RADIAL SOLUTIONS FOR INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS

Similar documents
EXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS WITH UNBOUNDED POTENTIAL. 1. Introduction In this article, we consider the Kirchhoff type problem

EXISTENCE OF NONTRIVIAL SOLUTIONS FOR A QUASILINEAR SCHRÖDINGER EQUATIONS WITH SIGN-CHANGING POTENTIAL

Bulletin of the. Iranian Mathematical Society

NONLINEAR SCHRÖDINGER ELLIPTIC SYSTEMS INVOLVING EXPONENTIAL CRITICAL GROWTH IN R Introduction

EXISTENCE OF SOLUTIONS FOR A RESONANT PROBLEM UNDER LANDESMAN-LAZER CONDITIONS

EXISTENCE OF SOLUTIONS FOR CROSS CRITICAL EXPONENTIAL N-LAPLACIAN SYSTEMS

EXISTENCE OF WEAK SOLUTIONS FOR A NONUNIFORMLY ELLIPTIC NONLINEAR SYSTEM IN R N. 1. Introduction We study the nonuniformly elliptic, nonlinear system

SOLUTIONS TO SINGULAR QUASILINEAR ELLIPTIC EQUATIONS ON BOUNDED DOMAINS

HOMOCLINIC SOLUTIONS FOR SECOND-ORDER NON-AUTONOMOUS HAMILTONIAN SYSTEMS WITHOUT GLOBAL AMBROSETTI-RABINOWITZ CONDITIONS

COMBINED EFFECTS FOR A STATIONARY PROBLEM WITH INDEFINITE NONLINEARITIES AND LACK OF COMPACTNESS

NONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian UNDER NONHOMOGENEOUS NEUMANN BOUNDARY CONDITION

MULTIPLE SOLUTIONS FOR AN INDEFINITE KIRCHHOFF-TYPE EQUATION WITH SIGN-CHANGING POTENTIAL

Non-homogeneous semilinear elliptic equations involving critical Sobolev exponent

Nonlinear elliptic systems with exponential nonlinearities

ON NONHOMOGENEOUS BIHARMONIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT

Existence and Multiplicity of Solutions for a Class of Semilinear Elliptic Equations 1

Existence of Positive Solutions to Semilinear Elliptic Systems Involving Concave and Convex Nonlinearities

EXISTENCE RESULTS FOR OPERATOR EQUATIONS INVOLVING DUALITY MAPPINGS VIA THE MOUNTAIN PASS THEOREM

MULTIPLE SOLUTIONS FOR A KIRCHHOFF EQUATION WITH NONLINEARITY HAVING ARBITRARY GROWTH

SUPER-QUADRATIC CONDITIONS FOR PERIODIC ELLIPTIC SYSTEM ON R N

MULTIPLE SOLUTIONS FOR CRITICAL ELLIPTIC PROBLEMS WITH FRACTIONAL LAPLACIAN

MULTIPLE POSITIVE SOLUTIONS FOR KIRCHHOFF PROBLEMS WITH SIGN-CHANGING POTENTIAL

Existence of Solutions for a Class of p(x)-biharmonic Problems without (A-R) Type Conditions

POSITIVE GROUND STATE SOLUTIONS FOR SOME NON-AUTONOMOUS KIRCHHOFF TYPE PROBLEMS

p-laplacian problems with critical Sobolev exponents

POSITIVE GROUND STATE SOLUTIONS FOR QUASICRITICAL KLEIN-GORDON-MAXWELL TYPE SYSTEMS WITH POTENTIAL VANISHING AT INFINITY

PERIODIC SOLUTIONS FOR NON-AUTONOMOUS SECOND-ORDER DIFFERENTIAL SYSTEMS WITH (q, p)-laplacian

arxiv: v1 [math.ap] 16 Jan 2015

EXISTENCE OF SOLUTIONS TO ASYMPTOTICALLY PERIODIC SCHRÖDINGER EQUATIONS

INFINITELY MANY SOLUTIONS FOR A CLASS OF SUBLINEAR SCHRÖDINGER EQUATIONS

MULTIPLE SOLUTIONS FOR THE p-laplace EQUATION WITH NONLINEAR BOUNDARY CONDITIONS

CRITICAL POINT METHODS IN DEGENERATE ANISOTROPIC PROBLEMS WITH VARIABLE EXPONENT. We are interested in discussing the problem:

ON THE EXISTENCE OF SIGNED SOLUTIONS FOR A QUASILINEAR ELLIPTIC PROBLEM IN R N. Dedicated to Luís Adauto Medeiros on his 80th birthday

POTENTIAL LANDESMAN-LAZER TYPE CONDITIONS AND. 1. Introduction We investigate the existence of solutions for the nonlinear boundary-value problem

NONHOMOGENEOUS ELLIPTIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT AND WEIGHT

Polyharmonic Elliptic Problem on Eistein Manifold Involving GJMS Operator

Multiplicity of weak solutions for a class of nonuniformly elliptic equations of p-laplacian type

A Caffarelli-Kohn-Nirenberg type inequality with variable exponent and applications to PDE s

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS

SEMILINEAR ELLIPTIC EQUATIONS WITH DEPENDENCE ON THE GRADIENT

Multiple positive solutions for a class of quasilinear elliptic boundary-value problems

MULTIPLE SOLUTIONS FOR BIHARMONIC ELLIPTIC PROBLEMS WITH THE SECOND HESSIAN

On a Nonlocal Elliptic System of p-kirchhoff-type Under Neumann Boundary Condition

ON THE EXISTENCE OF THREE SOLUTIONS FOR QUASILINEAR ELLIPTIC PROBLEM. Paweł Goncerz

Positive and Nodal Solutions For a Nonlinear Schrödinger Equation with Indefinite Potential

EXISTENCE OF SOLUTIONS TO P-LAPLACE EQUATIONS WITH LOGARITHMIC NONLINEARITY

Elliptic equations with one-sided critical growth

EXISTENCE OF MULTIPLE SOLUTIONS TO ELLIPTIC PROBLEMS OF KIRCHHOFF TYPE WITH CRITICAL EXPONENTIAL GROWTH

BIFURCATION AND MULTIPLICITY RESULTS FOR CRITICAL p -LAPLACIAN PROBLEMS. Kanishka Perera Marco Squassina Yang Yang

arxiv: v1 [math.ap] 24 Oct 2014

Variational eigenvalues of degenerate eigenvalue problems for the weighted p-laplacian

