieb lemmasee21, Lemma 1.32we have

n→ ∞lim

Ω|∇un|2dx lim

n→ ∞

Ω|∇un− ∇u|2dx lim

n→ ∞

Ω|∇u|2dx, 2.4 when 3 ≥ p > 2, using the lower semicontinuity of theLp-norm with respect to the weak convergence andun uinW1,pΩ, we deduce

|∇un|p−2∇un,∇un

|∇u|p−2∇u,∇u o1,

nlim→ ∞

|∇un− ∇u|p−2∇un,∇un

≥ lim

n→ ∞

|∇un− ∇u|p−2∇un,∇u

lim

n→ ∞

|∇un− ∇u|p−2∇u,∇un

lim

n→ ∞

|∇un− ∇u|p−2∇u,∇u .

2.5

Then,

nlim→ ∞

Ω

|∇un|p− |∇u|p dx lim

n→ ∞

Ω|∇un|p−2

|∇un|2− |∇u|2

dx lim

n→ ∞

Ω

|∇un|p−2− |∇u|p−2

|∇u|2dx lim

n→ ∞

Ω

|∇un|p−2|∇u|p−2

|∇un|2− |∇u|2 dx lim

n→ ∞

Ω

|∇un|p−2|∇u|2− |∇u|p−2|∇un|2 dx.

2.6

Fromun uinW1,pΩ,

nlim→ ∞

Ω

|∇un|p−2|∇u|2− |∇u|p−2|∇un|2

dx0. 2.7

So

nlim→ ∞

Ω

|∇un|p− |∇u|p

dx lim

n→ ∞

Ω

|∇un|p−2|∇u|p−2

|∇un|2− |∇u|2 dx

≥ lim

n→ ∞

Ω|∇un− ∇u|p−2

|∇un|2− |∇u|2 .

2.8

(6)

So we have

|∇un|p−2∇un,∇un

|∇un− ∇u|p−2∇u,∇un

|∇un− ∇u|p−2∇un,∇u

|∇un− ∇u|p−2∇un,∇un

|∇un− ∇u|p−2∇u,∇u

|∇u|p−2∇u,∇u

o1. 2.9

Then,

|∇un|p−2∇un,∇un

|∇un− ∇u|p−2∇un− ∇u,∇un− ∇u

|∇u|p−2∇u,∇u o1

nlim→ ∞

Ω|∇un|pdx≥ lim

n→ ∞

Ω|∇un− ∇u|pdx lim

n→ ∞

Ω|∇u|pdx,

2.10 whenp >3, there exists akNthat 0< pk≤1. Then, we only need to prove the following inequality:

nlim→ ∞

Ω

|∇un|p− |∇u|p

dx≥ lim

n→ ∞

Ω|∇un− ∇u|p−k

|∇un|k− |∇u|k

. 2.11

The proof of it is similar to the above, so we omit it here. So, the lemma is proved.

Lemma 2.2. Let{un}be a bounded sequence inW1,pRNsuch that

nlim→ ∞sup

y∈RN

By,Ruqndx0, pq < p 2.12 for someR >0. Thenun0 inLsRNforp < s < p, wherepNp/Np.

Proof. We consider the caseN ≥ 3. Letq < s < p anduW1,pRN. Holder and Sobolev inequalities imply that

|u|LsBy,R≤ |u|1−λLqBy,R|u|λLpBy,R

C|u|1−λLqBy,R

By,R

|u|p|∇u|pλ/p ,

2.13

whereλ s−q/pqp/s. Choosingλp/s, we obtain

By,R|u|sCs|u|1−λsLqBy,R

By,R

|u|p|∇u|p

. 2.14

(7)

Now, coveringRNby balls of radiusr, in such a way that each point ofRNis contained in at mostN1 balls, we find

RN|u|s≤N1Cssup

y∈RN

By,R|u|q

1−λs/q

By,R

|u|p|∇u|p

. 2.15

Under the assumption of the lemma,un → 0 inLsRN, p < s < p. The proof is complete.

Corollary 2.3. Let{um}be a sequence inW1,pRNsatisfying 0< ρ

RN|um|pdxand such that um 0 inW1,pRN. Then there exist a sequence{ym} ⊂ RN and a function 0/uW1,pRN such that up to a subsequenceum·ym uinW1,pRN.

