Skip to main content

Existence and multiplicity of positive solutions to a perturbed singular elliptic system deriving from a strongly coupled critical potential

Abstract

In this paper, we consider singular elliptic systems involving a strongly coupled critical potential and concave nonlinearities. By using variational methods and analytical techniques, the existence and multiplicity of positive solutions to the system are established.

MSC: 35J60, 35B33.

1 Introduction and main results

In this paper, we consider the following elliptic system:

{ L u = η 1 α 1 2 | u | α 1 2 | v | β 1 u + η 2 α 2 2 | u | α 2 2 | v | β 2 u + σ 1 | u | q 2 u , L v = η 1 β 1 2 | u | α 1 | v | β 1 2 v + η 2 β 2 2 | u | α 2 | v | β 2 2 v + σ 2 | v | q 2 v , u , v H 0 1 ( Ω ) ,
(1.1)

where Ω R N is a smooth bounded domain such that 0Ω, L:=(Δμ | x | 2 ), 2 := 2 N N 2 is the critical Sobolev exponent, μ ¯ := ( N 2 2 ) 2 is the best Hardy constant and H:= H 0 1 (Ω) denotes the completion of C 0 (Ω) with respect to the norm u 0 = ( Ω | u | 2 d x ) 1 2 and H μ = H μ (Ω) is defined as the completion of the C 0 (Ω) with respect to the norm defined by u μ = ( Ω ( | u | 2 μ u 2 | x | 2 ) d x ) 1 2 for μ< μ ¯ .

Definitions of strongly and weakly coupled terms are as follows.

The terms | u | α and | v | β (α,β>0) are weakly coupled, | L u | α | K v | β (α,β>0) is strongly coupled when L or K is a derivative operator. Thus, η 1 | u | α 1 | v | β 1 + η 2 | u | α 2 | v | β 2 is strongly coupled when η 1 and η 2 are positive.

The parameters in (1.1) satisfy the following assumption.

() N3, 0μ< μ ¯ , 1<q<2, η 1 + η 2 >0, 0 η i <+, σ i >0, α i , β i >1, α i + β i = 2 , i=1,2.

The corresponding energy functional of (1.1) is defined in H×H by

J(u,v):= 1 2 Ω ( | u | 2 + | v | 2 μ | u | 2 + | v | 2 | x | 2 ) dx 1 2 Q(u,v) 1 q K(u,v),

where Q(u,v):= Ω ( η 1 | u | α 1 | v | β 1 + η 2 | u | α 2 | v | β 2 )dx and K(u,v):= Ω ( σ 1 | u | q + σ 2 | v | q )dx. Then J C 1 (H×H,R) and the duality product between H×H and its dual space ( H × H ) 1 is defined as

J ( u , v ) , ( ϕ 1 , ϕ 2 ) : = Ω ( u ϕ 1 + v ϕ 2 μ u ϕ 1 + v ϕ 2 | x | 2 ) d x Ω ( η 1 α 1 2 | u | α 1 2 | v | β 1 u ϕ 1 + η 2 α 2 2 | u | α 2 2 | v | β 2 u ϕ 1 ) d x Ω ( η 1 β 1 2 | u | α 1 | v | β 1 2 v ϕ 2 + η 2 β 2 2 | u | α 2 | v | β 2 2 v ϕ 2 ) d x Ω ( σ 1 | u | q 2 u ϕ 1 + σ 2 | v | q 2 v ϕ 2 ) d x ,

where u,v, ϕ 1 , ϕ 2 H and J (u,v) denotes the Fréchet derivative of J at (u,v). A pair of functions (u,v)H×H is said to be a weak solution of (1.1) if

(u,v)(0,0), J ( u , v ) , ( ϕ 1 , ϕ 2 ) =0,( ϕ 1 , ϕ 2 )H×H.

Therefore, a weak solution of (1.1) is equivalent to a nonzero critical point of J(u,v) [1].

Problem (1.1) is related to the well-known Hardy inequality [2]

R N | u | 2 | x | 2 dx 1 μ ¯ R N | u | 2 dx,u C 0 ( R N ) .
(1.2)

If μ< μ ¯ , by (1.2), Ω ( | u | 2 μ u 2 | x | 2 )dx is an equivalent norm of H, the operator L is positive and the first eigenvalue Λ 1 (μ) of L and the following best constant are well defined:

S(μ):= inf u D 1 , 2 ( R N ) { 0 } R N ( | u | 2 μ u 2 | x | 2 ) d x ( R N | u | 2 d x ) 2 2 ,μ(, μ ¯ ),
(1.3)

where D 1 , 2 ( R N ) is the completion of C 0 ( R N ) with respect to ( R N | u | 2 d x ) 1 2 . Note that S(0) is the well-known best Sobolev constant. For 0μ< μ ¯ , the constant S(μ) is achieved by the following extremal functions [3]:

V μ , ε (x):= ε 2 N 2 U μ ( ε 1 x ) ,ε>0,
(1.4)

where U μ (x)= U μ (|x|) is a radially symmetric function

U μ (x)= ( 2 N ( μ ¯ μ ) μ ¯ ) μ ¯ 2 ( | x | μ ¯ μ ¯ μ μ ¯ + | x | μ ¯ + μ ¯ μ μ ¯ ) μ ¯ .