STEKLOV PROBLEMS INVOLVING THE p(x)-laplacian

Least energy solutions for indefinite biharmonic problems via modified Nehari-Pankov manifold

A REMARK ON MINIMAL NODAL SOLUTIONS OF AN ELLIPTIC PROBLEM IN A BALL. Olaf Torné. 1. Introduction

EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM. Saeid Shokooh and Ghasem A. Afrouzi. 1. Introduction

GROUND STATE SOLUTIONS FOR CHOQUARD TYPE EQUATIONS WITH A SINGULAR POTENTIAL. 1. Introduction In this article, we study the Choquard type equation

arxiv: v1 [math.ap] 7 May 2009

INFINITELY MANY SOLUTIONS FOR A CLASS OF SUBLINEAR SCHRÖDINGER EQUATIONS. Jing Chen and X. H. Tang 1. INTRODUCTION

EXISTENCE AND MULTIPLICITY OF PERIODIC SOLUTIONS GENERATED BY IMPULSES FOR SECOND-ORDER HAMILTONIAN SYSTEM

Existence of Positive Solutions to a Nonlinear Biharmonic Equation

ANALYSIS AND APPLICATION OF DIFFUSION EQUATIONS INVOLVING A NEW FRACTIONAL DERIVATIVE WITHOUT SINGULAR KERNEL

A NOTE ON THE EXISTENCE OF TWO NONTRIVIAL SOLUTIONS OF A RESONANCE PROBLEM

Weak Solutions to Nonlinear Parabolic Problems with Variable Exponent

Nonlinear Maxwell equations a variational approach Version of May 16, 2018

EXISTENCE OF POSITIVE SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS

KIRCHHOFF TYPE PROBLEMS WITH POTENTIAL WELL AND INDEFINITE POTENTIAL. 1. Introduction In this article, we will study the Kirchhoff type problem

LEAST ENERGY SIGN-CHANGING SOLUTIONS FOR NONLINEAR PROBLEMS INVOLVING FRACTIONAL LAPLACIAN

Nonvariational problems with critical growth

EXISTENCE OF POSITIVE GROUND STATE SOLUTIONS FOR A CLASS OF ASYMPTOTICALLY PERIODIC SCHRÖDINGER-POISSON SYSTEMS

Critical Groups in Saddle Point Theorems without a Finite Dimensional Closed Loop

Existence of positive solution for system of quasilinear elliptic systems on a bounded domain

Minimization problems on the Hardy-Sobolev inequality

Non-radial solutions to a bi-harmonic equation with negative exponent

Multiplicity of solutions for quasilinear elliptic equations with critical exponential growth

Existence of ground states for fourth-order wave equations

arxiv: v1 [math.ap] 28 Mar 2014

LIFE SPAN OF BLOW-UP SOLUTIONS FOR HIGHER-ORDER SEMILINEAR PARABOLIC EQUATIONS

A GLOBAL COMPACTNESS RESULT FOR SINGULAR ELLIPTIC PROBLEMS INVOLVING CRITICAL SOBOLEV EXPONENT

HOMOLOGICAL LOCAL LINKING

ON A CONJECTURE OF P. PUCCI AND J. SERRIN

On non negative solutions of some quasilinear elliptic inequalities

HARNACK S INEQUALITY FOR GENERAL SOLUTIONS WITH NONSTANDARD GROWTH

On a Bi-Nonlocal p(x)-kirchhoff Equation via Krasnoselskii s Genus

Nehari manifold for non-local elliptic operator with concave convex nonlinearities and sign-changing weight functions

KIRCHHOFF TYPE PROBLEMS INVOLVING P -BIHARMONIC OPERATORS AND CRITICAL EXPONENTS

STOKES PROBLEM WITH SEVERAL TYPES OF BOUNDARY CONDITIONS IN AN EXTERIOR DOMAIN

Borderline Variational Problems Involving Fractional Laplacians and Critical Singularities

VARIATIONAL AND TOPOLOGICAL METHODS FOR DIRICHLET PROBLEMS. The aim of this paper is to obtain existence results for the Dirichlet problem

NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS. Shouchuan Hu Nikolas S. Papageorgiou. 1. Introduction

CONSEQUENCES OF TALENTI S INEQUALITY BECOMING EQUALITY. 1. Introduction

EXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE. Leszek Gasiński

FIRST CURVE OF FUČIK SPECTRUM FOR THE p-fractional LAPLACIAN OPERATOR WITH NONLOCAL NORMAL BOUNDARY CONDITIONS

A NONLINEAR DIFFERENTIAL EQUATION INVOLVING REFLECTION OF THE ARGUMENT

LERAY LIONS DEGENERATED PROBLEM WITH GENERAL GROWTH CONDITION

UNIFORM DECAY OF SOLUTIONS FOR COUPLED VISCOELASTIC WAVE EQUATIONS

Strongly nonlinear parabolic initial-boundary value problems in Orlicz spaces

ON A CERTAIN GENERALIZATION OF THE KRASNOSEL SKII THEOREM

MULTIPLE POSITIVE SOLUTIONS FOR P-LAPLACIAN EQUATION WITH WEAK ALLEE EFFECT GROWTH RATE

RELATION BETWEEN SMALL FUNCTIONS WITH DIFFERENTIAL POLYNOMIALS GENERATED BY MEROMORPHIC SOLUTIONS OF HIGHER ORDER LINEAR DIFFERENTIAL EQUATIONS

ON THE SCHRÖDINGER EQUATION INVOLVING A CRITICAL SOBOLEV EXPONENT AND MAGNETIC FIELD. Jan Chabrowski Andrzej Szulkin. 1.