Lemma 2.4. LetfCRN×Rand suppose that

|s| → ∞lim fx, s

|s|p−1 0 2.16

uniformly inxRNand

fx, s≤C

|s|p−1|s|p−1

2.17

for allxRNandtR. Ifum u0inW1,pRNandumu0a.e. onRN, then

mlim→ ∞

RNFx, umdx−

RNFx, u0dx−

RNFx, umu0dx

0, 2.18

whereFx, u u

0fx, tdt.

Proof. LetR >0. Applying the mean value theorem we have

RNFx, umdx

|x|≤RFx, umdx

|x|≥RFx, u0 umu0dx

|x|≤RFx, umdx

|x|≥R

Fx, umu0 fx, θu0 umu0u0

dx, 2.19

(8)

whereθdepends onxandRand satisfies 0< θ <1. We now write

RNFx, umdx−

RNFx, u0dx−

RNFx, umu0dx

|x|≤RFx, umFx, u0dx

|x|≥RFx, u0dx

|x|≤RFx, umu0dx

|x|≥Rfx, θu0 umu0u0dx .

2.20

For each fixedR >0

mlim→ ∞

|x|≤RFx, umFx, u0dx0,

m→ ∞lim

|x|≤RFx, umu0dx0.

2.21

Applying2.20and the Holder inequality we get that

|x|≥Rfx, θu0 umu0u0dx

C

|x|≥R

|θu0 umu0|p−1|u0||θu0 umu0|p−1|u0| dx

C

|x|≥R|u0|p

1/p

|x|≥R|θu0 umu0|p

p−1/p

C

|x|≥R|u0|p

1/p

|x|≥R|θu0 umu0|p

p−1/p .

2.22

Since{um}is bounded inW1,pRNwe see that

Rlim→ ∞

|x|≥Rfx, θu0 umu0u0dx

0. 2.23

The result follows from2.21and2.23.

Lemma 2.5. FunctionsIλandIλare continuous on0,∞and minimizing sequences for problems IλandIλare bounded inW1,pRN.

(9)

Proof. From conditionA, we observe that for eachε >0 there existsCε>0 such that Fu,|Fx, u| ≤ε

RN|u|pdxε

RN|u|pp2/NdxCε

RN|u|αdx, 2.24 wherep < α < pp2/Nandε >0.

By the Holder and Sobolev inequalities we have

RN|u|pp2/Ndx

RN|u|pp−p−p2/N/p−ppp2/N/p−pdx

RN|u|p

p−p−p2/N/p−p

RN|u|p

p2/N/p−p

S−1

RN|u|p p/N

RN|∇u|pdx,

2.25

where|u|ppS−1|∇u|pp. Similarly we have

RN|u|αdx

RN|u|pp−α/p−ppα−p/p−pdx

RN|u|pdx

p−α/p−p

RN|u|pdx

α−p/p−p

S−pα−p/pp−p

RN|u|pdx

p−α/p−p

RN|∇u|pdx

pα−p/pp−p .

2.26

Consequently by the Young inequality we have

RN|u|αdxη

RN|∇u|pdxK

η

RN|u|αdx

pp−α/p2p−p2−pα

2.27

forη >0, whereKη>0 is a constant.

BecauseuW1,pW1,qRNso we can by Sobolev embedding andλ

RNax|u|p bx|u|qdxlettingλ

RN|u|pdx <∞, we derive the following estimates forIuandIu:

Iu, Iu≥ 1

pεS−1λp/NCεη

RN|∇u|pdx 1

q

RN|∇u|qdxελK η

Cελpp−α/p2p−p2−pα.

2.28

(10)

Choosingε >0 andη >0 so that 1

pεS−1λp/NCεη >0, 2.29

we see thatIλandIλ are finite and moreover minimizing sequences for problemsIλand Iλare bounded. It is easy to check thatIλandIλare continuous on0,∞.

