• Nem Talált Eredményt

ON THE EXISTENCE OF SOLUTIONS TO A CLASS OF p-LAPLACE ELLIPTIC EQUATIONS

N/A
N/A
Protected

Academic year: 2022

Ossza meg "ON THE EXISTENCE OF SOLUTIONS TO A CLASS OF p-LAPLACE ELLIPTIC EQUATIONS"

Copied!
19
0
0

Teljes szövegt

(1)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page

Contents

JJ II

J I

Page1of 19 Go Back Full Screen

Close

ON THE EXISTENCE OF SOLUTIONS TO A CLASS OF p-LAPLACE ELLIPTIC EQUATIONS

HUI-MEI HE AND JIAN-QING CHEN

Fujian Normal University Fuzhou, 350007 P.R. China

EMail:hehuimei20060670@163.com jqchen@fjnu.edu.cn

Received: 19 September, 2008

Accepted: 07 December, 2008

Communicated by: C. Bandle 2000 AMS Sub. Class.: 35J20.

Key words: p-Laplace elliptic equations, Radial solutions, Nonradial solutions.

Abstract: We study the equation−∆pu+|x|a|u|p−2u = |x|b|u|q−2u with Dirichlet boundary condition onB(0, R)or onRN. We prove the existence of the ra- dial solution and nonradial solutions of this equation.

(2)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page2of 19 Go Back Full Screen

Close

Contents

1 Introduction and Main Result 3

2 Radial Solution 6

3 Nonradial Solutions 12

4 Necessary Conditions 16

(3)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page3of 19 Go Back Full Screen

Close

1. Introduction and Main Result

Equations of the form (1.1)

( −∆tu+g(x)|u|s−2u=f(x, u) inΩ

u= 0, on∂Ω

have attracted much attention. Many papers deal with the problem (1.1) in the case of t= 2, Ω =RN, s= 2, glarge at infinity andf superlinear, subcritical and bounded inx, see e.g. [1], [2] and [4]. The problem (1.1) witht = 2, Ω =B(0,1), g(x) = 0 and f(x, u) = |x|bul−1 was studied in [9]; in particular, it was proved that under some conditions the ground states are not radial symmetric. The caset = 2, Ω = B(0,1) or on RN, g(x) = 1 and f(x, u) = |x|b|u|l−2u was studied in [7]. The problem (1.1) witht =s, Ω =RN, g(x) = V(|x|)andf(x, u) =Q(|x|)|u|l−2uwas studied by J. Su., Z.-Q. Wang and M. Willem ([11], [12]). They proved embedding results for functions in the weightedW1,p(RN)space of radial symmetry. The results were then used to obtain ground state and bound state solutions of equations with unbounded or decaying radial potentials.

In this paper, we consider the nonlinear elliptic problem

(1.2)





−∆pu+|x|a|u|p−2u=|x|b|u|q−2u inΩ u >0, u∈W1,p(Ω),

u= 0, on∂Ω

and prove the existence of the radial and the nonradial solutions of the problem (1.2).

Here, ∆pu = div(|∇u|p−2∇u)is the p-Laplacian operator, and 1 < p < N, a ≥ 0, b≥0.

We denote byWr1,p(RN)the space of radially symmetric functions in W1,p(RN) =

u∈Lp(RN) :∇u∈Lp(RN) .

(4)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page4of 19 Go Back Full Screen

Close

Wr,a1,p(RN)is denoted by the space of radially symmetric functions in Wa1,p(RN) =

u∈W1,p(RN) : Z

RN

|x|a|u|p <∞

. We also denote byDr1,p(RN)the space of radially symmetric functions in

D1,p(RN) = n

u∈LN−pN p RN

:∇u∈Lp RNo . Our main results are:

Theorem 1.1. Ifa ≥0, b≥0, 1< p < N and p < q <q˜= N p

N −p+ bp N −p, pb−a

p+ (p−1)(q−p) p

<(q−p)(N −1), then the problem (1.2) has a radial solution.

Remark 1. In [8], Sirakov proves that the problem (1.2) with p = 2 has a solution for

2< q < q#= 2N

N −2− 4b a(N −2).

