Startseite Multiple solutions for a class of fourth-order elliptic equations with critical growth
Artikel Open Access

Multiple solutions for a class of fourth-order elliptic equations with critical growth

  • Guaiqi Tian , Jun Lei und Yucheng An EMAIL logo
Veröffentlicht/Copyright: 25. April 2025

Abstract

In this article, we study the semilinear biharmonic problem with a critical growth:

Δ 2 u = μ Q ( x ) u p 2 u + V ( x ) u 2 * * 2 u in Ω , u = Δ u = 0 on Ω ,

where Ω R N ( N > 4 ) is a smooth bounded domain, μ > 0 , 1 < p < 2 , and 2 * * = 2 N ( N 4 ) is the critical Sobolev exponent. By using the Nehari method and the critical point theory, at least k nontrivial solutions of the above equations for μ sufficiently small and under some appropriate assumptions on Q and V are obtained.

MSC 2010: 35J35; 35J40; 47J65

1 Introduction and main result

The article considers semilinear biharmonic elliptic problem as follows:

(1.1) Δ 2 u = μ Q ( x ) u p 2 u + V ( x ) u 2 * * 2 u in Ω , u = Δ u = 0 on Ω ,

where Ω R N ( N > 4 ) is a smooth bounded domain, μ > 0 , 1 < p < 2 , and 2 * * = 2 N ( N 4 ) is the critical Sobolev exponent, Q L r ( Ω ) with r = 2 * * 2 * * p is nonzero and nonnegative, and V C ( Ω ¯ ) is a positive function.

In recent years, elliptical systems are favored by many researchers, and many results were obtained under different conditions, see [14]. Furthermore, biharmonic equations have a wide range of applications. For example, problem (1.1) arises in the study of travelling waves in a suspension bridge [5], and the study of the static deflection of an elastic plate in a fluid [6]. After that, many important results have been obtained by many scholars, see [714] and references therein. Specifically, in [8], Deng ad Wei consider the existence of nontrivial solutions to the following biharmonic problem with critical nonlinearity

Δ 2 u + V ( x ) u = μ K ( x ) f ( u ) + P ( x ) u 2 * * 2 u , x R N , u D 2,2 ( R N ) ,

where D 2,2 ( R N ) = { u L 2 * * ( R N ) : Δ u L 2 < } , N > 4 , μ > 0 , and 2 * * = 2 N ( N 4 ) , the positive continuous functions V ( x ) and K ( x ) disappear at infinity. Using the variational method, they obtained at least one nontrivial solution of the above problem. And, Cheng et al. in [7] studied the following equation:

(1.2) Δ 2 u = f ( x ) u q 1 u + h ( x ) u p 1 u in Ω , u = Δ u = 0 on Ω ,

where Ω is a bounded smooth domain in R N ( N > 4 ) , f ( x ) , h ( x ) , p , q satisfy some suitable assumptions. Applying the Nehari manifold method along with the fibering maps and minimization method, the effect of f ( x ) and h ( x ) on the existence and multiplicity of nontrivial solutions for equation (1.2). Recently, in [11], Liao et al. considered the following elliptic equations involving the critical Sobolev exponent

Δ u = g ( x ) u 2 * 2 u + λ f ( x ) u q 2 u in Ω , u = 0 on Ω ,

here Ω R N ( N 3 ) is an open-bounded domain with smooth boundary, λ > 0 , 1 < q < 2 , 2 * = 2 N ( N 2 ) , and under some appropriate assumptions on f ( x ) and g ( x ) . By the Nehari method and variational method, k + 1 positive solutions are obtained. Here, motivated by the above references, what we are going to study is the existence of at least k nontrivial solutions of (1.1).

