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Miskolc Mathematical Notes HU e-ISSN 1787-2413 Vol. 18 (2017), No. 1, pp. 31–45 DOI: 10.18514/MMN.2017.1906 MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS IN AN ORLICZ-SOBOLEV SPACE SETTING GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH Received 05 December, 2015 Abstract. In this paper, the authors improve some results on the existence of at least three weak solutions for non-homogeneous systems. The proof of the main result relies on a recent vari- ational principle due to Ricceri. 2010 Mathematics Subject Classification: 34B37; 35J60; 35J70; 46N20; 58E05 Keywords: three solutions, non-homogeneous differential operator, Orlicz-Sobolev space 1. I NTRODUCTION This paper is motivated by phenomena that are described by non-homogeneous Neumann double eigenvalue systems of the type 8 ˆ < ˆ : div ˛ i .jr u i j/r u i C ˛ i .ju i j/u i D F u i .x;u 1 ;:::;u n / CG u i .x;u 1 ;:::;u n /; in ˝; @u i @ D 0; on @˝; (1.1) for 1 i n; where ˝ is a bounded domain in R N (N 3) with a smooth boundary , is the outward unit normal to , and are positive parameters, F , G W ˝ R n ! R are measurable functions with respect to x 2 ˝ for every .t 1 ;:::;t n / 2 R n and are C 1 with respect to .t 1 ;:::;t n / 2 R n for a.e. x 2 ˝. Here, F u i and G u i denote the partial derivative of F and G with respect to u i ; respectively, and the functions ˛ i .t/ W R ! R for 1 i n will be specified later. For any function H W ˝ R n ! R, we denote by .H0/ the following assumption on H W (H0) H is measurable with respect to x 2 ˝ for every .t 1 ;:::;t n / 2 R n , and for every M>0 and for every 1 i n; sup j.t 1 ;:::;t n /jM jH u i .x;t 1 ;:::;t n /j2 L 1 .˝/: Our approach in this paper relies on variational methods in Orlicz-Sobolev spaces. Such spaces originated with Nakano [26] and were further developed by Musielak c 2017 Miskolc University Press

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Page 1: MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS IN AN ORLICZ ...mat76.mat.uni-miskolc.hu › mnotes › download_article › 1906.pdf · MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS IN AN ORLICZ-SOBOLEV

Miskolc Mathematical Notes HU e-ISSN 1787-2413Vol. 18 (2017), No. 1, pp. 31–45 DOI: 10.18514/MMN.2017.1906

MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS IN ANORLICZ-SOBOLEV SPACE SETTING

GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

Received 05 December, 2015

Abstract. In this paper, the authors improve some results on the existence of at least three weaksolutions for non-homogeneous systems. The proof of the main result relies on a recent vari-ational principle due to Ricceri.

2010 Mathematics Subject Classification: 34B37; 35J60; 35J70; 46N20; 58E05

Keywords: three solutions, non-homogeneous differential operator, Orlicz-Sobolev space

1. INTRODUCTION

This paper is motivated by phenomena that are described by non-homogeneousNeumann double eigenvalue systems of the type8<

:�div

�˛i .jrui j/rui

�C˛i .jui j/ui D �Fui .x;u1; : : : ;un/

C�Gui .x;u1; : : : ;un/; in˝;@ui

@�D 0; on @˝;

(1.1)

for 1� i � n; where˝ is a bounded domain in RN (N � 3) with a smooth boundary@˝, � is the outward unit normal to @˝, � and � are positive parameters, F , G W˝�Rn! R are measurable functions with respect to x 2 ˝ for every .t1; : : : ; tn/ 2 Rn

and are C 1 with respect to .t1; : : : ; tn/ 2Rn for a.e. x 2˝. Here, Fui andGui denotethe partial derivative of F and G with respect to ui ; respectively, and the functions˛i .t/ W R! R for 1� i � n will be specified later.