In [6], P. Sintzoff and M. Willem proved the existence of a solution of the prob- lem (1.2) with

p= 2, q≤2, 2b−a 1 + q

2

<(N −1)(q−2).

Theorem1.1 extends the results of [6] to the general equation with ap−Laplacian operator.

(5)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page5of 19 Go Back Full Screen

Close

Theorem 1.2. Suppose thata≥0, b≥0, 1< p < N and p < q < N p

N −p, pb−a

p+(p−1)(q−p) p

<(q−p)(N −1), aq < pb,

then for everyR, problem (1.2) withΩ =B(0, R), Rlarge enough has a radial and a nonradial solution.

This paper is organized as follows: In Section 2, we study (1.2) in the case of Ω =RN. We prove the existence of a radial least energy solution of (1.2) when

1< p < N, p < q <q,˜ pb−a

p+(p−1)(q−p) p

<(q−p)(N−1).

In Section 3, we consider the existence of nonradial solutions of (1.2) with Ω = B(0, R), R large enough. Finally, in Section 4, we consider necessary conditions for the existence of solutions of (1.2).

(6)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page6of 19 Go Back Full Screen

Close

2. Radial Solution

In this paper, unless stated otherwise, all integrals are understood to be taken over all ofRN. Also, throughout the paper, we will often denote various constants by the same letter.

Lemma 2.1. Suppose that 1 < p < N. There existAN > 0,such that, for every u∈Wr,a1,p(RN), u ∈C(RN\{0}), fora ≥ p−1p (1−N),we have that

|x|N−1p +

a(p−1)

p2 |u(x)| ≤AN Z

|x|a|u|p p−1

p2 Z

|∇u|p 1

p2

. Proof. Since

d dr

|u|pr

p−1 p rN−1

= p

2 |u|2p2−1

·2u·du drr

p−1 p rN−1 +|u|p

a·p−1

p +N −1

rp−1p −1rN−1, and

a≥ p

p−1(1−N), we get that

d dr

|u|prp−1p rN−1

≥pu|u|p−2du

drrp−1p rN−1 and obtain

rp−1p rN−1|u(r)|p ≤AN Z +∞

r

|u|p−1

du dr

SN−1Sp−1p dS

≤AN Z

|u|p−1

du dr

|x|p−1p dx

(7)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page7of 19 Go Back Full Screen

Close

≤AN Z

|x|a|u|p

p−1p Z

|∇u|p 1p

. It follows that

|x|N−1+a·p−1p |u(x)|p ≤AN

Z

|x|a|u|p

p−1p Z

|∇u|p 1p

, and we have

|x|N−1p +

a(p−1)

p2 |u(x)| ≤AN Z

|x|a|u|p p−1

p2 Z

|∇u|p 1

p2

.

Lemma 2.2. If1 < p < N, p ≤ r < N−ppN , then for anyu ∈ W1,p(RN), we have that

Z

|u|rdx ≤C Z

|∇u|p

N(r−p)

p2 Z

|u|p

N p+r(p−N)

p2

.

Proof. The proof can be adapted directly from the Gagliardo-Nirenberg inequality.

The following inequality extends the results of [5] to the general equation with thep−Laplacian operator.

Lemma 2.3. For

1< p < N, p < q < pN

N −p+ c

N−1

p +a(p−1)p2

, a≥ p

p−1(1−N),

(8)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page8of 19 Go Back Full Screen