The space H 0 2 ( Ω ) is a Sobolev space equipped with the norm u = ( Ω Δ u 2 d x ) 1 2 . The norm in L r ( Ω ) is represented as u r = ( Ω u p d x ) 1 r . Let S be the optimal constant for the Sobolev embedding H 0 2 ( Ω ) L 2 * * ( Ω ) , namely

(1.3) S = inf u H 0 2 ( Ω ) \ { 0 } Ω Δ u 2 d x Ω u 2 * * d x 2 2 * * .

It is well known that

(1.4) U ( x ) = [ N ( N + 2 ) ( N 2 ) ( N 4 ) ] N 4 8 ( 1 + x 2 ) N 4 2 , x R N ,

is an extremal function (see [8] or [15]); that is, it is a positive solution of the following problem

Δ 2 u = u 2 * * 2 u , in R N ,

satisfying

U 2 = U 2 * * 2 * * = S N 4 .

In the following, for problem (1.1), we define the functional

I μ ( u ) = 1 2 Ω Δ u 2 d x μ p Ω Q ( x ) u p d x 1 2 * * Ω V ( x ) u 2 * * d x .

We know that the functional I μ ( u ) belongs to class C 1 on H 0 2 ( Ω ) , and every critical point of I μ ( u ) exactly corresponds to a solution of (1.1).

In this article, we posit that Q and V meet the following conditions:

( Q ) Q L r ( Ω ) with Q 0 , and Q 0 , where r = 2 * * 2 * * p .

( V ) There exist k points b 1 , b 2 , , b k in Ω satisfying

{ b 1 , b 2 , , b k } = { x Ω : V ( x ) = V M = max h Ω V ( h ) = 1 } ,

and moreover,

V ( x ) V ( b i ) = o ( x b i N 4 2 ) , x b i ,

uniformly for i N + , where 1 i k .

We say that u H 0 2 ( Ω ) is a weak solution of problem (1.1), if for every v H 0 2 ( Ω ) , there holds

Ω Δ u Δ v d x μ Ω Q ( x ) u p 1 v d x Ω V ( x ) u 2 * * 1 v d x = 0 .

Therefore, if the solution exists, it must lie in the Nehari manifold N μ , which is defined by

N μ = u H 0 2 ( Ω ) : Ω Δ u 2 d x = μ Ω Q ( x ) u p d x + Ω V ( x ) u 2 * * d x .

Theorem 1.1

Let 1 < p < 2 , V C ( Ω ¯ ) be a positive function. Suppose that Q and V satisfy the hypotheses ( Q ) and ( V ) , respectively. Thus, there exists Γ * > 0 such that for μ ( 0 , Γ * ) , problem (1.1) has at least k nontrivial solutions.

Remark 1.2

Theorem 1.1 generalizes the results found in [7, 8]. In fact, the authors in [7] studied only the case that μ = 1 and subcritical case. Meanwhile, only one nontrivial solution is obtained in [8]. Hence, our result is new and interesting.

2 Some preliminary results

We present several lemmas that are crucial for proving our main results.

Lemma 2.1

Suppose that 1 < p < 2 and N > 4 , then, N μ . Furthermore, I μ is coercive and bounded below on N μ for all μ > 0 .

Proof

First, for u H 0 2 ( Ω ) , we define a firbering map J u : t I μ ( t u ) by

J u ( t ) = t 2 2 Ω Δ u 2 d x μ t p p Ω Q ( x ) u p d x t 2 * * 2 * * Ω V ( x ) u 2 * * d x ,

from the above equation, we see that J u ( 0 ) = 0 and J u ( t ) as t + . Besides, we have

J u ( t ) = t Ω Δ u 2 d x μ t p 2 Ω Q ( x ) u p d x t 2 * * 2 Ω V ( x ) u 2 * * d x ,

therefore, there exists unique a t u > 0 such that

J u ( t u ) = t u Ω Δ u 2 d x μ t u p 1 Ω Q ( x ) u p d x t u 2 * * 1 Ω V ( x ) u 2 * * d x = 0 ,

and then t u u N μ . Thus, N μ .

Second, by the Hölder and Sobolev inequalities, we know

(2.1) Ω Q ( x ) u p d x S p 2 Q r u p .