For any function H W˝ �Rn! R, we denote by .H0/ the following assumptionon H W

(H0) H is measurable with respect to x 2 ˝ for every .t1; : : : ; tn/ 2 Rn, and forevery M > 0 and for every 1� i � n;

supj.t1;:::;tn/j�M

jHui .x; t1; : : : ; tn/j 2 L1.˝/:

Our approach in this paper relies on variational methods in Orlicz-Sobolev spaces.Such spaces originated with Nakano [26] and were further developed by Musielak

c 2017 Miskolc University Press

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32 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

and Orlicz [25]. Many properties of Sobolev spaces have been extended to Orlicz-Sobolev spaces, mainly by Dankert [11], Donaldson and Trudinger [14], and O’Neill[27] (see also [1] for an excellent account of those works). Orlicz-Sobolev spaceshave been used in the last two decades to model various phenomena. These kindof spaces play a significant role in many fields of mathematics, such as approxima-tion theory, partial differential equations, calculus of variations, nonlinear potentialtheory, quasiconformal mappings, differential geometry, geometric function theory,and probability theory. Due to this, several authors have widely studied the existenceof solutions for eigenvalue problems involving non-homogeneous operators (see, forexample, [2, 3, 5–10, 15, 17, 18, 20–22, 33]).

Notice that if i D 1 and �D 0, then problem (1.1) becomes8<: �div�˛.jruj/ru

�C˛.juj/uD �f .x;u/; in˝;

@u

@�D 0; on @˝:

(1.2)

Bonanno, Molica Bisci, and Radulescu [5] used a recent critical points result in orderto prove the existence of an open interval of positive eigenvalues for which the prob-lem (1.2) admits at least three weak solutions. The same authors in [6] establishedan open interval of positive parameters for which the problem (1.2) admits infinitelymany weak solutions that strongly converges to zero.

In [8] Cammaroto and Vilasi proved the existence of three weak solutions to thenonhomogeneous boundary value problem:�

�div�˛.jruj/ru

�D �f .x;u/C�g.x;u/; in˝;

uD 0; on @˝: (1.3)

Note that if we take ˛.t/D jt jp�2 .p > 1/ in problems (1.2) and (1.3), the operatoron the left hand side reduces to the classical p-Laplacian; these types of problemshave been widely investigated and a large variety of existence results can be found inthe literature.

The classical three critical point theorem of Pucci and Serrin [28,29] asserts that ifh W Y ! R is of class C 1 (Y is a Banach space), satisfies the Palais-Smale condition,and has two local minima, then h has a third critical point. The general variationalprinciple of Ricceri [31, 32] extends the Pucci-Serrin theorem and provides altern-atives for the multiplicity of critical points of certain functionals depending on aparameter. We refer to [19] and the monograph of Graef and Kong [16] for severalapplications of Ricceri’s variational principles.

In this paper, motivated by the above facts and the recent paper of Molica Bisciand Radulescu [23], under appropriate conditions on F and G, we present sufficientconditions for the system (1.1) to possesses three weak solutions in an Orlicz-Sobolevspace.

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MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS 33

Our paper is organized as follows. In Section 2, some preliminaries and the ab-stract Orlicz-Sobolev space settings are presented. In Section 3, we discuss the exist-ence of three weak solutions for the system (1.1). We also point out special cases ofthe results and we illustrate the results by presenting an example.

2. FUNCTIONAL SETTING

We now recall the following three critical points theorem that follows from a com-bination of [4, Theorem 3.6] and [32, Theorem 1].

Theorem 1. Let X be a reflexive real Banach space, J WX ! R be a sequentiallyweakly lower semicontinuous and continuously Gateaux differentiable functional thatis bounded on bounded subsets of X and whose Gateaux derivative admits a con-tinuous inverse on the dual space X�, and let I WX ! R be a continuously Gateauxdifferentiable functional whose Gateaux derivative is compact and satisfies

J.0/D I.0/D 0:

Assume that there exist r > 0 and Nx 2X with r < J. Nx/ such that(j) supJ.x/�r I.x/ < rI. Nx/=J. Nx/,

(jj) for each � in

�r WD

J. Nx/

I. Nx/;

r

supJ.x/�r I.x/

!;

the functional J ��I is coercive.Then, for each compact interval Œa;b� 2 �r ; there exists � > 0 with the followingproperty: for every � 2 Œa;b� and every C 1 functional � W X ! R with compactderivative, there exists ı > 0 such that, for each � 2 Œ0;ı�; the equation J 0.x/��I 0.x/��� 0.x/D 0 has at least three solutions in X whose norms are less than �.