On the other hand, for any μ< μ ¯ , η 1 + η 2 >0, 0 η i <, α i , β i >1 and α i + β i = 2 , i=1,2, by the Young and Sobolev inequalities, the following best constants are well defined on the space D= ( D 1 , 2 ( R N ) { 0 } ) 2 :

S η , β (μ):= inf ( u , v ) D R N ( | u | 2 + | v | 2 μ | u | 2 + | v | 2 | x | 2 ) d x ( R N ( η 1 | u | α 1 | v | β 1 + η 2 | u | α 2 | v | β 2 ) d x ) 2 2 .
(1.5)

We define

f(τ):= 1 + τ 2 ( η 1 τ β 1 + η 2 τ β 2 ) 2 2 ,τ>0.
(1.6)

Since f is a continuous function on (0,) such that lim τ 0 + f(τ)= lim τ + f(τ)=+. Then there exists τ 0 >0 such that

f( τ 0 ):= min τ > 0 f(τ)>0.
(1.7)

Set α 1 = β 1 , α 2 = β 2 , σ 1 = σ 2 and u=v. Then (1.1) reduces to the semilinear scalar problems that have been extensively investigated by many authors. See [46] and the references therein.

Regular semilinear elliptic systems have been studied extensively and many conclusions have been established. For example, Alves et al. studied in [7] an elliptic system and some important conclusions had been obtained. However, the elliptic systems involving the Hardy inequality have seldom been studied and we only find some results in [816]. Thus it is necessary for us to investigate the related singular systems deeply. Among the references above, the elliptic systems involving the Hardy inequality and concave-convex nonlinearities had been studied only in [12]. In this paper, only the case 1<q<2 of (1.1) involving multiple strongly-coupled critical terms is considered.

Let |Ω| be the Lebesgue measure of Ω. We define the following constant:

ϒ 1 := ( 2 q 2 2 Λ 1 q 2 | Ω | 1 q 2 ) 1 ( 2 q 2 q ( S η , β ( μ ) ) 2 2 ) 2 q 2 2 .
(1.8)

Then the main results of this paper can be concluded in the following theorems and the conclusions are new to the best of our knowledge. It can be verified that the intervals in Theorems 1.1 and 1.2 for the parameters σ 1 , σ 2 , μ and q are allowable.

Theorem 1.1 Suppose that () holds and σ 1 + σ 2 < ϒ 1 . Then problem (1.1) has at least one positive solution.

Theorem 1.2 Suppose that () holds, N>4, μ< μ ¯ ( N q μ ¯ ) 2 and N N 2 <q<2. Then there exists ϒ 2 >0 such that problem (1.1) has at least two positive solutions for all σ 1 and σ 2 satisfying σ 1 + σ 2 < ϒ 2 .

This paper is organized as follows. Some preliminary results and properties of the Nehari manifold are established in Sections 2 and 3, and Theorems 1.1 and 1.2 are proved in Section 4.

2 The local Palais-Smale condition

Throughout this paper, we always assume that the assumption () holds, u H := u μ = ( Ω ( | u | 2 μ | u | 2 | x | 2 ) d x ) 1 / 2 denotes the norm of the space H, by the Hardy inequality μ is equivalent to 0 , i.e.,

( 1 1 μ ¯ max ( μ , 0 ) ) 1 / 2 u 0 u μ ( 1 1 μ ¯ min ( μ , 0 ) ) 1 / 2 u 0 ,uH.

Λ 1 denotes the first eigenvalue of the operator L, z= z H × H = ( u , v ) H × H = ( u H 2 + v H 2 ) 1 / 2 means the norm of the space E:= H 0 1 (Ω)× H 0 1 (Ω), E 1 is the dual space of E. tz=t(u,v)=(tu,tv) for all zE and tR. z=(u,v) is said to be nonnegative in Ω if u0 and v0 in Ω. z=(u,v) is said to be positive in Ω if u>0 and v>0 in Ω. B r (0)={x R N |x|<r} is a ball in R N . O( ε t ) denotes a quantity satisfying |O( ε t )|/ ε t C, o( ε t ) means |o( ε t )|/ ε t 0 as ε0 and o(1) is a generic infinitesimal value. In particular, the quantity O 1 ( ε t ) means that there exist the constants C 1 , C 2 >0 such that C 1 ε t O 1 ( ε t ) C 2 ε t as ε is small. We always denote positive constants as C and omit dx in integrals for convenience.