Transcription:

Electronic Journal of Differential Equations, Vol. 018 (018), No. 67, pp. 1 14. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu RADIAL SOLUTIONS FOR INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS REGINALDO DEMARQUE, NARCISO DA HORA LISBOA Abstract. In this article we obtain weak radial solutions for the inhomogeneous elliptic system u + V 1 ( x ) u q u = Q( x )F u(u, v) in, v + V ( x ) v q v = Q( x )F v(u, v) in, u, v D, 0 (RN ), N 5, where is the biharmonic operator, V i, Q C 0 ((0, + ), [0, + )), i = 1,, are radially symmetric potentials, 1 < q < N, q, and F is a s-homogeneous function. Our approach relies on an application of the Symmetric Mountain Pass Theorem and a compact embedding result proved in [17]. 1. Introduction In this article concerns the existence of nontrivial solutions for the inhomogeneous biharmonic elliptic system u + V 1 ( x ) u q u = Q( x )F u (u, v) in, v + V ( x ) v q v = Q( x )F v (u, v) in, u, v D, 0 (RN ), N 5, (1.1) where is the biharmonic operator, V i, Q C 0 ((0, + ), [0, + )), i = 1,, are radially symmetric potentials, 1 < q < N, q, and F is a s-homogeneous function satisfying the following assumptions: (A1) V i C 0 ((0, + ), [0, + )), such that V i (r) lim inf r + r a > 0, lim inf r 0 for some real numbers a and a 0. (A) Q C 0 ((0, + ), [0, + )), is such that lim sup r + V i (r) r a0 > 0, (1.) Q(r) Q(r) r b <, lim sup <, (1.3) r 0 r b0 for some real numbers b and b 0. (A3) F C 1 (R R, R) is a homogeneous function of degree s, with s > max{, q}. 010 Mathematics Subject Classification. 35J50, 31A30. Key words and phrases. Biharmonic operator; elliptic systems; existence of solutions; radial solution; mountain pass theorem. c 018 Texas State University. Submitted June 16, 017. Published March 14, 018. 1

R. DEMARQUE, N. H. LISBOA EJDE-018/67 (A4) There exists C > 0 such that (A5) F (u, v) > 0, u, v > 0. F u (u, v) C( u s 1 + v s 1 ), (u, v) R, F v (u, v) C( u s 1 + v s 1 ), (u, v) R. (1.4) Nonlinear elliptic problems of fourth order without singularities in bounded domains have been extensively studied by several authors, see [9, 0, 38, 40], and references therein. For application or motivation, we note that, when Ω is a bounded domain, the problem u + c u = f(x, u) in Ω, u = u = 0 on Ω, which arises in the study of traveling waves in suspension bridges (see [16, 4, 8]) and in the study of the static deflection of an elastic plate in a fluid. For studies on the existence and multiplicity of solutions for nonlinear biharmonic problems in unbounded domains, the reader is referred to [19, 30, 35] in the radial case, and to [1] in the non-radial sub-(sup) linear case. Maximum principle results for biharmonic equation in unbounded domains are obtained in [3]. Also for unbounded domains, nontrivial solutions and multiplicity results are obtained in [4, 5, 6, 15, 31, 39] and in references therein. Additional results in the scalar case may be found in [34, 36, 37, 41, 4]. Elliptic systems may be used to describe the multiplicative chemical reactions catalyzed by catalyst. For the existence of nontrivial solutions to nonvariational systems, potential systems and Hamiltonian systems including critical exponents case see, for instance, [3, 1, 5, 6, 4]. See also [, 7, 1, 13, 14, 7, 9]. For results for fourth-order equations with singular potential see [30] and [6]. Alves et. al. in [6] proved the existence of solutions to the problem u + V (x) u q 1 u = u u, u D, 0 (Ω), N 5, in Ω where 1 q 1 and V = V (x) is a potential that changes sign and has singularities in Ω. Wang and Shen in [39] proved existence of sign-changing solutions for the problem u = λ u (s) u x s + βa(x) u r u, in Ω u D, 0 (Ω), N 5, motivated by the Hardy-Rellich s inequality RN u λ x 4 dx u dx, as improved in their work. Radial solutions for the biharmonic equation u + V ( x ) u q u = Q( x )f(u), were obtained in [11], when q =, and in [17], when q. Motivated by the work of Alves [] for elliptic systems, a natural question is whether or not the results of

EJDE-018/67 INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS 3 [17] can be extended to the elliptic system (1.1). Here we answer this question in the affirmative when (A3) and (A4) are satisfied. Before stating our results, we to introduce some notation. Let D, 0 (RN ) be the closure of C0 ( ) under the norm u and D, 0,r (RN ) the set of radially symmetric functions in D, 0 (RN ). For p 1 and a function ν : R define L p ( ; ν) = { u : R u is Lebesgue measurable and ν(x) u p dx < + } endowed with the norm ( u p,ν := ν(x) u p dx ) 1/p. Define the Banach space X Vi := D, 0 (RN ) L p ( ; V i ), with the norm u Vi = u + u p,vi and X Vi,r the set of radially symmetric functions in X Vi, i = 1,. We consider the product space X := X V1 X V endowed with the norm ( ) 1/ ( (u, v) := ( u + v )dx + (V 1 ( x ) u q + V ( x ) v q )dx ) 1/q, and X r := X V1,r X V,r. Also, we endow the space L s ( ; Q) L s ( ; Q) endowed with the norm ( ) 1/s. (u, v) s,q = Q( x )( u s + v s )dx Let α := N 4 + q 1 q (a + N) and α 0 := N 4 + q 1 q (a 0 + N). Now, as in [17], we define some indexes that will appear in our results. The bottom indices are defined as q, b a, b N or b N + q(n 4) ε, (N+b+ε) N 4, b a and N < b < N + q(n 4) ε, q + q(b a) s := α, b > a N + q(n 4), q + (b a) N 4, q(n 4) b > a, b > N and N + ε < a < N + q(n 4), (N+b+ε) N 4, b > a, b > N and a N + q(n 4) ε, q + (b a) a < b N, N 4, and the top indices are defined as (N+b 0 ε) N 4, a 0 b 0 > N or b 0 a 0 N + q(n 4) + ε, s q + (b0 a0) N 4, b 0 a 0 and N + q(n 4) a 0 < N + q(n 4) + ε, := q + q(b0 a0) α, b 0 a 0 and N q(n 4) 0 (q 1) < a 0 < N + q(n 4), +, b 0 a 0 and a N q(n 4) (q 1). Consider also s := q + q(b0 a0) α, with b 0 a 0 < N q(n 4) 0 (q 1). Our main result is the following.