In order to study the problem (1.1), let us introduce the function spaces settingsto be used. We will give just a brief review of some basic concepts and facts of thetheory of Orlicz-Sobolev spaces that will be useful in what follows; for more detailswe refer the reader to Adams [1], Diening [12], Musielak [24], and Rao and Ren [30].

We begin by recalling some facts from the theory of Orlicz-Sobolev spaces thatwill be used in the present paper. Suppose that the function ˛ W R! R is such thatthe mapping ' W R! R defined by

'.t/D

�˛.jt j/t; for t ¤ 0;

0; for t D 0;

is an odd and strictly increasing homeomorphism from R onto R. Consider the func-tions

˚.t/D

Z t

0

'.s/ds and ˚?.t/D

Z t

0

'�1.s/ds for t 2 R:

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34 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

We observe that ˚ is a Young’s function, that is, ˚.0/D 0; ˚ is convex, and

limt!1

˚.t/DC1:

Furthermore, since ˚.t/D 0 if and only if t D 0,

limt!0

˚.t/

tD 0; and lim

t!1

˚.t/

tDC1;

˚ is called an N –function. The function ˚? is called the complementary function of˚ and satisfies

˚?.t/D supfst �˚.s/ W s � 0g for all t � 0:

We note that ˚? is also an N –function and the following Young’s inequality holds:

st � ˚.s/C˚?.t/; for all s; t � 0:

Assume that ˚ satisfies the structural hypotheses

.˚0/ 1 < liminft!1

t'.t/

˚.t/� 'C WD sup

t>0

t'.t/

˚.t/<1

and

.˚1/ N < '� WD inft>0

t'.t/

˚.t/< liminf

t!1

log.˚.t//log.t/

:

We also assume that the function

.˚2/ t ! ˚.pt / for t 2 Œ0;1/

is convex. To illustrate these notions, we have the following example.

Example 1. Let p > N C1. Define

'.t/Djt jp�2

log.1Cjt j/t for t ¤ 0; '.0/D 0;

and

˚.t/D

Z t

0

'.s/ ds:

By [9, Example 3, p. 243], we have

'� D p�1 < 'C D p D liminft!1

log.˚.t//log.t/

:

Thus, conditions .˚0/ and .˚1/ are satisfied. Furthermore, by a direct computation,we see that the function t 7!˚.

pt / for t 2 Œ0;1/ is convex, so .˚2/ is also satisfied.

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MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS 35

The Orlicz space L˚ .˝/ defined by the N–function ˚ (see for instance [1] and[13]) is the space of measurable functions u W˝! R such that

kukL˚ WD sup�ˇZ

˝

u.x/v.x/ dx

ˇW

˚?.jv.x/j/ dx � 1

�<1 :

The space .L˚ .˝/;k � kL˚ / is a Banach space whose norm is equivalent to the Lux-emburg norm

kuk1;˚ WD inf�k > 0 W

˚

�u.x/

k

�dx � 1

�:

We denote by W 1L˚ .˝/ the corresponding Orlicz-Sobolev space for problem(1.1) defined by

W 1L˚ .˝/D

�u 2 L˚ .˝/ W

@u

@xj2 L˚ .˝/; j D 1; :::;N

�:

This is a Banach space with respect to the norm

kuk2;˚ D kjrujk1;˚ Ckuk1;˚ I

see [1, 10, 15].The following two lemmas can be found in [18].

Lemma 1. ([18, Lemma 2.2]) In W 1L˚ .˝/, the norms

kuk2;˚ D kjrujk1;˚ Ckuk1;˚ ;

kuk3;˚ Dmaxfkjrujk1;˚ ;kuk1;˚g;and

kuk˚ D inf�� > 0I

�˚

�ju.x/j

�C˚

�jru.x/j

��dx � 1

�are equivalent. More precisely, for every u 2W 1L˚ .˝/ we have

kuk˚ � 2kuk3;˚ � 2kuk2;˚ � 4kuk˚ :

Lemma 2. ([18, Lemma 2.3]) Let u 2W 1L˚ .˝/. Then:Z˝

Œ˚.ju.x/j/C˚.jru.x/j/� dx � kuk'�

˚ ; if kuk˚ > 1IZ˝

Œ˚.ju.x/j/C˚.jru.x/j/� dx � kuk'C

˚ ; if kuk˚ < 1:

These spaces generalize the usual spaces Lp.˝/ and W 1;p.˝/, in which the roleplayed by the convex mapping t 7! jt jp=p is assumed by a more general convexfunction ˚.t/.