Lemma 2.1 If { z n }E is a (PS) c -sequence of J with z n z in E, then J (z)=0 and J(z)F( τ 0 ( 1 ) , τ 0 ( 2 ) ), where

Proof Let z n =( u n , v n ) and z=(u,v). Since { z n } is a (PS) c -sequence of J with z n z in E, we can deduce that J (z)=0, and therefore J (z),z=0, that is,

Q(z)= z 2 K(z).

Consequently,

J(z)= ( 1 2 1 2 ) z 2 ( 1 q 1 2 ) K(z).

From the Hölder inequality it follows that

J ( z ) ( 1 2 1 2 ) z 2 ( 1 q 1 2 ) | Ω | 1 q 2 ( σ 1 ( Ω | u | 2 ) q 2 + σ 2 ( Ω | u | 2 ) q 2 ) 1 N z 2 2 q 2 q Λ 1 q 2 | Ω | 1 q 2 ( σ 1 u H q + σ 2 v H q ) F ( τ 0 ( 1 ) , τ 0 ( 2 ) ) .

Thus, the proof is complete. □

Lemma 2.2 If { z n }E is a (PS) c -sequence of the functional J, then { z n } is bounded in E.

Proof See Hsu [[12], Lemma 2.2]. □

Lemma 2.3 Suppose that () holds. Then J satisfies the (PS) c condition for all c< c , where

c = 1 N ( S η , β ( μ ) ) N 2 +F ( τ 0 ( 1 ) , τ 0 ( 2 ) ) .
(2.1)

Proof We follow the argument in [15]. Let { z n }E be a (PS) c -sequence of J with c< c . Write z n =( u n , v n ). We know from Lemma 2.2 that { z n } is bounded in E, and then z n z=(u,v) up to a subsequence, z is a critical point of J. Furthermore, we may assume that u n u, v n v weakly in H and u n u, v n v strongly in L s (Ω) for all 1s< 2 and u n u, v n v a.e. in Ω. Hence, we have that

J (z)=0andK( z n )=K(z)+o(1).
(2.2)

Set u ˜ n = u n u, v ˜ n = v n v and z ˜ n =( u ˜ n , v ˜ n ). From the Brézis-Lieb lemma [17] it follows that

z ˜ n 2 = z n 2 z 2 +o(1),
(2.3)

and by Lemma 2.1 in [18] we have

Ω | u ˜ n | α i | v ˜ n | β i = Ω | u n | α i | v n | β i Ω | u | α i | v | β i +o(1),i=1,2.
(2.4)

Since J( z n )=c+o(1), J ( z n )=o(1) and by (2.2) to (2.4), we can deduce that

1 2 z ˜ n 2 1 2 Q( z ˜ n )=cJ(z)+o(1)
(2.5)

and

z ˜ n 2 Q( z ˜ n )=o(1).

Hence, we may assume that

lim n z ˜ n 2 = lim n Q( z ˜ n )=l.
(2.6)

If l=0, the proof is complete. Assume l>0; then from (2.6) and the definition of S η , β (μ) it follows that

S η , β ( μ ) l 2 2 = lim n S η , β ( μ ) ( Q ( z ˜ n ) ) 2 2 lim n z ˜ n 2 = l ,

which implies that

l ( S η , β ( μ ) ) N 2 .
(2.7)

In addition, from (2.5) to (2.7) and Lemma 2.1, we get

c = ( 1 2 1 2 ) l + J ( z ) 1 N ( S η , β ( μ ) ) N 2 + F ( τ 0 ( 1 ) , τ 0 ( 2 ) ) = c ,

which is a contradiction. Therefore, the proof of Lemma 2.3 is complete. □

3 Nehari manifold

Since J is unbounded below on E, we need to consider J on the Nehari manifold

M σ = { z E { 0 } : J ( z ) , z = 0 } .

Thus, z M σ if and only if

J ( z ) , z = z 2 Q(z)K(z)=0.
(3.1)

By the Hölder inequality and the definition of Λ 1 it follows that

K ( z ) ( σ 1 ( Ω | u | 2 ) q 2 + σ 2 ( Ω | v | 2 ) q 2 ) | Ω | 1 q 2 ( σ 1 ( u H ) q + σ 2 ( v H ) q ) Λ 1 q 2 | Ω | 1 q 2 ( σ 1 + σ 2 ) Λ 1 q 2 | Ω | 1 q 2 z q .
(3.2)

Lemma 3.1 The functional J is coercive and bounded below on M σ .