4 R. DEMARQUE, N. H. LISBOA EJDE-018/67 Theorem 1.1. Let (A1) (A5) be satisfied. If s < s < s, then system (1.1) has a nontrivial solution (u, v) X r by which we mean ( u. ϕ + v. ψ)dx + (V 1 ( x ) u q uϕ + V ( x ) v q vψ)dx R N (1.5) = Q( x )(ϕf u (u, v) + ψf v (u, v))dx, for all (ϕ, ψ) X. Moreover, if F (u, v) = F ( (u, v)) and there exists η > 0 such that F (u, v) η( u s + v s ), for all (u, v) R, then system (1.1) has infinitely many radial solutions (u, v) X r, i = 1,. The proof of Theorem 1.1 will be given using arguments similar to those developed in [17]. First we define an Euler functional I : X r R associated with the equation (1.5). Then, we obtain a Principle of Symmetric Criticality result, which yields that the critical points of I are solutions of the system. Finally, we prove that this functional has the mountain pass geometry and apply the Symmetric Mountain Pass Theorem to obtain the result.. Existence results In this section we will prove our main result. To do this, we will divide the proof in some lemmas. Firstly, let us present the following embedding theorem established in [17]. Theorem.1. Let V i, i = 1,, and Q be functions satisfying (1.) and (1.3). If s < s, then the embedding X Vi,r L s ( ; Q), is continuous for all s s s when s <, s s < when s = or max{s, s } s <. Furthermore, the embedding is compact for all s < s < s or max{s, s } < s <. Now let us define the Euler functional I : X r R by I(u, v) = 1 ( u + v )dx + 1 (V 1 ( x ) u q + V ( x ) v q )dx R q N R N Q( x )F (u, v) dx. By conditions (A1) (A4) and the continuous embeddings obtained in Theorem.1, we have that I C 1 (X r ; R) with Fréchet derivative in (u, v) X r given by I (u, v), (ϕ, ψ) = ( u. ϕ + v. ψ)dx + (V 1 ( x ) u q uϕ + V ( x ) v q vψ)dx R N Q( x )(ϕf u (u, v) + ψf v (u, v))dx, for all (ϕ, ψ) X r. The proof of the next lemma follows the arguments presented in [17]. Lemma.. Every critical point of the functional I : X r R satisfies (1.5).

EJDE-018/67 INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS 5 Proof. Let (u, v) X r be a critical point of I. Given (ϕ, ψ) X, define ϕ(r) := 1 1 ϕ(ξ)ds(ξ), ψ(r) := ψ(ξ)ds(ξ), (.1) B r B r B r B r where B r denotes the sphere of center 0 and radius r and B r denotes its Lebesgue measure. Proceeding as in the proof of the mean-value formulas for Laplace s equation (see [18]), using polar coordinates in and divergence theorem, we conclude that d dr ϕ(r) = r ϕ(ξ)dξ, N B r B r d dr ψ(r) = r ψ(ξ)dξ, N B r B r d 1 d ϕ(r) = N dr r dr ϕ(r) + 1 ϕ(ξ)ds(ξ) B r B r d dr ψ(r) = N 1 d r dr ψ(r) + 1 ψ(ξ)ds(ξ). B r B r Since ϕ = d dr ϕ + N 1 d r dr ϕ and ψ = d ψ dr + N 1 d ψ, r dr we obtain ϕ = 1 ϕ(ξ)ds(ξ) and B r ψ = 1 ψ(ξ)ds(ξ). (.) B r B r B r From this we see that ( ϕ, ψ) X r and then I (u, v), ( ϕ, ψ) = ( u. ϕ + v. ψ)dx + (V 1 ( x ) u q u ϕ + V ( x ) v q v ψ)dx R N Q( x )( ϕf u (u, v) + ψf v (u, v))dx = 0. Therefore, using polar coordinates in and Fubini s Theorem again and the identities (.1) and (.) we obtain result. Before we prove the Palais-Smale condition for the functional I, we need to make some remarks about assumptions of the function F. Remark.3. (a) Since F is a C 1 homogeneous function of degree s, then sf (u, v) = uf u (u, v) + vf v (u, v) and F is a homogeneous function of degree s 1. (b) From (F 1 ), (a) and the Young inequality we have F (u, v) C( u s + v s ) for all (u, v) R. (c) Our prototype of F is F (u, v) = (a u + b v ) s + c u α v β, u, v R; a, b, c > 0 and α + β = s, with α, β > 1. Lemma.4. The functional I : X r R satisfies the Palais-Smale condition. Proof. Let {(u n, v n )} be a sequence X r such that I (u n, v n ) 0 and I(u n, v n ) c, as n +. We shall see that {(u n, v n )} is bounded in X. Indeed, since I (u n, v n ) 0, we have I (u n, v n ) < 1 for all n sufficiently large, and so, I (u n, v n ), (u n, v n ) (u n, v n ). Since {I(u n, v n )} is convergent sequence, there