So, for each u N μ , from (2.1) and the Young’s inequality, we obtain

(2.2) I μ ( u ) = 1 2 Ω Δ u 2 d x μ p Ω Q ( x ) u p d x 1 2 * * Ω V ( x ) u 2 * * d x 2 N Ω Δ u 2 d x μ 1 p 1 2 * * S p 2 Q r u p 4 + N p 2 N Ω Δ u 2 d x μ 2 2 p 2 p 2 2 * * p 2 * * p S p 2 Q r 2 2 p .

Since 1 < p < 2 < 2 * * , I μ is coercive and bounded below on N μ for any μ > 0 .□

By the fact that V is nonnegative continuous on Ω ¯ and ( V ) , we can choose r 0 > 0 such that

B r 0 ( b i ) ¯ B r 0 ( b j ) ¯ = for i j and 1 i , j k ,

and i = 1 k B r 0 ( b i ) ¯ Ω , here B r 0 ( b i ) ¯ = { x R N x b i r 0 } . Let K r 0 2 = i = 1 k B r 0 2 ( b i ) , assume that i = 1 k B r 0 ( b i ) ¯ B ρ 0 ( 0 ) for some ρ 0 > 0 . By [16], let ϕ : H 0 2 ( Ω ) \ { 0 } R N be a barycenter map defined by

ϕ ( u ) = Ω χ ( z ) u 2 * * d z Ω u 2 * * d z ,

where χ : R N R N

χ ( z ) = z , z ρ 0 , ρ 0 z z , z > ρ 0 .

For every 1 i k , define

O μ i = { u N μ ϕ ( u ) b i < r 0 } , O μ i = { u N μ ϕ ( u ) b i = r 0 }

and

β μ i = inf u O μ i I μ ( u ) and β μ i ˜ = inf u O μ i I μ ( u ) .

In addition, consider the following critical exponent problem

(2.3) Δ 2 u = u 2 * * 2 u in Ω , u = Δ u = 0 on Ω .

We consider the energy functional associated with (2.3), that is

I ( u ) = 1 2 Ω Δ u 2 d x 1 2 * * Ω u 2 * * d x .

Now, similar to [17], let η i C 0 be a radially symmetric function such that 0 η i 1 , Δ η i C i for 1 i k , where C i are some positive constants, we define

η i ( x ) = 1 , x b i δ ˜ 2 , 0 , x b i δ ˜

and

v ε i ( x ) = ε N 4 2 η i ( x ) U x b i ε = η i [ N ( N + 2 ) ( N 2 ) ( N 4 ) ε 4 ] N 4 8 [ ε 2 + x b i 2 ] N 4 2 ,

where U ( x ) is defined by (1.4). From Lemma 2.1, there exists t ε i > 0 , such that t ε i v ε i N μ for each 1 i k . Then, we state the following proposition.

Proposition 2.2

For 1 i k , then β μ i > 0 for each μ ( 0 , Γ ) . And, ϕ ( t ε i v ε i ) b i as ε 0 + . Additionally, there exists ε 0 > 0 , such that for all 0 < ε < ε 0 , then, ϕ ( t ε i v ε i ) K r 0 2 for each 1 i k .

Proof

For every u N μ , by (2.1), we have

I μ ( u ) = 1 2 Ω Δ u 2 d x μ p Ω Q ( x ) u p d x 1 2 * * Ω V ( x ) u 2 * * d x 2 N Ω Δ u 2 d x μ 1 p 1 2 * * S p 2 Q r u p .

Since 1 < q < 2 < 2 * * , β μ i > 0 for all μ ( 0 , Γ ) .