Proof Suppose that z=(u,v) M σ . From (3.1) and (3.2) we get

J(z)= ( 1 2 1 2 ) z 2 ( 1 q 1 2 ) K(z)
(3.3)
1 N z 2 ( 2 q 2 q ) ( σ 1 + σ 2 ) Λ 1 q 2 | Ω | 1 q 2 z q .
(3.4)

Thus, J is coercive and bounded below on M σ . □

Define Φ(z)= J (z),z. Then for all z=(u,v) M σ we have

Φ ( z ) , z = 2 z 2 2 Q ( z ) q K ( z ) = ( 2 q ) z 2 ( 2 q ) Q ( z )
(3.5)
= ( 2 2 ) z 2 + ( 2 q ) K(z).
(3.6)

We split M σ into three parts:

Lemma 3.2 Suppose that zE is a local minimizer of J on M σ and z M σ 0 . Then J (z)=0 in E 1 .

Proof The proof is similar to that of [19] and the details are omitted. □

Lemma 3.3 M σ 0 = for all σ 1 + σ 2 (0, ϒ 1 ).

Proof We argue by contradiction. Suppose that there exist σ 1 , σ 2 >0 such that 0< σ 1 + σ 2 < ϒ 1 and M σ 0 . Then the fact z=(u,v) M σ 0 together with (3.5) and (3.6) imply that

z 2 = 2 q 2 q Q(z),
(3.7)

and

z 2 = 2 q 2 2 K(z).
(3.8)

By (1.5) and (3.7) we have

z 2 2 q 2 q ( S η , β ( μ ) ) 2 2 z 2 ,

which implies that

z ( 2 q 2 q ( S η , β ( μ ) ) 2 2 ) 1 2 2 .
(3.9)

By (3.2) and (3.8) we have

z ( 2 q 2 2 Λ 1 q 2 | Ω | 1 q 2 ) 1 2 q ( σ 1 + σ 2 ) 1 2 q .
(3.10)

From (3.9) and (3.10) it follows that

σ 1 + σ 2 ( 2 q 2 2 Λ 1 q 2 | Ω | 1 q 2 ) 1 ( 2 q 2 q ( S η , β ( μ ) ) 2 2 ) 2 q 2 2 = ϒ 1 ,

which is a contradiction. □

By Lemma 3.3, we write M σ = M σ + M σ and define

α σ = inf z M σ J(z); α σ ± = inf z M σ ± J(z).

Lemma 3.4

  1. (i)

    α σ α σ + <0 for all σ 1 + σ 2 (0, ϒ 1 ).

  2. (ii)

    There exists a positive constant d 0 depending on σ 1 , σ 2 , q, N, S η , β (μ), Λ 1 and |Ω| such that α σ > d 0 for all σ 1 + σ 2 (0, q 2 ϒ 1 ).

Proof (i) Let z=(u,v) M σ + . By (3.1) and (3.6) it follows that

2 q 2 q z 2 >Q(z).
(3.11)

According to (3.1) and (3.11), we have that

J ( z ) = ( 1 2 1 q ) z 2 + ( 1 q 1 2 ) Q ( z ) < [ ( 1 2 1 q ) + ( 1 q 1 2 ) 2 q 2 q ] z 2 = 2 q q N z 2 < 0 ,

which implies that α σ α σ + <0.

  1. (ii)

    Suppose that σ 1 + σ 2 (0, q 2 ϒ 1 ) and z=(u,v) M σ . By (1.7), (3.1) and (3.5) we have that

    2 q 2 q z<Q(z) ( S η , β ( μ ) ) 2 2 z 2 ,

which implies that

z> ( 2 q 2 q ) 1 2 2 ( S η , β ( μ ) ) 2 2 ( 2 2 ) .
(3.12)

From (3.4) and (3.12) it follows that

J(z) z q ( 1 N z 2 q ( 2 q 2 q ) Λ 1 q 2 | Ω | 1 q 2 ( σ 1 + σ 2 ) ) d 0 ,

where d 0 = d 0 ( σ 1 , σ 2 ,q,N, Λ 1 , S η , β (μ),|Ω|) is a positive constant. □

Lemma 3.5 Suppose that σ 1 + σ 2 (0, ϒ 1 ) and zE with Q(z)>0. Then there exist unique t + , t >0 such that t + z M σ + and t z M σ . In particular, we have

t > t max := ( ( 2 q ) z 2 ( 2 q ) Q ( z ) ) 1 2 2 > t + ,

J( t + z)= min 0 t t max J(tz) and J( t z)= max t t max J(tz).

Proof The proof is similar to that of [20] and is omitted. □

For each zE with K(z)>0, we write

t ¯ max = ( ( 2 q ) K ( z ) ( 2 2 ) z 2 ) 1 2 q >0.

Then we have the following lemma.

Lemma 3.6 Suppose that σ 1 + σ 2 (0, ϒ 1 ) and zE{(0,0)} with K(z)>0. Then there exist unique 0< t + < t ¯ max < t such that t + z M σ + , t z M σ and

J ( t + z ) = inf 0 t t ¯ max J(tz);J ( t z ) = sup t 0 J(tz).