We observe thatIμ≤0 for allμ >0. Indeed, letuC0RNand

RNax ux/σ

σN/q

pdx

RNbx ux/σ

σN/q

qdxμ, 2.30

then for eachσ >0 we have

Iμ≤ 1 pp/q−1N

RN|∇u|pdx 1 q

RN|∇u|qdxσN

RNF

σ−N/qu

dx−→0 2.31

asσ → ∞.

Lemma 2.6. Suppose that Iλ < 0 for some λ > 0, thenIμ is nonincreasing on 0,∞ and limμ→0Iμ/μ 0. Moreover there existsλλsuch that

Iμ μ > Iλ

λ forμ∈0, λ. 2.32

Proof. We observe that

inf Iu

RNax|u|pbx|u|qdx

inf I u

x/σ1/N

RNa

x/σ1/Nu

x/σ1/Npdxb

x/σ1/Nu

x/σ1/Nqdx.

2.33

So if

RNax|u|p bx|u|qdx k and

RNax/σ1/N|ux/σ1/N|pdx bx/σ1/N|ux/

σ1/N|qdxkthenIux Iux/σ1/N Ik. We have that ifσ >0 andα >0 with

RNax|u|pbx|u|qdxα, then

RNa x

σ1/N u

x σ1/N

pdxb x

σ1/N u

x σ1/N

qdxσα, I

u x

σ1/N

Iσα. 2.34

(11)

Consequently, for allα1>0 andα2>0 we have

Iα1 inf 1

p α1

α2

N−p/N

RN|∇u|pdx1 q

α1

α2

N−q/N

RN|∇u|qdxα1

α2

RNFudx;

RNax|u|pbx|u|qdxα2

.

2.35

If 0< α1 < α2, then for eachε >0 there existsuW1,pW1,qRNwith

RNax|u|p bx|u|qdxα2such that

Iα1ε > 1 p

α1

α2

N−p/N

RN|∇u|pdx1 q

α1

α2

N−q/N

RN|∇u|qdxα1

α2

RNFudx

α1

α2

1 p

RN|∇u|pdx1 q

RN|∇u|qdx

RNFudx

α1

α2Iα2.

2.36

This inequality yields

Iα1 α1 > Iα2

α2. 2.37

SinceIμ≤0 for allμ >0, we see that

μlim0

Iμ

μ c≤0. 2.38

We claim thatc0. Indeed, it follows from2.36and from the estimate obtained in the Lemma 2.1that for every 0< μ < λthere exists anuμW1,pW1,qRN, with

RNax|uμ|p bx|uμ|qdxλsuch that

Iμμ2> 1 p

μ λ

N−p/N

RN

∇uμpdx1 q

μ λ

N−q/N

RN

∇uμqdxμ λ

RNF uμ

dx

μ λ

1 p

RN

∇uμpdx1 q

RN

∇uμqdx

RNF uμ

dx

μ λ

C1λ

RN

∇uμpdxC2λ

RN

∇uμqdxC3λ

,

2.39

whereC1λ>0, C2λ>0,andC3λ>0 are constants. Hence

μ2μ λ

C1λ

RN

∇uμpdxC2λ

RN

∇uμqdxC3λ

, 2.40

(12)

that is,

RN|∇uμ|pdxC4λ,

RN|∇uμ|pdxC5λ for some constant C4λ, C5λ > 0 independent ofμ. We see that there existsε0>0 and a sequenceμn → 0 such that

RN

∇uμnpdxε0,

RN

∇uμnqdxε0. 2.41 If

RN|∇uμn|pdxε0then

RN|∇uμn|qdxη≥0.

Then, using the fact that

RNFuμndx≤Cfor some constantC >0, we get Iμn

μn μn≥ 1

−N−p/Nμn−p/Nε01

−N−q/Nμn−q/NηC

λ −→ ∞ 2.42

asμn → 0 and this contradicts the fact that limμ0Iμ/μ c≤0. Therefore

μlim0

RN

∇uμpdx0, lim

μ0Iμ0, 2.43

when

RN|∇uμn|pdxε0>0 we can use the same method to obtain that limμ→0

RN|∇uμ|qdx 0.

So

μ→lim0

RN

∇uμpdx lim

μ→0

RN

∇uμqdx0, lim

μ0Iμ0, 2.44 this implies that limμ0

RNFuμdx0 and consequently Iμ

μ μ≥ −1 λ

RN

F uμ

dx−→0. 2.45

This shows that limμ0Iμ 0. Finally, we observe that limμ→0Iμ 0 > Iλ which obtain2.32.