Proposition 1. (See [1, p. 241 and p. 247]) The spaces L˚ .˝/ and W 1L˚ .˝/

are separable and reflexive Banach spaces.

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36 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

Remark 1. In view of condition .˚1/, from [10, Lemma D.2] it follows thatW 1L˚ .˝/ is continuously embedded in W 1;'�.˝/. On the other hand, since weassumed that '� > N , we can conclude that W 1;'�.˝/ is compactly embedded inC 0.˝/. Thus, we have that W 1L˚ .˝/ is compactly embedded in C 0.˝/.

Throughout this paper, the functions ˛i W R! R are such that the mappings 'i WR! R defined by

'i .t/D

�˛i .jt j/t; for t ¤ 0;

0; for t D 0;

for 1 � i � n are odd and strictly increasing homeomorphism from R to R: Also,assume that the functions

˚i .t/D

Z t

0

'i .s/ ds for t 2 R

for 1� i � n satisfying the structural hypotheses .˚0/, .˚1/, and .˚2/.We let E be the Cartesian product of n Orlicz-Sobolev spaces W 1L˚i .˝/ for

1� i � n; i.e., E DQniD1W

1L˚i .˝/ endowed with the norm

kuk WD

nXiD1

kuk˚i ; uD .u1; : : : ;un/ 2E:

In the space C 0.˝/, we consider the norm kuk1 WD supx2˝ ju.x/j. Set

m WDmax

8<: supu2W 1L˚i .˝/nf0g

kuk1

kuk˚iW for1� i � n

9=; : (2.1)

Since N < '�i for 1 � i � n; from Remark 1, the embedding E ,! C 0.˝/� : : :�

C 0.˝/ is compact, so that m<C1:We say that uD .u1; : : : ;un/ 2E is a weak solution of the problem (1.1) ifZ

˝

nXiD1

�˛i .jrui .x/j/rui .x/rvi .x/C˛i .jui .x/j/ui .x/vi .x/

�dx

��

nXiD1

Fui .x;u1.x/; : : : ;un.x//vi .x/ dx

��

nXiD1

Gui .x;u1.x/; : : : ;un.x//vi .x/ dx D 0

for every v D .v1; : : : ;vn/ 2E.

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MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS 37

3. MAIN RESULTS

We begin this section with our main existence result.

Theorem 2. Assume that F W˝�Rn! R satisfies .H0/ and the following condi-tions:

(F1) there exist d 2L1.˝/ and n positive constants ˇi , with ˇi < '�i for 1� i �n; such that

0� F.x; t1; : : : ; tn/� d.x/

1C

nXiD1

jti jˇi

!for a.e. x 2˝ and all .t1; : : : ; tn/ 2 Rn;

(F2) F.x;0; : : : ;0/D 0 for a.e x 2˝;(F3) there exist 0 < ci <m and si 2 R for 1� i � n with

j˝j

nXiD1

˚i .jsi j/ >min��cim

�'Ci W 1� i � n

�;

such thatZ˝

supjt1j�c1;:::;jtnj�cn

F.x; t1; : : : ; tn/dx

<

min��cim

�'Ci W 1� i � n

�j˝j

PniD1˚i .jsi j/

F.x;s1; : : : ; sn/dx;

where j˝j denotes the Lebesgue measure of the set ˝:

Then, setting

� WD

0BB@ j˝jPniD1˚i .jsi j/R

˝ F.x;s1; : : : ; sn/dx;

min��cim

�'Ci W 1� i � n

�R˝ supjt1j�c1;:::;jtnj�cn F.x; t1; : : : ; tn/dx

1CCA ;for each compact interval Œa;b���; there exists � > 0 with the following property:for every � 2 Œa;b� and for every functionG W˝�Rn! R satisfying condition .H0/;there exists ı > 0 such that, for each � 2 Œ0;ı�; the system (1.1) admits at least threeweak solutions in E whose norms are less than �.