Proof The proof is almost the same as that in [[20], Lemma 2.7] and is omitted here. □

4 Proof of Theorems 1.1 and 1.2

Lemma 4.1

  1. (i)

    If σ 1 + σ 2 (0, ϒ 1 ), then the functional J has a (PS)-sequence { z n } M σ .

  2. (ii)

    If σ 1 + σ 2 (0, q 2 ϒ 1 ), then the functional J has a ( PS ) α σ -sequence { z n } M σ .

Proof The proof is similar to that of [21] and is omitted. □

Lemma 4.2 Suppose that σ 1 + σ 2 (0, ϒ 1 ). Then J has a minimizer z ( 1 ) M σ + such that z ( 1 ) is a positive solution of (1.1) and J( z ( 1 ) )= α σ = α σ + <0.

Proof By Lemma 4.1(i), there exists a (PS)-sequence { z n } M σ of J such that

J( z n )= α σ +o(1)and J ( z n )=o(1)in  E 1 .
(4.1)

Since J is coercive on M σ (see Lemma 3.1), we get that { z n } is bounded in E. Passing to a subsequence (still denoted by { z n }), we can assume that there exists z ( 1 ) =( u ( 1 ) , v ( 1 ) )E such that

{ u n u ( 1 ) , v n v ( 1 ) weakly in  H , u n u ( 1 ) , v n v ( 1 ) a.e. in  Ω , u n u ( 1 ) , v n v ( 1 ) strongly in  L s ( Ω )  for all  1 s < 2 ,
(4.2)

which implies that

K( z n )=K ( z ( 1 ) ) +o(1)as n.
(4.3)

First, we claim that z ( 1 ) is a solution of (1.1). By (4.1) and (4.2), it is easy to see that z ( 1 ) is a solution of (1.1). Furthermore, from { z n } M σ and (3.3), we deduce that

K( z n )= q ( 2 2 ) 2 ( 2 q ) z n 2 2 q 2 q J( z n ).
(4.4)

Taking n in (4.4), by (4.1), (4.2) and the fact α σ <0, we get

K ( z ( 1 ) ) 2 q 2 q α σ >0.

Therefore, z ( 1 ) M σ is a nontrivial solution of (1.1).

Next, we prove that z n z ( 1 ) strongly in E and J( z ( 1 ) )= α σ . Noting z ( 1 ) M σ and applying the Fatou lemma, we have

α σ J ( z ( 1 ) ) = 1 N z ( 1 ) 2 2 q 2 q K ( z ( 1 ) ) lim inf n ( 1 N z n 2 2 q 2 q K ( z n ) ) = lim inf n J ( z n ) = α σ .

Therefore, J( z ( 1 ) )= α σ and lim n z n 2 = z ( 1 ) 2 . Set z ˜ n = z n z ( 1 ) . By the Brézis-Lieb lemma [17], we get

z ˜ n 2 = z n 2 z ( 1 ) 2 +o(1).

Then standard argument shows that z n z ( 1 ) strongly in E. Moreover, we have z ( 1 ) M σ + . Otherwise, if z ( 1 ) M σ , then by Lemma 3.5 there exist unique t 0 ± such that t 0 ± z ( 1 ) M σ ± and t 0 + < t 0 =1. Since

d d t J ( t 0 + z ( 1 ) ) =0and d 2 d t 2 J ( t 0 + z ( 1 ) ) >0,

there exists t ¯ ( t 0 + , t 0 ) such that J( t 0 + z ( 1 ) )<J( t ¯ z ( 1 ) ). By Lemma 3.5 we get that

J ( t 0 + z ( 1 ) ) <J ( t ¯ z ( 1 ) ) J ( t 0 z ( 1 ) ) =J ( z ( 1 ) ) ,

which is a contradiction. Since J( z ( 1 ) )=J(| z ( 1 ) |) and | z ( 1 ) | M σ + , by Lemma 3.2 we may assume that z ( 1 ) is a nontrivial nonnegative solution of (1.1).

In particular u ( 1 ) 0, v ( 1 ) 0. Indeed, without loss of generality, we may assume that v ( 1 ) 0. Then as u ( 1 ) is a nontrivial nonnegative solution of

{ Δ u μ u | x | 2 = σ 1 | u | q 2 u in  Ω , u = 0 on  Ω ,

by the standard regularity theory, we have u ( 1 ) >0 in Ω and

( u ( 1 ) , 0 ) 2 =K ( u ( 1 ) , 0 ) >0.

Moreover, we may choose w H 0 1 (Ω){0} such that

( 0 , w ) 2 =K(0,w)>0.