Close

there existBN,p,csuch that for everyu∈Dr1,p(RN), we have Z

|x|c|u|qdx ≤BN,p,c Z

|∇u|p

p(N−1)+a(p−1)c +N

p2

q−p−p(N−1)+a(p−1)cp2

. Proof. Using Lemma2.1and Lemma2.2, we have

Z

|x|c|u|qdx

= Z

|x|N−1p +

a(p−1) p2

(N−1)/p+a(p−1)pc −2

|u|

(N−1)/p+a(p−1)pc −2

|u|

q−(N−1)/p+a(p−1)pc −2

dx

≤ Z

|x|a|u|p p−1

p2 · c

(N−1)/p+a(p−1)p−2 Z

|∇u|p 1

p2· c

(N−1)/p+a(p−1)p−2

· Z

|∇u|p N

p2(q−p− c

(N−1)/p+a(p−1)p−2)Z

|u|p N p

p2+p−N

p2

q− c

(N−1)/p+a(p−1)p−2

= Z

|x|a|u|pdx

p(N−1)+a(p−1)c(p−1) Z

|u|p N p

p2+p−N

p2

q−p(N−1)+a(p−1)cp2

· Z

|∇u|p

p(N−1)+a(p−1)c +N

p2

q−p−p(N−1)+a(p−1)cp2

≤BN,p,c Z

|∇u|p

p(N−1)+a(p−1)c +N

p2

q−p−p(N−1)+a(p−1)cp2

.

(9)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page9of 19 Go Back Full Screen

Close

Next, to prove Theorem1.1, we consider the following minimization problem m =m(a, b, p, q) = inf

u∈Wr,a1,p(RN) R|x|b|u|qdx=1

Z

|∇u|p+|x|a|u|p dx.

Theorem 2.4. Ifa ≥0, b≥0, 1< p < N and p < q <q˜= N p

N −p+ bp N −p, pb−a

p+ (p−1)(q−p) p

<(q−p)(N −1), thenm(a, b, p, q)is achieved.

Proof. Let(un)⊂Wr,a1,p(RN)be a minimizing sequence form=m(a, b, p, q) : Z

|x|b|un|qdx= 1, Z

(|∇un|p +|x|a|un|p)dx→m.

By going (if necessary) to a subsequence, we can assume thatun * uinWr,a1,p(RN).

Hence, by weak lower semicontinuity, we have Z

(|∇u|p +|x|a|u|p)dx≤m, Z

|x|b|u|qdx≤1.

(10)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page10of 19 Go Back Full Screen

Close

Ifcis defined byq = NpN−p +N−ppc , thenc < band it follows from Lemma2.3that Z

|x|≤ε

|x|b|un|qdx≤εb−c Z

|x|c|un|qdx≤Cεb−c. Since(un)is bounded inWr,a1,p(RN). We deduce from Lemma2.1that

Z

|x|≥1

ε

|x|b|un|qdx= Z

|x|≥1

ε

|x|b−a|un|q−p|x|a|un|pdx

≤ 1

ε

b−a−(q−p)(N−1p +a(p−1)

p2 )

C Z

|x|a|u|pdx

≤Cεa(

q+1 p q

p2)−b+(q−p)(N−1)p

.

So we get that, for everyt <1, there existsε >0, such that for everyn, Z

ε≤|x|≤1

ε

|x|b|un|qdx≥t.

By the Rellich theorem and Lemma2.1, 1≥

Z

|x|b|un|qdx≥ Z

ε≤|x|≤1ε

|x|b|un|qdx≥t.

FinallyR

|x|b|u|qdx= 1andm =m(a, b, p, q)is achieved atu.

Now we will prove Theorem1.1.

Proof. By Theorem 2.4, m is achieved. Then by the Lagrange multiplier rule, the symmetric criticality principle (see e.g. [13]) and the maximum principle, we obtain

(11)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page11of 19 Go Back Full Screen

Close

a solution of

−∆pυ+|x|a|υ|p−2υ =λ|x|b|υ|q−2υ, υ >0, υ ∈W1,p(RN).

Henceu=λq−p1 υ is a radial solution of (1.2), withλ= pqm.

(12)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page12of 19 Go Back Full Screen

Close

3. Nonradial Solutions

In this section, we will prove Theorem1.2. We use the preceding results to construct nonradial solutions of problem (1.2) in the caseΩ =B(0, R).

Consider

M =M(a, b, p, q) = inf

u∈Wa1,p(RN) R|x|b|u|qdx=1

Z

|∇u|p+|x|a|u|p dx.

It is clear thatM ≤m,and using our previous results, we prove thatM is achieved under some conditions.

Theorem 3.1. Ifa ≥0, b≥0, 1< p < N and p < q < q#= pN

N −p− p2b a(N −p), thenM(a, b, p, q)is achieved.