6 R. DEMARQUE, N. H. LISBOA EJDE-018/67 exists a positive constant C 0 such that I(u n, v n ) C 0. In this case, from (F 0 ) and the Remark (a), we have C 0 + 1 s (u n, v n ) I(u n, v n ) 1 s I (u n, v n ), (u n, v n ) (.3) [ ] C ( u n + v n )dx + (V 1 ( x ) u n q + V ( x ) v n q )dx, where C 0 and C are positive constants. To conclude that {(u n, v n )} is bounded, we will split our arguments in the cases: 1 < q < and q >. Case q >. Suppose {(u n, v n )} is unbounded. Then, up to a subsequence, (u n, v n ) +, as n +. From (.3) we see that C 0 (u n, v n ) + 1 1 s (u n, v n ) C [ (u n, v n ) ( u n + v n )dx (.4) R N ] + (V 1 ( x ) u n q + V ( x ) v n q )dx, for some positive constants C 0 and C. If { (V 1 ( x ) u n q + V ( x ) v n q )dx } is an unbounded sequence, then, up to a subsequence, (V 1 ( x ) u n q + V ( x ) v n q )dx +, as n +. This implies that (V 1 ( x ) u n q + V ( x ) v n q )dx > 1, for n sufficiently large. Consequently, since q >, we obtain [ ] (u n, v n ) ( u n + v n )dx + (V 1 ( x ) u n q + V ( x ) v n q )dx. Combining this with (.4) we deduce that C 0 (u n, v n ) + 1 1 s (u n, v n ) C, for some constants C 0, C > 0 and for n sufficiently large. So we obtain a contradiction. On the other hand, if { (V 1 ( x ) u n q + V ( x ) v n q )dx } is bounded, we conclude that ( u n + v n )dx +, as n +, up to a subsequence. Using (.4) we see that, for some positive constants C 0 and C, C 0 (u n, v n ) + 1 1 s (u n, v n ) C u n + v n + u n q q,v 1 + v n q q,v (u n, v n ) 1 + un q q,v + v 1 n q q,v u n = C + vn ] [1+ ( un q q,v + v 1 n q q,v ) 1/q C, ( u n + vn )1/

EJDE-018/67 INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS 7 as n +. Here we also have a contradiction. Case 1 < q <. If { ( u n + v n )dx } is an unbounded sequence, then, up to a subsequence, ( u n + v n )dx +, as n +. As a consequence ( u n + v n )dx > 1, for n sufficiently large. 1 < q <, it follows that (u n, v n ) q ) q ] + (V 1 ( x ) u n q + V ( x ) v n q )dx ] q[( ( u n + v n )dx q[ ( u n + v n )dx + (V 1 ( x ) u n q + V ( x ) v n q )dx. Using this and (.3) we conclude that, for some positive constants C 0 and C, C 0 + 1 s (u n, v n ) C q (u n, v n ) q, for n sufficiently large. But this is a contradiction. Now, if { ( u n + v n )dx } is bounded, then, up to a subsequence, (V 1 ( x ) u n q + V ( x ) v n q )dx +, as n +. Hence, using (.3) again, we obtain C 0 (u n, v n ) q + 1 1 s (u n, v n ) q 1 C u n + v n + u n q q,v 1 + v n q q,v (u n, v n ) q = C u n + vn u n q q,v + v 1 n + 1 q q,v [ ] ( un q C, + vn )1/ ( u n q q,v + v 1 n + 1 q q,v ) 1/q Since as n +. We have again a contradiction and, therefore, {(u n, v n )} is bounded in X r. Consequently, {u n } and {v n } are also bounded in X r,v1 and X r,v, respectively. Using the fact that X r,vi, i {1, }, is reflexive, we conclude that there exist u X r,v1 and v X r,v such that u n u weakly in X r,v1 and v n v weakly in X r,v, as n +, up to subsequences. Hence (u n, v n ) (u, v) weakly in X r, as n +, up to a subsequence. Since X r,vi is compactly imbedded in L s ( ; Q), i {1, } (see Theorem.1), we deduce that u n u and v n v strongly in L s ( ; Q), as n +. As a consequence, u n u and v n v a.e. in, as n +. Now we shall prove that I (u n, v n ), (ϕ, ψ) I (u, v), (ϕ, ψ), for all (ϕ, ψ) X r, as n +. For (ϕ, ψ) X r, we define F (ϕ,ψ) (u, v) := [ u ϕ + v ψ]dx.

8 R. DEMARQUE, N. H. LISBOA EJDE-018/67 Note that F (ϕ,ψ) X r and F (ϕ,ψ) (u, v), (z, w) = [ z ϕ + w ψ]dx, for all (z, w) X r. Since (u n, v n ) (u, v) weakly in X r, as n +, we deduce that F (ϕ,ψ) (u n, v n ) F (ϕ,ψ) (u, v) strongly in X r, as n +, for all (ϕ, ψ) X r, that is, [ u n ϕ + v n ψ]dx [ u ϕ + v ψ]dx, (.5) as n +, for all (ϕ, ψ) X r. We consider (ϕ, ψ) X r and define g n := (V 1 ) q 1 q un q u n, h n := (V ) q 1 q vn q v n, g := (V 1 ) q 1 q u q u, h := (V ) q 1 q v q v. So, g n g and h n h a.e. in. Moreover, {g n } and {h n } are bounded in L q/(q 1) ( ). It follows from Brézis and Lieb lemma [10] (see also [, Lemma 4.8]) that g n ϕdx gϕdx and h n ψdx hψdx, as n +, for all ϕ, ψ L q ( ). In particular, given (ϕ, ψ) X r, we have (V 1 ) 1/q ϕ, (V ) 1/q ψ L q ( ), so that, g n (V 1 ( x )) 1/q ϕdx g(v 1 ( x )) 1/q ϕdx and h n (V ( x )) 1/q ψdx h(v ( x )) 1/q ψdx, as n +. Hence, V 1 ( x ) u n q u n ϕdx V 1 ( x ) u q uϕdx and V ( x ) v n q v n ψdx V ( x ) v q vψdx, as n +. Consequently, (V 1 ( x ) u n q u n ϕ + V ( x ) v n q v n ψ)dx (.6) (V 1 ( x ) u q uϕ + V ( x ) v q vψ)dx, as n +, for all (ϕ, ψ) X r. We define K : X r X r by K(u, v), (ϕ, ψ) := Q( x )[ϕf u (u, v) + ψf v (u, v)]dx. First, we prove that F u (u n, v n ) F u (u, v) s s 1,Q 0 and F v (u n, v n ) F v (u, v) s s 1,Q 0,