Now,

K ( u ( 1 ) , w ) =K ( u ( 1 ) , 0 ) +K(0,w)>0

and so by Lemma 3.6 there is unique 0< t + < t ¯ max such that ( t + u ( 1 ) , t + w) M σ + . Moreover,

t ¯ max = ( ( 2 q ) K ( u ( 1 ) , w ) ( 2 2 ) ( u ( 1 ) , w ) 2 ) = ( 2 q 2 2 ) 1 / ( 2 q ) >1

and

J ( t + u ( 1 ) , t + w ) = inf 0 t t ¯ max J ( t u ( 1 ) , t w ) .

This implies

α σ + J ( t + u ( 1 ) , t + w ) J ( u ( 1 ) , w ) <J ( u ( 1 ) , 0 ) = α σ +

which is a contradiction.

Finally, from the maximum principle [22] we deduce that z ( 1 ) >0 in Ω and z ( 1 ) is thus a positive solution of (1.1). □

Let V μ , ε (x) be defined as in (1.4) and set u ε (x)=ψ(x) V μ , ε (x), where ψ(x) is a cut-off function:

ψ(x) D (Ω):= { ψ C 0 ( Ω ) : ψ ( x ) 1  in a neighborhood of  x = 0 } .

The following results are already known.

Lemma 4.3 [4]

As ε0 we have the following estimates:

(4.5)
(4.6)
(4.7)

Lemma 4.4 [11]

Suppose that () holds, f(τ) is defined as in (1.6) and V μ , ε (x) are the minimizers of S(μ) defined as in (1.4). Then S η , β (μ)=f( τ 0 )S(μ) and has the minimizers ( V μ , ε (x), τ 0 V μ , ε (x)), where f( τ 0 ):= min τ 0 f(τ)>0.

Lemma 4.5 Under the assumptions of Theorem 1.2, there exist z ˜ E{0} and Λ >0 such that for all σ 1 + σ 2 < Λ there holds

sup t 0 J(t z ˜ )< c = 1 N ( S η , β ( μ ) ) N 2 +F ( τ 0 ( 1 ) , τ 0 ( 2 ) ) .
(4.8)

In particular, α σ < c for all σ 1 + σ 2 < Λ .

Proof For all t0, define the functions g 1 (t):=J(t u ε ,t τ 0 u ε ) and

g 2 (t):= t 2 2 ( 1 + ( τ 0 ) 2 ) u ε H 2 t 2 2 ( η 1 ( τ 0 ) β 1 + η 2 ( τ 0 ) β 2 ) Ω | u ε | 2 .

Note that lim t + g 2 (t)= and g 2 (t)>0 as t is closed to 0. Thus, sup t 0 g 2 (t) is attained at some finite t ε >0 with g 2 ( t ε )=0. Furthermore, C < t ε < C , where C and C are the positive constants independent of ε.

Choose δ 1 >0 small enough such that c >0 for all σ 1 + σ 2 < δ 1 . Set z ε =( u ε , τ 0 u ε ). Then J(t z ε ) t 2 2 z ε 2 for all t0 and σ 1 , σ 2 >0, which implies that there exists t 0 (0,1) satisfying sup 0 t t 0 J(t z ε )< c , for all σ 1 + σ 2 < δ 1 . Note that

max t 0 ( t 2 2 B 1 t 2 2 B 2 ) = 1 N ( B 1 B 2 2 2 ) N 2 , B 1 , B 2 >0.
(4.9)

From (4.9) and Lemmas 4.3, 4.4 it follows that

g 2 ( t ε ) 1 N ( ( 1 + ( τ 0 ) 2 ) u ε H 2 ( ( η 1 ( τ 0 ) β 1 + η 2 ( τ 0 ) β 2 ) Ω | u ε | 2 ) 2 2 ) N 2 1 N ( f ( τ 0 ) S ( μ ) N 2 + O ( ε 2 μ ¯ μ ) ( S ( μ ) N 2 + O ( ε 2 μ ¯ μ ) ) 2 2 ) N 2 1 N ( f ( τ 0 ) S ( μ ) ) N 2 + O ( ε 2 μ ¯ μ ) = 1 N ( S η , β ( μ ) ) N 2 + O ( ε 2 μ ¯ μ ) .

Consequently,

sup t t 0 g 1 ( t ) < sup t t 0 ( g 2 ( t ) t q q K ( z ε ) ) 1 N ( S η , β ( μ ) ) N 2 + O ( ε 2 μ ¯ μ ) t 0 q q ( σ 1 + ( τ 0 ) q σ 2 ) Ω | u ε | q 1 N ( S η , β ( μ ) ) N 2 + O ( ε 2 μ ¯ μ ) C ( σ 1 + σ 2 ) Ω | u ε | q 1 N ( S η , β ( μ ) ) N 2 + O ( ε 2 μ ¯ μ ) ( σ 1 + σ 2 ) O 1 ( ε N q μ ¯ )

and

(Nq μ ¯ ) 2 q q <2 μ ¯ μ (Nq μ ¯ ),

where we have used the assumption μ< μ ¯ ( N q μ ¯ ) 2 .