3. Proof of Main Theorems

Theorem 3.1. Suppose thatIλ <0 for someλ >0, then there exists 0< α0λsuch that problem Iα0has a minimizer. Moreover each minimizing sequence forIα0up to a translation is relatively compact inW1,pW1,qRN.

Proof. According toLemma 2.6the set

α1; Iα α > Iλ

λ for eachα∈0, α1

3.1

(13)

is nonempty. We define

α0sup α1; Iα α > Iλ

λ for eachα∈0, α1

. 3.2

It follows from the continuity ofIλthat

0< α0λ , Iα0 α0

λ Iλ<0, Iα> α

λIλ,

3.3

for all 0< α < α0. This yields Iα0 α0

λ Iλ α0α λ Iλ α

λIλ< Iα0−αIα 3.4 for eachα∈0, α0.

Let{um} ⊂W1,pW1,qRNbe a minimizing sequence forIα0. Since{um}is bounded we may assume thatum uinW1,pW1,qRN,umua.e. onRN. First we consider the caseu ≡ 0. In this case byLemma 2.2um → 0 forq < α < p or Corollary there exists a sequence{um} ⊂RNsuch thatum·ym v /0 inW1,pW1,qRN.

In the first case limm→ ∞

RNFumdx0 and consequently Iα0 lim

m→ ∞Ium lim

m→ ∞

1 p

RN|∇um|pdx1 q

RN|∇um|qdx

RNFumdx

≥0, 3.5

which is impossible. Henceum·ym v /0 inW1,pW1,qRNholds and lettingvmx umxymfrom Brezis-Lieb lemmasee21, Lemma 1.32we have

RNax|um|pbx|um|qdx

RNa xym

|vm|pb xym

|vm|qdx

RNa xym

|v|pb xym

|v|qdx

RNa xym

|vmv|p

b xym

|vmv|qdxo1.

3.6

We now show that

RNa xym

|v|pb xym

|v|qdxα0. 3.7

(14)

In the contrary case fromLemma 2.1we have

0<

RNa xym

|v|pb xym

|v|qdx < α0. 3.8

By3.21we have

m→ ∞lim

RNa xym

|vmv|pb xym

|vmv|qdx−→α0λ,

λ

RNa xym

|v|pb xym

|v|qdx.

3.9

On the other hand, by Lemmas2.1and2.4we have

RNFvmdx

RNFvdx

RNFvmvdxo1,

RN|∇vm|p|∇vm|qdx

RN|∇v|p|∇v|qdx

RN|∇vmv|p|∇vmv|qdxo1, 3.10

and this implies that

Iα0Iv Ivmv o1IλIα0−λ0o1. 3.11 Lettingm → ∞we getIα0IλIα

0−λ0which contradicts3.4. Therefore

RNaxym|v|p bxym|v|qdxα0. It then follows from3.6thatvmvinLp∩LqRN. By the Gagliardo- Nirenberg inequalityvmvinLsRN,qs <∞. Obviously this implies thatIα0 Iv Iv·−ymand

RNax|v·−ym|pbx|v·−ym|qdxα0. To complete the proof we show thatvmvinW1,pW1,qRN. Indeed, we have

Iα0 1 p

RN|∇vm|pdx 1 q

RN|∇vm|qdx

RNFvmdxo1

≥ 1 p

RN|∇v|pdx1 q

RN|∇v|qdx1 p

RN|∇vmv|pdx1 q

RN|∇vmv|qdx

RNFvdx

RN

FvFvm

dxo1.

3.12

Since limm→ ∞

RNFv−Fvmdx0, we deduce from3.12that∇vm → ∇vinLp∩LqRN and hencevmvinW1,pW1,qRN.

Ifu /0, we repeat the previous argument to show thatIα0is attained.

Theorem 3.2. Suppose thatFx, tFtonRN ×R and thatIλ < 0 for someλ > 0, then the infimumIλ0is attained for some 0< λ0λ.

(15)

Proof. SinceFx, tFtonRN×R we haveIμIμforμ≥0. We distinguish two cases:i IλIλ<0,iiIλ< Iλ.