EJDE-018/67 INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS 9 as n +. By using (A4), we will deduce that Q( x ) F u (u n, v n ) F u (u, v) s s 1 h(x) a.e. x, for some function h L 1 ( ). In fact, since Q 1 s u n Q 1/s u s 0 and Q 1 s v n Q 1/s v s 0, as n +, we conclude that (1) Q 1/s u n Q 1/s u and Q 1/s v n Q 1/s v a.e. in, as n + ; () Q 1/s u n h 1 and Q 1 s v n h a.e. in, where h 1, h L 1 ( ). Hence, for some positive constant C, where h(x) = C s s 1 Q( x ) F u (u n, v n ) F u (u, v) ) s s s s 1 Q( x ) ( F u (u n, v n ) s 1 + Fu (u, v) s 1 ( C Q( x ) u n s + Q( x ) v n s + Q( x ) u s + Q( x ) v s) h(x), ) ((h 1 (x)) s + (h (x)) s + Q( x ) u s + Q( x ) v s. s Since Q( x ) F u (u n, v n ) F u (u, v) s 1 0 a.e. in, as n +, we see, by the Dominated Convergence Theorem of Lebesgue, that F u (u n, v n ) F u (u, v) s s 1,Q 0, as n +. Similarly, F v (u n, v n ) F v (u, v) s s 1,Q 0, as n +. On the other hand, using Hölder s inequality and the continuous embedding X r,v i L s (, Q), i {1, }, we have, for all (ϕ, ψ) X r, K(u n, v n ) K(u, v), (ϕ, ψ) Q( x ) F u (u n, v n ) F u (u, v) ϕ dx R N + Q( x ) F v (u n, v n ) F v (u, v) ψ dx F u (u n, v n ) F u (u, v) s s 1,Q ϕ s,q + F v (u n, v n ) F v (u, v) s s 1,Q ψ s,q C F u (u n, v n ) F u (u, v) s s 1,Q (ϕ, ψ) + C F v (u n, v n ) F v (u, v) s s 1,Q (ϕ, ψ), for some positive constant C. Using this we see that K(u n, v n ) K(u, v) X r C[ F u (u n, v n ) F u (u, v) s s 1,Q + F v (u n, v n ) F v (u, v) s s 1,Q ] 0, as n +, so that, we obtain K(u n, v n ) K(u, v), (ϕ, ψ) 0, as n + ; that is, K(u n, v n ), (ϕ, ψ) K(u, v), (ϕ, ψ), as n +, for all (ϕ, ψ) X r. Consequently, Q( x )[ϕf u (u n, v n ) + ψf v (u n, v n )]dx Q( x )[ϕf u (u, v) + ψf v (u, v)]dx, (.7) as n +, for all (ϕ, ψ) X r. Moreover, since (u n, v n ) (u, v) in X r and K(u n, v n ) K(u, v) in X r, as n +, it follows that K(u n, v n ), (u n, v n ) K(u, v), (u, v), (.8)

10 R. DEMARQUE, N. H. LISBOA EJDE-018/67 as n + ; that is, Q( x )[F u (u n, v n )u n + F v (u n, v n )v n ]dx Q( x )[F u (u, v)u + F v (u, v)v]dx, as n +. Combining (.5), (.6) and (.7) we obtain I (u n, v n ), (ϕ, ψ) I (u, v), (ϕ, ψ), as n +, for all (ϕ, ψ) X r. Hence, as I (u n, v n ) 0, as n +, we deduce that I (u, v) = 0. This implies 0 = I (u, v), (u, v) = [ u + v ]dx + [V 1 ( x ) u q + V ( x ) v q ]dx K(u, v), (u, v). Therefore, K(u, v), (u, v) = [ u + v ]dx + [V 1 ( x ) u q + V ( x ) v q ]dx. (.9) On the other hand, [ u n + v n ]dx + [V 1 ( x ) u n q + V ( x ) v n q ]dx (.10) = I (u n, v n ), (u n, v n ) + K(u n, v n ), (u n, v n ). From (.8), (.9) and (.10) we have [ u n + v n ]dx + [V 1 ( x ) u n q + V ( x ) v n q ]dx R N (.11) [ u + v ]dx + [V 1 ( x ) u q + V ( x ) v q ]dx, as n +. As before, from the Brezis-Lieb Lemma, we can show that V 1 ( x ) u n q dx V 1 ( x ) u n u q dx V 1 ( x ) u q dx, R N V ( x ) v n q dx V ( x ) v n v q dx R N V ( x ) v q dx, u n dx (u n u) dx u dx, R N v n dx (v n v) dx v dx, as n +. This implies [V 1 ( x ) u n q + V ( x ) v n q ]dx [V 1 ( x ) u n u q + V ( x ) v n v q ]dx [V 1 ( x ) u q + V ( x ) v q ]dx and [ u n + v n ]dx [ (u n u) + (v n v) ]dx R N [ u + v ]dx, (.1) (.13)

EJDE-018/67 INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS 11 as n +. By (.11), (.1) and (.13), we obtain [ (u n u) + (v n v) ]dx + [V 1 ( x ) u n u q + V ( x ) v n v q ]dx 0, as n +. As a consequence, we deduce that ( ) 1/ (u n, v n ) (u, v) = ( (u n u) + (v n v) )dx ( )1/q + (V 1 ( x ) u n u q + V ( x ) v n v q )dx 0, as n +. Therefore, (u n, v n ) (u, v) in X r, as n +. Lemma.5 (Geometry of the Mountain Pass Theorem). The functional I : X r R satisfies the following conditions: (a) I(0, 0) = 0 and there exist c > 0, ρ > 0 such that I(u, v) c for (u, v) = ρ; (b) There exists (u, v) X r, with (u, v) > ρ, such that I(u, v) < 0. Proof. First we note that I(0, 0) = 0. Now, taking q 0 := max{, q} and using the Remark.3 item (b), we conclude that I(u, v) 1 [ ] [ u + v ]dx + [V 1 ( x ) u q + V ( x ) v q ]dx q 0 R N (.14) C Q( x )[ u s + v s ]dx, for some constant C > 0. By the continuous embedding X r,vi L s ( ; Q), i = 1,, we deduce that Q( x ) u s dx C (u, v) s, Q( x ) v s dx C (u, v) s, for some positive constant C. This and (.14) implies that I(u, v) 1 [ ] [ u + v ]dx + [V 1 ( x ) u q + V ( x ) v q ]dx q 0 (.15) C (u, v) s, for some constant C > 0. For 0 < (u, v) < 1, we have (u, v) q0 [( ) q0/ ( q0 ( u + v )dx + (V 1 ( x ) u q + V ( x ) v q ]dx R [ N ] q0 ( u + v )dx + (V 1 ( x ) u q + V ( x ) v q )dx. Combining (.15) with (.16) we obtain I(u, v) 1 q 0 q0 (u, v) q0 C (u, v) s, ) q0/q] (.16) for some positive constant C and for 0 < (u, v) < 1. So, there exist 0 < ρ < 1 sufficiently small and c > 0 such that I(u, v) c > 0 for all (u, v) X, with (u, v) = ρ. This completes the proof of (a).