Proof. In order to prove the theorem, we will apply Theorem 1. For each.u1; : : : ;un/ 2E, let the functionals J , I WE! R be defined by

J.u/ WD

nXiD1

�˚i .jrui .x/j/C˚i .jui .x/j/

�dx

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38 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

and

I.u/ WD

F.x;u1.x/ : : : ;un.x// dx:

Clearly, J is bounded on each bounded subset of E and similar arguments as thoseused in [21, Lemma 4.2] imply that J and I are continuously Gateaux differentiablefunctionals whose derivatives at the point u D .u1; : : : ;un/ 2 E are the functionalJ 0.u/ and I 0.u/ given by

J 0.u/.v/D

nXiD1

�˛i .jrui .x/j/rui .x/rvi .x/C˛i .jui .x/j/ui .x/vi .x/

�dx

and

I 0.u/.v/D

nXiD1

Fui .x;u1.x/ : : : ;un.x//vi .x/ dx

for every v D .v1; : : : ;vn/ 2 E: Moreover, since ˚i for 1 � i � n are convex, itfollows that J is a convex functional, and hence it is sequentially weakly lower semi-continuous. By Lemma 2, we see that J is coercive, and arguing as in the proof of[18, Lemma 3.2], we have that J 0 W E ! E� is a uniformly monotone operator inE: By applying the Minty-Browder theorem (Theorem 26.A of [34]), J 0 admits acontinuous inverse on E�:

We claim that I 0 W E! E� is a compact operator. To this end, it suffices to showthat I 0 is strongly continuous on E, so for fixed .u1; : : : ;un/ 2E; let .u1m; : : : ;unm/! .u1; : : : ;un/ weakly in E as m!C1: Then we have .u1m; : : : ;unm/ convergesuniformly to .u1; : : : ;un/ on ˝ as m!C1 (see [34]). Since F.x; �; : : : ; �/ is C 1

in Rn for every x 2 ˝; the partial derivatives of F are continuous in Rn for everyx 2 ˝; so for 1 � i � n; Fui .x;u1m; : : : ;unm/! Fui .x;u1; : : : ;un/ strongly asm!C1: By the Lebesgue dominated convergence theorem, I 0.u1m; : : : ;unm/!I 0.u1; : : : ;un/ strongly as m!C1: Thus, I 0 is strongly continuous on E; whichimplies that I 0 is a compact operator by [34, Proposition 26.2]. Hence, our claim istrue.

From the definitions of J and I and from .F2/; we have

J.0/D I.0/D 0:

Next, set w.x/ WD .s1; : : : ; sn/ for any x 2˝; and

r WDmin��cim

�'Ci W 1� i � n

�:

Clearly, w 2E; and we have

J.w/D j˝j

nXiD1

˚i .jsi j/ > r > 0:

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MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS 39

Let J.u/� r for uD .u1; : : : ;un/ 2E: By Lemma 2, for 1� i � n; we have

kuk˚i �maxfr1='�i ; r1='

C

i g:

Then, for 1� i � n;

kuk˚i �ci

m:

Taking into account that for each u 2W 1L˚i .˝/,

kuk1 �mkuk˚i

for 1� i � n (see (2.1)), we obtain

kuik1 � ci for1� i � n:

Therefore, for every uD .u1; : : : ;un/ 2E;

supu2J�1..�1;r//

I.u/ D

F.x;u1.x/; : : : ;un.x//dx

supjt1j�c1;:::;jtnj�cn

F.x; t1; : : : ; tn/dx:

Condition .F3/ implies

supu2J�1..�1;r// I.u/

r�

R˝ supjt1j�c1;:::;jtnj�cn F.x; t1; : : : ; tn/dx

min��cim

�'Ci W 1� i � n

�<

R˝ F.x;s1; : : : ; sn/dx

j˝jPniD1˚i .jsi j/

DI.w/

J.w/:

Thus, assumption (j) of Theorem 1 is satisfied.In view of .F1/, the functional J ��I is coercive for every positive parameter �;

in particular, for every

� 2��

J.w/

I.w/;

r

supJ.u/�r I.u/

!;

so condition (jj) of Theorem 1 holds. In addition, for every function G W˝�Rn! Rsatisfying condition .H0/, the functional

� .u/ WD

G.x;u1.x/ : : : ;un.x// dx

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40 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

is well defined and continuously Gateaux differentiable on E with a compact deriv-ative given by

� 0.u/.v/D

nXiD1

Gui .x;u1.x/ : : : ;un.x//vi .x/ dx

for every uD .u1; : : : ;un/, vD .v1; : : : ;vn/2E. Thus, all the conditions of Theorem1 are satisfied. Also, note that the solutions of the equation

J 0.u/��I 0.u/��� 0.u/D 0

are exactly the weak solutions of (1.1). So, the conclusion follows from Theorem1. �

Next, we consider the special case of Theorem 2 where F does not depend onx 2˝:

Theorem 3. Assume that F W Rn! R is a C 1-function satisfying

(F4) there exist nC1 positive constants � and ˇi with ˇi <'�i for 1� i � n; suchthat

0� F.t1; : : : ; tn/� �

1C

nXiD1

jti jˇi

!for all .t1; : : : ; tn/ 2 Rn;

(F5) F.0; : : : ;0/D 0;(F6) there exist 0 < ci <m and si 2 R for 1� i � n with

j˝j

nXiD1

˚i .jsi j/ >min��cim

�'Ci W 1� i � n

�;

such that

supjt1j�c1;:::;jtnj�cn

F.t1; : : : ; tn/

<

min��cim

�'Ci W 1� i � n

�j˝j

PniD1˚i .jsi j/

F.s1; : : : ; sn/:

Then, setting

� WD

0BB@PniD1˚i .jsi j/

F.s1; : : : ; sn/;

min��cim

�'Ci W 1� i � n

�j˝jsupjt1j�c1;:::;jtnj�cn F.t1; : : : ; tn/

1CCA ;

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MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS 41

for each compact interval Œa;b���; there exists � > 0 with the following property:for every � 2 Œa;b� and for every functionG W˝�Rn! R satisfying condition .H0/;there exists ı > 0 such that, for each � 2 Œ0;ı�; the system8<

:�div

�˛i .jrui j/rui

�C˛i .jui j/ui D �Fui .u1; : : : ;un/

C�Gui .x;u1; : : : ;un/; in˝;@ui

@�D 0; on @˝;

(3.1)

for 1� i � n; admits at least three weak solutions in E whose norms are less than �.

Now, consider the problem8<: �div�˛.jruj/ru

�C˛.juj/uD �f .u/C�g.x;u/ in˝;

@u

@�D 0 on @˝;

(3.2)

where � and � are positive parameters, f W R! R is a continuous function, g W˝ �R! R is an L1-Caratheodory function, and ˛ is as in Section 2.

Let

k WD supu2W 1L˚ .˝/nf0g

kuk1

kuk˚

and

F.t/ WD

Z t

0

f .�/d� for t 2 R: (3.3)

The following result is a special case of Theorem 3.

Theorem 4. Let f W R! R be a non-negative continuous function, and assumethat the function F in (3.3) satisfies:

(F7) there exist two positive constants � and ˇ < '� such that

F.t/� ��1Cjt jˇ

�for t 2 RI

(F8) there exist 0 < c < k and s 2 R with

j˝j˚.jsj/ >� ck

�'Csuch that

supjt j�c

F.t/ <

�ck

�'Cj˝j˚.jsj/

F.s/:

Then, setting

� WD

0@˚.jsj/F.s/

;

�ck

�'Cj˝jsupjt j�cF.t/

1A ;for each compact interval Œa;b���; there exists � > 0 with the following property:for every � 2 Œa;b� and for every L1-Caratheodory function g W ˝ �R! R; there

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42 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

exists ı > 0 such that, for each � 2 Œ0;ı�; the system (3.2) admits at least three weaksolutions in W 1L˚ .˝/ whose norms are less than �.

As an example of our main result, we state a special case of Theorem 4.