Proof. Let(un)⊂Wa1,p(RN)be a minimizing sequence forM =M(a, b, p, q) : Z

|x|b|un|qdx= 1, Z

|∇un|p+|x|a|un|p

dx→M.

By going (if necessary) to a subsequence, we can assume thatun * uinWa1,p(RN).

(13)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page13of 19 Go Back Full Screen

Close

Hence, by weak lower semicontinuity, we have Z

|∇u|p+|x|a|u|p

dx≤M, Z

|x|b|u|qdx≤1.

Ifcis defined byq = NpN−pa(N−p)p2c , thenc > band r = a

c, s=

aN p N−p

aq−pc

are conjugate. It follows from the Hölder and Sobolev inequalities that Z

|x|≥1ε

|x|b|un|qdx≤ 1

ε b−cZ

|x|c|un|qdx

= 1

ε b−cZ

|x|c|un|pca|un|q−pcadx

≤εc−b Z

|x|a|un|pdx 1r Z

|un|N−pN p dx 1s

≤Cεc−b.

As in Theorem2.4, for everyt <1, there existsε >0such that, for everyn, Z

|x|≤1ε

|x|b|un|qdx≥t.

By the compactness of the Sobolev theorem in the bounded domain, for 1 < p <

(14)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page14of 19 Go Back Full Screen

Close

N, p < q < NN p−p, 1≥

Z

|x|b|u|qdx≥ Z

|x|≤1ε

|x|b|un|qdx≥t.

HenceR

|x|b|u|qdx= 1andM =M(a, b, p, q)is achieved atu.

Now we will prove Theorem1.2.

Proof. By Theorem2.4,m(a, b, p, q)is positive. Sincepb > aq, it is easy to verify thatM(a, b, p, q) = 0.Let us define

M(a, b, p, q, R) = inf

u∈Wa1,p(B(0,R)) R

B(0,R)|x|b|u|qdx=1

Z

B(0,R)

|∇u|p+|x|a|u|p dx,

m(a, b, p, q, R) = inf

u∈Wr,a1,p(B(0,R)) R

B(0,R)|x|b|u|qdx=1

Z

B(0,R)

|∇u|p+|x|a|u|p dx.

It is clear that, for every R > 0, M(a, b, p, q, R) and m(a, b, p, q, R) are achieved and

R→∞lim M(a, b, p, q, R) =M(a, b, p, q) = 0,

R→∞lim m(a, b, p, q, R) =m(a, b, p, q)>0.

Then from Theorem 1.1, we know that problem (1.2) with B(0, R) has a radial solution.

(15)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page15of 19 Go Back Full Screen

Close

On the other hand, by the Lagrange multiplier rule, the symmetric criticality prin- ciple (see e.g.[13]) and the maximum principle, we obtain a solution of





−∆pυ +|x|a|υ|p−2υ =λ|x|b|υ|q−2υ inB(0, R) υ >0, u∈W1,p(B(0, R)),

υ = 0, on∂B(0, R).

Hence u = λq−p1 υ is a solution of (1.2), with λ = pqM(a, b, p, q, R). Thus, Prob- lem (1.2) has a nonradial solution.

(16)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page16of 19 Go Back Full Screen

Close

4. Necessary Conditions

In this section we obtain a nonexistence result for the solution of problem (1.2) using a Pohozaev-type identity. The Pohozaev identity has been derived for very general problems by H. Egnell [3].

Lemma 4.1. Letu∈W1,p(RN)be a solution of (1.2), thenusatisfies N −p

p Z

|∇u|pdx+ N +a p

Z

|x|a|u|pdx−N +b q

Z

|x|b|u|qdx= 0.

Theorem 4.2. Suppose that

˜

q= N p

N −p+ pb N −p ≤q

or N +a

p ≤ N +b q . Then there is no solution for problem (1.2).

Proof. Multiplying (1.2) byuand integrating, we see that Z

|x|b|u|qdx= Z

|∇u|p+|x|a|u|p dx.

On the other hand, using Lemma4.1, we obtain N −p

p −N +b q

Z

|∇u|pdx+

N +a

p −N +b q

Z

|x|a|u|pdx= 0.