1 R. DEMARQUE, N. H. LISBOA EJDE-018/67 Fixing (u 0, v 0 ) X r such that F (u 0, v 0 ) > 0, we have, for all t > 0, I(t(u 0, v 0 )) = t [ u 0 + v 0 ]dx + tq [V 1 ( x )(u 0 ) q + V ( x )(v 0 ) q ]dx R q N This implies t s Q( x )F (u 0, v 0 )dx. I(t(u 0, v 0 )) as t +. Thus, for t > 0, sufficiently large, t(u 0, v 0 ) > ρ and I(t(u 0, v 0 )) < 0. Therefore, (b) follows. This completes the proof. Finally, we can prove our main result. Proof of Theorem 1.1. As a consequence of Lemma.4 and Lemma.5, we conclude, by using the Mountain Pass Theorem, due to Ambrosetti-Rabinowitz [8], that there exists a sequence {(u n, v n )} in X so that I(u n, v n ) c > 0 and I (u n, v n ) 0, as n +. By Lemma.4, (u n, v n ) (u, v) in X r, as n +, up to a subsequence. In view of I C 1 (X r, R), it follows that I(u n, v n ) I(u, v) and I (u n, v n ) I (u, v), as n +. This implies that I (u, v) = 0 and I(u, v) = c 0, that is, (u, v) X r is a nontrivial critical point of I. By Lemma., we conclude that (u, v) is a radial solution for the system (1.1) in the sense of equation (1.5). Our next goal is to apply the Symmetric Mountain Pass Theorem [33, Theorem 6.5] to complete the proof of Theorem 1.1. So, we need to show that I satisfies the following conditions: (a) I( (u, v)) = I(u, v), for all (u, v) X r ; (b) For any nontrivial finite dimensional subspace U X r, there exists R > 0 such that I(u, v) 0 for all (u, v) U, with (u, v) R. Since F (u, v) = F ( (u, v)), (a) occurs. Now, suppose that (b) is not true. Therefore, there exists a nontrivial finite dimensional subspace U X r and a sequence {(u n, v n )} in U such that (u n, v n ) +, as n +, and I(u n, v n ) > 0, for all n N. Since U has finite dimension, all norms are equivalent on U. In this case, since F (u, v) η( u s + v s ) for all (u, v) R, we obtain Q( x )F (u n, v n )dx η Q( x )( u n s + v n s )dx = η (u n, v n ) s s,q C (u n, v n ) s, for some positive constant C. Since s > max{, q} = q 0 and (u n, v n ) +, as n +, we deduce that I(u n, v n ) 1 [ u n + v n ]dx + 1 [V 1 ( x ) u n q + V ( x ) v n q ]dx R q N C (u n, v n ) s 1 (u n, v n ) + 1 q (u n, v n ) q C (u n, v n ) s

EJDE-018/67 INHOMOGENEOUS BIHARMONIC ELLIPTIC SYSTEMS 13 ( 1 + 1 q ) (u n, v n ) q0 C (u n, v n ) s, for n sufficiently large and for some positive constant C. As a consequence, lim I(u n, v n ) = ; n + that is, there exists n, sufficiently large, such that I(u n, v n ) < 0, which is a contradiction. This completes the proof of (b). So, by Symmetric Mountain Pass Theorem, there exists an unbounded sequence of critical values for I, which corresponds to the existence of a sequence of nontrivial critical points for I. Consequently, by Lemma., equation (1.5) holds, which completes the proof of Theorem 1.1. Acknowledgments. We wish to thank Professor Olimpio Miyagaki for the suggestions made on an earlier version of this article, and for encouraging us to publish it. We also like to thank the referee for his/her valuable comments and suggestions that certainly improved this article. References [1] W. Allegretto, L. S. Yu; Decaying solutions of -th order elliptic problems, Canad. J. Math., 43 (1991), 449-460. [] C. O. Alves; Local mountain pass for a class of elliptic System, J. Math. Anal. Appl., 335 (007), 135-150. [3] C. O. Alves, D. G. de Figueiredo; Nonvariational elliptic systems, Discr. Contin. Dyn. Syst., 8 (00), 89-30. [4] C. O. Alves, J. M. do Ó; Positive solutions of a fourth-order semilinear problem involving critical growth, Adv. Nonlinear Stud., (00), 437-458. [5] C. O. Alves, J. M. do O, O. H. Miyagaki; Nontrivial solutions for a class of semilinear biharmonic problems involving critical exponents, Nonlinear Anal., 46 (001), 11-133. [6] C. O. Alves, J. M. do Ó, O. H. Miyagaki; On a class singular biharmonic problems involving critical exponent, J. Math. Anal. Appl., 77 (003), 1-6. [7] C. O. Alves, S.H.M. Soares; Existence and concentration of positive solutions for a class gradient systems, NoDEA Nonlinear Differential Equations Appl., 1 (005), 437-457. [8] A. Ambrosetti, P. H. Rabinowitz; Dual variational methods in critical point theory and applications, J. Funct. Anal. 14 (1973), 349-381. [9] F. Bernis, J. Garcia Azorero, I. Peral; Existence and multiplicity of nontrivial solutions in semilinear critical problems of fourth order, Adv. Differential Equations, (1996), 19-40. [10] H. Brezis, E. Lieb; A relation between pointwise convergence of functions and convergence of functionals, Proc. Amer. Math. Soc. 88 (1983), 486-490. [11] P. C. Carrião, R. Demarque, O. H. Miyagaki; Nonlinear biharmonic problems with singular potentials, Comm. on Pure and Appl. Anal. 13 (014), 141-154. [1] P. C. Carrião, N. H. Lisboa, O. H. Miyagaki; Positive radial solutions for a class of elliptic systems concentrating on spheres with potential decay, Bull. Korean Math. Soc. 50 (013), 839-865. [13] P. C. Carrião, N. H. Lisboa, O. H. Miyagaki; Positive solutions for a class of elliptic systems with singular potentials, ZAMP 66 (015), 317-339. [14] P. C. Carrião, O. H. Miyagaki; Existence of non-trivial solutions of elliptic variational systems in unbounded domains, Nonlinear Anal., 51 (00), 155-169. [15] J. Chabrowski, J. M. do Ó; On some fourth order semilinear elliptic problems in RN, Nonlinear Anal., 49 (00), 861-884. [16] Y. Chen, P. J. McKenna; Traveling waves in a nonlinear suspension beam: theoretical results and numerical observations, J. Differential Equations, 135 (1997), 35-355. [17] R. Demarque, O. H. Miyagaki; Radial solutions of inhomogeneous fourth order elliptic equations and weighted Sobolev embeddings, Adv. in Nonlinear Anal., 4 (015), 135-151. [18] L. C. Evans; Partial differential equations, AMS, Providence, Rhode Island, 1998.