Corollary 1. Let f W R! R be a non-negative (not identically zero) continuousfunction such that

.`0/ limt!0C

f .t/

t'C�1D 0:

Assume thatF.t/� �

�1Cjt jˇ

�for t 2 R;

and set

� WD

�j˝j inf

s2S

˚.s/

F.s/;C1

�;

whereS WD fs > 0 W F.s/ > 0g :

Then, for each compact interval Œa;b� � �; there exists � > 0 with the followingproperty: for every �2 Œa;b� and for everyL1-Caratheodory function g W˝�R!R;there exists ı > 0 such that, for each � 2 Œ0;ı�; the system (3.2) admits at least threeweak solutions in W 1L˚ .˝/ whose norms are less than �.

Proof. Fix � > j˝j infs2S˚.s/F .s/

: Then, there exists s such that F.s/ > 0 and

� > j˝j˚.s/

F.s/:

From condition .`0/, we have

lim�!0C

F.�/

�'CD 0:

Therefore, we can find a positive constant c such that

c < kminn1;�j˝j˚.jsj/

�1='Co;

andF.c/

c'C<

1

k'C

min�

F.s/

j˝j˚.jsj/;1

�j˝j

�:

Hence,

� 2

0@˚.jsj/F.s/

;

�ck

�'Cj˝jF.c/

1A :The hypotheses of Theorem 4 are satisfied, so the conclusion follows. �

Next, we give a concrete application of Corollary 1.

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MULTIPLE SOLUTIONS FOR NEUMANN SYSTEMS 43

Example 2. Let ˝ be a non-empty bounded open subset of the Euclidean SpaceRN (N � 3) with smooth boundary @˝, and let˚ be a Young’s function that satisfieshypotheses .˚0/–.˚2/. Define f W R! R by

f .t/ WD

8<:0; if t < 0;t'C

; if 0� t � 1;ts; if t > 1;

where s 2 .0;'��1/. Setting

� WD

0@˚.jsj/F.s/

;

�ck

�'Cj˝jsupjt j�cF.t/

1A ;from Corollary 1 for each compact interval Œa;b� � �; there exists � > 0 with thefollowing property: for every � 2 Œa;b� and for every L1-Caratheodory function g W˝ �R! R; there exists ı > 0 such that, for each � 2 Œ0;ı�; the system (3.2) admitsat least three weak solutions in W 1L˚ .˝/ whose norms are less than �.

In particular, let ˝ � R3 with j˝j D 1. Consider f W R! R defined by

f .t/ WD

8<:0; if t < 0;t5; if 0� t � 1;t2; if t > 1:

Set ˚.s/ WDZ s

0

t jt j3

log.1Cjt j/dt . Then, for every s > 0,

˚.s/

F.s/WD

8ˆ<ˆ:6

Z s

0

t jt j3

log.1Cjt j/dt

s6; if 0� s � 1,

6

Z s

0

t jt j3

log.1Cjt j/dt

2s3�1; if s > 1.

Moreover, by direct computations, since the function˚.s/

F.s/attains its minimum at

s0 � 1:189089126, it follows that

infs>0

˚.s/

F.s/� 1:804670144:

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44 GHASEM A. AFROUZI, JOHN R. GRAEF, AND SAEID SHOKOOH

So, for every L1-Caratheodory function g W˝ �R! R; there exists ı > 0 such that,for each � 2 Œ0;ı�, the non-homogeneous Neumann problem8<:�div

�jruj3

log.1Cjruj/ru�C

juj3

log.1Cjuj/uD 2f .u/C�g.x;u/; in ˝;

@u

@�D 0; on @˝;

admits at least three weak solutions in W 1L˚ .˝/.

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Authors’ addresses

Ghasem A. AfrouziDepartment of Mathematics, Faculty of Mathematical Sciences, University of Mazandaran, Babolsar,

IranE-mail address: [email protected]

John R. GraefDepartment of Mathematics, University of Tennessee at Chattanooga, Chattanooga, TN 37403, USAE-mail address: [email protected]

Saeid ShokoohDepartment of Mathematics, Faculty of Sciences, Gonbad Kavous University, Gonbad Kavous, IranE-mail address: [email protected]