Therefore we can choose σ 1 = O 1 ( ε r 1 ), σ 2 = O 1 ( ε r 2 ) such that

The definition of F( τ 0 ( 1 ) , τ 0 ( 2 ) ) in Lemma 2.1 implies that

F ( τ 0 ( 1 ) , τ 0 ( 2 ) ) = O 1 ( ε 2 2 q min ( r 1 , r 2 ) ) .

Note that

Taking ε small enough, there exists δ 2 >0 such that for all 0< σ 1 + σ 2 < δ 2 ,

O ( ε 2 μ ¯ μ ) ( σ 1 + σ 2 ) O 1 ( ε N q μ ¯ ) <F ( τ 0 ( 1 ) , τ 0 ( 2 ) ) .
(4.10)

Choose Λ =min{ δ 1 , δ 2 }>0. Then for all σ 1 + σ 2 (0, Λ ) there holds

sup t 0 J(t z ε )< c .
(4.11)

Finally, we prove that α σ < c for all σ 1 + σ 2 < Λ . Recall that z ε =( u ε , τ 0 u ε ). By Lemma 3.5, the definition of α σ and (4.11), we can deduce that there exists t ˜ 0 >0 such that t ˜ 0 z ε M σ and

α σ J( t ˜ 0 z ε ) sup t 0 J( t ˜ 0 z ε )< c .

The proof is thus complete by taking z ˜ = z ε . □

Lemma 4.6 Set ϒ 2 :=min{ Λ , q 2 ϒ 1 }. Then for all σ 1 + σ 2 (0, ϒ 2 ), problem (1.1) has a positive solution z ( 2 ) such that z ( 2 ) M σ and J( z ( 2 ) )= α σ .

Proof By Lemma 4.1, there exists a (PS) α σ -sequence { z n } M σ of J for all σ 1 + σ 2 < q 2 ϒ 1 . From Lemmas 2.3, 3.4 and 4.5, it follows that α σ >0 and J satisfies the (PS) α σ condition for all σ 1 + σ 2 < ϒ 2 . Since J is coercive on M σ , we get that { z n } is bounded in E. Therefore, there exist a subsequence (still denoted by { z n }) and z ( 2 ) =( u ( 2 ) , v ( 2 ) ) M σ such that z n z ( 2 ) strongly in E and J( z ( 2 ) )= α σ >0 for all σ 1 + σ 2 < ϒ 2 . Since J( z ( 2 ) )=J(| z ( 2 ) |) and | z ( 2 ) | M σ , by Lemma 3.2 we may assume that z ( 2 ) is a nontrivial nonnegative solution of (1.1). Moreover, by (3.7) and z ( 2 ) =( u ( 2 ) , v ( 2 ) ) M σ , we get

Q ( z ( 2 ) ) = 2 q 2 q z ( 2 ) 2 >0.

This implies that u ( 2 ) 0 and v ( 2 ) 0. From the strong maximum principle [22] it follows that z ( 2 ) is a positive solution of (1.1). □

Proof of Theorems 1.1 and 1.2. By Lemma 4.2, we obtain that (1.1) has a positive solution z ( 1 ) M σ + for all σ 1 + σ 2 < ϒ 1 . On the other hand, from Lemma 4.6, we can get the second positive solution z ( 2 ) M σ for all σ 1 + σ 2 < ϒ 2 < ϒ 1 . Since M σ + M σ =, this implies that z ( 1 ) and z ( 2 ) are distinct. □

References

  1. Rabinowitz P CBMS Regional Conference Series in Mathematics 65. In Minimax Methods in Critical Point Theory with Applications to Differential Equations. Am. Math. Soc, Providence; 1986.

    Google Scholar 

  2. Hardy G, Littlewood J, Polya G: Inequalities. Cambridge University Press, Cambridge; 1952.

    Google Scholar 

  3. Terracini S: On positive solutions to a class of equations with a singular coefficient and critical exponent. Adv. Differ. Equ. 1996, 2: 241-264.

    MathSciNet  Google Scholar 

  4. Kang D, Peng S: Solutions for semilinear elliptic problems with critical Sobolev-Hardy exponents and Hardy potential. Appl. Math. Lett. 2005, 18: 1094-1100. 10.1016/j.aml.2004.09.016

    Article  MathSciNet  Google Scholar 

  5. Cao D, Kang D: Solutions of quasilinear elliptic problems involving a Sobolev exponent and multiple Hardy-type terms. J. Math. Anal. Appl. 2007, 333: 889-903. 10.1016/j.jmaa.2006.12.005

    Article  MathSciNet  Google Scholar 

  6. Kang D: On the quasilinear elliptic problems with critical Sobolev-Hardy exponents and Hardy terms. Nonlinear Anal. 2008, 68: 1973-1985. 10.1016/j.na.2007.01.024