14 R. DEMARQUE, N. H. LISBOA EJDE-018/67 [19] Y. Furusho, T. Kusano; Existence of positive entire solutions for higher order quasi-linear elliptic equations, J. Math. Soc. Japan 46, (1994), 449-465. [0] F. Gazzola, H. C. Grunau, G. Sweers; Polyharmonic boundary value problems, Springer- Verlag, Berlin Heidelberg, 010. [1] P. G. Han; Strongly indefinite systems with critical Sobolev exponents and weights, Appl. Math. Lett., 17 (004), 909-917. [] O. Kavian; Introduction theorie des points critiques et applications aux problems elliptiques, Mathematiques et apllications 13, Springer-Verlag, New York/Berlin, 1993. [3] T. Kusano, M. Naito, C. A. Swanson; Radial entire solutions of even order semilinear elliptic equations, Canad. J. Math., 195 (1988), 181-1300. [4] A. C. Lazer, P. J. McKenna; Large-amplitude periodic oscillations in suspension bridges: some new connections with nonlinear analysis, SIAM Rev., 3 (1990), 537-578. [5] Z. X. Liu, P. G. Han; Existence of solutions for singular elliptic systems with critical exponents, Nonlinear Anal., 69 (008), 968-983. [6] Y. Lou; Necessary and sufficient condition for the existence of positive solutions of certain cooperative system, Nonlinear Anal., 6 (1996), 1079-1095. [7] D. Lü, J. Xiao; Multiplicity of solutions for biharmonic elliptic systems involving critical nonlinearity, Bull. Korean Math. Soc. 50 (013), 1693-1710. [8] P. J. McKenna, W. Walter; Traveling waves in a suspension bridge, SIAM J. Appl. Math., 50 (1990), 703-715. [9] D. C. de Morais Filho, M. A. S. Souto; Systems of p-laplacean equations involving homogeneous nonlinearities with critical Sobolev exponent degrees, Comm. Partial Differential Equations 4 (1999), 1537-1553. [30] E. S. Noussair, C. A. Swanson, J. Yang; Critical semilinear biharmonic equation in, Proc. Roy. Soc. Edinburgh Sect. A 11 (199), 139-148. [31] E. S. Noussair, C. A. Swanson, J. Yang; Transcritical biharmonic equations in, Funkcialaj Ekvacioj, 35 (199), 533-543. [3] N. M. Stavrakakis, G. Sweers; Positivity for a noncooperative system of elliptic equations on all of, Adv. Differential Equations 4, (1999), 115-136. [33] M. Struwe; Variational methods, Springer-Velarg, Berlin-Heidelberg, 1990. [34] J. B. Su, Z.-Q. Wang, M. Willem; Weighted Sobolev embedding with unbounded and decaying radial potentials, J. Differential Equations, 38 (007), 01-19. [35] C. A. Swanson; Uniqueness for semilinear polyharmonic problems, Nonlinear Anal., 5 (1995), 1055-106. [36] J. Su, R. Tian; Weighted Sobolev embeddings and radial solutions of inhomogeneous quasilinear elliptic equations, Comm. on Pure and Appl. Anal., 9 (010), 885-904. [37] J. Su, R. Tian; Weighted Sobolev type embeddings and coercive quasilinear elliptic equations on, Proc. Amer. Math. Soc., 140 (01), 891-903. [38] Y. Wang, Y. Shen; Nonlinear biharmonic equations with hardy potential and critical parameter, J. Math. Anal. Appl. 355 (009), 649-660. [39] Y. Wang, Y. Shen; Multiple and sign-changing solutions for a class of semilinear biharmonic equation, J. Differential Equations, 46 (009), 3109-315. [40] H. Xiong, Y. T. Shen; Nonlinear biharmonic equations with critical potential, Acta Math. Sin. (Engl. Ser.), 1 (005), 185-194. [41] W. Zhang, X. Tang, J. Zhang; Infinitely many solutions for fourth-order elliptic equations with sign-changing potential, Taiwanese J. of Math., 18 (014), 645-659. [4] P. H. Zhao, X. Y. Wang; The existence of positive solutions of elliptic system by a linking theorem on product space, Nonlinear Anal., 56 (004), 7-40. Reginaldo Demarque Departamento de Ciências da Natureza, Universidade Federal Fluminense, Rio das Ostras, RJ, 8895-53, Brazil E-mail address: r.demarque@gmail.com Narciso da Hora Lisboa Departamento de Ciências Exatas, Universidade Estadual de Montes Claros, Montes Claros, MG, 39401-089, Brazil E-mail address: narciso.lisboa@unimontes.br