(17)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page17of 19 Go Back Full Screen

Close

So, ifuis a solution of problem (1.2), we must have N −p

p < N +b

q , N +a

p > N +b q .

Remark 2. The second assumption of Theorem2.4,

pb−a

p+(q−p)(p−1) p

<(q−p)(N−1) implies that

N +b

q < N+a p .

(18)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page18of 19 Go Back Full Screen

Close

References

[1] T. BARTSCHAND Z.-Q. WANG, Existence and multiplicity results for some superlinear elliptic problem onRN, Comm. Partial Diff. Eq., 20 (1995), 1725–

1741.

[2] W. OMANAANDM. WILLEM, Homoclinic orbits for a class of Hamiltonian systems, Diff. Int. Eq., 5 (1992), 115–1120.

[3] H. EGNELL, Semilinear elliptic equations involving critical Sobolev expo- nents, Arch. Rat. Mech. Anal., 104 (1988), 27–56.

[4] P.H. RABINOWITZ, On a class of nonlinear Schrödinger equations, Z. Angew.

Math. Phys., 43 (1992), 270–291.

[5] W . ROTHER, Some existence results for the equation −4u+k(x)up = 0, Comm. Partial Differential Eq., 15 (1990), 1461–1473.

[6] P. SINTZOFF AND M. WILLEM, A semilinear elliptic equation on RN with unbounded coefficients, in Variational and Topological Methods in the Study of Nonlinear Phenomena, V. Benci et al. eds., PNLDE Vol. Birkhäuser, Boston, 49 (2002), 105–113.

[7] P. SINTZOFF, Symmetry of solutions of a semilinear elliptic equation with unbound coefficients, Diff. Int. Eq., 7 (2003), 769–786.

[8] B. SIRAKOV, Existence and multiplicity of solutions of semi-linear elliptic equations inRN, Calc. Var. Partial Differential Equations, 11 (2002), 119–142.

[9] D. SMETS, J. SUANDM. WILLEM, Non radial ground states for the Hénon equation, Commun. Contemp. Math., 4 (2002), 467–480.

[10] W.A. STRAUSS, Existence of solitary waves in higher dimensions, Comm.

Math. Phys., 55 (1977), 149–162.

(19)

Radial Solution and Nonradial Solutions Hui-mei He and Jian-qing Chen

vol. 10, iss. 2, art. 59, 2009

Title Page Contents

JJ II

J I

Page19of 19 Go Back Full Screen

Close

[11] J. SU, Z.-Q. WANG AND M. WILLEM, Weighted Sobolev embedding with unbounded decaying radial potentials, J. Differential Equations, 238 (2007), 201–219.

[12] J. SU, Z.-Q. WANGANDM. WILLEM, Nonlinear Schrödinger equations with unbounded and decaying radial potentials, Commun. Contemp. Math., 9(4) (2007), 571–583.

[13] M. WILLEM, Minimax Theorems, Birkhäuser, Boston, 1996.

Hivatkozások

KAPCSOLÓDÓ DOKUMENTUMOK

Agarwal, Double positive solutions of (n, p) boundary value problems for higher order difference equations, Comput. Agarwal, Existence theorems for a system of difference equations

In [6] we considered some nonlinear elliptic functional differential equations where we proved theorems on the number of weak solutions of boundary value problems for such equations

In 2013, Tang [29] gave some much weaker conditions and studied the existence of in- finitely many solutions for Schrödinger equation via symmetric mountain pass theorem

W ei , Existence of infinitely many large solutions for the nonlinear Schrödinger–Maxwell equations, Nonlinear Anal... W ang , Multiplicity for a 4-sublinear Schrödinger–Poisson

Z eddini , On the existence of positive solutions for a class of semilinear elliptic equations, Nonlinear Anal.. D rissi , Large and entire large solutions for a class of

Regularization of radial solutions of p-Laplace equations, and computations using infinite series.. Philip

K ristály , Multiple solutions of a sublinear Schrödinger equation, NoDEA Nonlinear Differential Equations Appl.. S zulkin , An asymptotically periodic Schrödinger equation

At the same time, in the last few decades the questions of existence, multiplicity and qualitative properties of nodal (sign-changing) solutions to the wide class of elliptic