    Article  MathSciNet  Google Scholar 

  7. Alves C, Filho D, Souto M: On systems of elliptic equations involving subcritical or critical Sobolev exponents. Nonlinear Anal. 2000, 42: 771-787. 10.1016/S0362-546X(99)00121-2

    Article  MathSciNet  Google Scholar 

  8. Abdellaoui B, Felli V, Peral I:Some remarks on systems of elliptic equations doubly critical in the whole R N . Calc. Var. Partial Differ. Equ. 2009, 34: 97-137. 10.1007/s00526-008-0177-2

    Article  MathSciNet  Google Scholar 

  9. Bouchekif M, Nasri Y: On elliptic system involving critical Sobolev-Hardy exponents. Mediterr. J. Math. 2008, 5: 237-252. 10.1007/s00009-008-0147-0

    Article  MathSciNet  Google Scholar 

  10. Bouchekif M, Nasri Y: On a singular elliptic system at resonance. Ann. Mat. Pura Appl. 2010, 189: 227-240. 10.1007/s10231-009-0106-9

    Article  MathSciNet  Google Scholar 

  11. Cai M, Kang D: Elliptic systems involving multiple strongly-coupled critical terms. Appl. Math. Lett. 2012, 25: 417-422. 10.1016/j.aml.2011.09.026

    Article  MathSciNet  Google Scholar 

  12. Hsu TS: Multiplicity of positive solutions for critical singular elliptic systems with concave-convex nonlinearities. Adv. Nonlinear Stud. 2009, 9: 295-311.

    MathSciNet  Google Scholar 

  13. Huang Y, Kang D: On the singular elliptic systems involving multiple critical Sobolev exponents. Nonlinear Anal. 2011, 74: 400-412. 10.1016/j.na.2010.08.051

    Article  MathSciNet  Google Scholar 

  14. Huang Y, Kang D: Elliptic systems involving the critical exponents and potentials. Nonlinear Anal. 2009, 71: 3638-3653. 10.1016/j.na.2009.02.024

    Article  MathSciNet  Google Scholar 

  15. Liu Z, Han P: Existence of solutions for singular elliptic systems with critical exponents. Nonlinear Anal. 2008, 69: 2968-2983. 10.1016/j.na.2007.08.073

    Article  MathSciNet  Google Scholar 

  16. Wang L, Wei Q, Kang D: Existence and multiplicity of positive solutions to elliptic systems involving critical exponents. J. Math. Anal. Appl. 2011, 383: 541-552. 10.1016/j.jmaa.2011.05.053

    Article  MathSciNet  Google Scholar 

  17. Brézis H, Lieb E: A relation between pointwise convergence of functions and convergence of functionals. Proc. Am. Math. Soc. 1983, 88: 486-490.

    Article  Google Scholar 

  18. Han P: The effect of the domain topology on the number of positive solutions of elliptic systems involving critical Sobolev exponents. Houst. J. Math. 2006, 32: 1241-1257.

    Google Scholar 

  19. Brown KJ, Zhang Y: The Nehari manifold for a semilinear elliptic equation with a sign-changing weigh function. J. Differ. Equ. 2003, 193: 481-499. 10.1016/S0022-0396(03)00121-9

    Article  MathSciNet  Google Scholar 

  20. Brown KJ, Wu TF: A semilinear elliptic system involving nonlinear boundary condition and sign-changing weigh function. J. Math. Anal. Appl. 2008, 337: 1326-1336. 10.1016/j.jmaa.2007.04.064

    Article  MathSciNet  Google Scholar 

  21. Wu TF: On semilinear elliptic equations involving concave-convex nonlinearities and sign-changing weight function. J. Math. Anal. Appl. 2006, 318: 253-270. 10.1016/j.jmaa.2005.05.057

    Article  MathSciNet  Google Scholar 

  22. Vazquez J: A strong maximum principle for some quasilinear elliptic equations. Appl. Math. Optim. 1984, 12: 191-202. 10.1007/BF01449041

    Article  MathSciNet  Google Scholar 

Download references

Acknowledgements

The author was grateful for the referee’s helpful suggestions and comments.

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Tsing-San Hsu.

Additional information

Competing interests

The author declares that he has no competing interests.

Rights and permissions

Open Access This article is distributed under the terms of the Creative Commons Attribution 2.0 International License (https://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Reprints and Permissions

About this article

Cite this article

Hsu, TS. Existence and multiplicity of positive solutions to a perturbed singular elliptic system deriving from a strongly coupled critical potential. Bound Value Probl 2012, 116 (2012). https://doi.org/10.1186/1687-2770-2012-116

Download citation

  • Received:

  • Accepted:

  • Published:

  • DOI: https://doi.org/10.1186/1687-2770-2012-116

Keywords

  • Palais-Smale condition
  • Nehari manifold
  • strongly coupled
  • elliptic system
  • critical potential