Casei. ByTheorem 3.1there existsλ0∈0, λsuch that Iλ0 Iu,

RNax|u|pbx|u|qdxλ0 for someuW1,pW1,q RN

. 3.13

Thus

Iλ0Iu 1 p

RN|∇u|pdx 1 q

RN|∇u|qdx

RNFx, udx

≤ 1 p

RN|∇u|pdx 1 q

RN|∇u|qdx

RNFudxIu Iλ0.

3.14

IfIλ0 Iλ0, thenI also attains its infimumIλ0 atu. Therefore it remains to consider the case Iλ0< Iλ0. Consequently we need to prove the following claim.

IfIλ < Iλfor someλ >0, then there existsα0 ∈ 0, λsuch that problemIα0has a solution. This obviously completes the proof of caseiand also provides the proof of case ii.

By virtue ofLemma 2.5,IβIλ−β is continuous forβ ∈0, λand alsoI0 I0 0. If Iλ< Iλfor someλ >0, then there existsγ >0 such that

Iλ< IβIλ−β 3.15

for allβ∈0, γ. Let

α0sup

γ; Iλ< IβIλ−β , for 0≤β < γ

. 3.16

Then we have

IλIα0Iλ−α 0, Iλ< IαIλ−α

3.17

for 0≤α < α0. This implies that

Iα0Iλ−α 0 Iλ< Iλ≤0, 3.18 and hence

Iα0 < IλIλ−α 0Iα0 ≤0, 3.19 we show thatIα0 is attained by auW1,pW1,qRNand every minimizing sequence for Iα0is relatively compact inW1,pW1,qRN. Let{um}be a minimizing sequence forIα0. Since

(16)

{um}is bounded, we may assume that um uin W1,pW1,qRN,um u a.e. on RN. Arguing indirectly we assume thatu≡0 onRN. We see that

mlim→ ∞

B0,R|Fx, um|dx lim

m→ ∞

B0,R

Fumdx0 3.20

for eachR >0. We now write

Ium

1 p

RN|∇um|pdx 1 q

RN|∇um|qdx

RNFx, umdx Ium

RN

FumFx, um dx.

3.21

We show that

mlim→ ∞

RN

FumFx, um

dx0. 3.22

Towards this end we write

RN

FumFx, umdx

B0,R|Fx, um|dx

B0,R

Fumdx

|x|≥R,|um|≤δ

|x|≥R,δ≤|um|≤1/δ

|x|≥R,|um|>1/δ

FumFx, um.

3.23

We now define the following quantities:

1δ sup

0<|t|<δ,x∈RN

Ft−Fx, t

|t|p

R sup

δ≤|t|≤1/δ,|x|≥R

Ft−Fx, t,

2δ sup

|t|≥1/δ

Ft−Fx, t

|t|pN/N−p .

3.24

参照

関連したドキュメント

The main results of this paper are complete characterization of Fucik type eigenvalues, their associated eigenfunctions and observations of changes of frequency, amplitude of

Global Existence and Global Nonexistence of Solutions of the Cauchy Problem for a Nonlinearly Damped Wave Equation, Journal of Mathematical Analysis and Applications, 1998, vol..

Existence of solutions for a Kirchhoff type problem involving the fractional p-Laplacian operator.. Wenjing Chen B and

The aim of our article is the existence of bounded weak solutions to the Robin problem for an elliptic quasi-linear second-order equation with the variable p ( x ) -Laplacian in

We establish sufficient conditions for the existence of multiple positive solutions to nonautonomous quasilinear elliptic equations with p(x)- Laplacian and sign-changing

Li, “Multiple solutions and sign-changing solutions of a class of nonlinear elliptic equations with Neumann boundary condition,” Journal of Mathematical Analysis and Applications,

Wei, “Existence of positive solutions for fourth-order m-point boundary value problems with a one-dimensional p-Laplacian operator,” Nonlinear Analysis: Theory, Methods

Yang; The existence of a nontrivial solution to a nonlinear elliptic boundary value problem of p-Laplacian type without the Ambrosetti-Rabinowitz condition, Nonlinear Anal.. (TMA),