By the definition of ϕ , we have

ϕ ( t ε i v ε i ) = Ω χ ( x ) ε 4 N 2 t ε i η i ( x ) U x b i ε 2 * * d x Ω ε 4 N 2 t ε i η i ( x ) U x b i ε 2 * * d x = Ω χ ( b i + ε x ) t ε i η i ( b i + ε x ) U ( x ) 2 * * d x Ω t ε i η i ( b i + ε x ) U ( x ) 2 * * d x Ω χ ( b i ) U ( x ) 2 * * d z Ω U ( x ) 2 * * d z = b i ,

as ε 0 + . This indicates that there exists ε 0 > 0 , such that ϕ ( t ε i v ε i ) K r 0 2 for any 0 < ε < ε 0 and 1 i k .□

Proposition 2.3

There exists Γ 0 > 0 , such that

β μ i ˜ > 2 N S N 4 ,

for each 0 < μ < Γ 0 , and for all 1 i k .

Proof

We prove this proposition by contradiction. Assume that there exists a positive sequence { μ n } with μ n 0 as n , such that β μ i ˜ m ˜ 2 N S N 4 for some 1 i k . Hence, there exists a sequence { u n } O μ i such that I μ n ( u n ) m ˜ as n . For every 0 < μ n < Γ 0 , it follows that { u n } is bounded in H 0 2 ( Ω ) , and

(2.4) Ω Δ u n 2 d x μ n Ω Q ( x ) u n p d x Ω V ( x ) u n 2 * * d x = 0 .

Moreover,

lim n μ n Ω Q ( x ) u n p d x = 0 .

From (2.4), fixed a constant l > 0 , by the Hölder and Sobolev inequalities, one obtains

Ω Δ u n 2 d x l , Ω V ( x ) u n 2 * * d x l .

By considering a subsequence of { u n } , it follows that

lim n Ω Δ u n 2 d x = lim n Ω V ( x ) u n 2 * * d x = l > 0 .

Moreover, one obtains

(2.5) l V M Ω u n 2 * * d x V M S 2 * * 2 lim n Ω Δ u n 2 d x 2 * * 2 V M S 2 * * 2 l 2 * * 2 .

Then, we have l S N 4 . In addition, as n , we have

(2.6) 2 N l + 1 2 * * Ω V ( x ) u n 2 * * d x = 1 2 Ω Δ u n 2 d x + o ( 1 ) = I μ n ( u n ) + o ( 1 ) 2 N S N 4 .

It follows from (2.5) and (2.6) that l = S N 4 . Consequently, from (2.5), one obtains

lim n Ω V M u n 2 * * d x = S N 4 = l .

Therefore, we know

(2.7) lim n Ω ( V M V ( x ) ) u n 2 * * d x = 0 .

Set ω n = u n u n 2 * * , then, ω n 2 * * = 1 , and

lim n Ω Δ ω n 2 d x = lim n Ω Δ u n 2 d x u n 2 * * 2 = S .

Hence, { ω n } is a minimizing sequence for S . According to [18], there exists a x 0 Ω ¯ such that

Δ ω n 2 d μ = S δ x 0 , ω n 2 * * d ν = δ x 0 ,

weakly in the sense of measure, here μ and ν are finite measures, and δ x 0 is the Dirac measure at x 0 . Since ω n O μ i , as n , it follows that

ϕ ( ω n ) = Ω χ ( z ) ω n 2 * * d z Ω ω n 2 * * d z x 0 ,

which implies that x 0 O μ i , and x 0 b i for 1 i k . Additionally, from (2.7), we deduce

V M = lim n Ω V M ω n 2 * * d x = lim n Ω V ( x ) ω n 2 * * d x = V ( x 0 ) ,

which yields a contradiction.□

Lemma 2.4

For u O μ i , there exist τ > 0 , and a differentiable functional ζ : B ( 0 ; τ ) H 0 2 ( Ω ) R + such that ζ ( 0 ) = 1 , ζ ( v ) ( u v ) O μ i for any v B ( 0 ; τ ) , and

ζ ( 0 ) , φ = 2 Ω ( Δ u , Δ φ ) d x p μ Ω Q ( x ) u p 1 φ d x 2 * * Ω V ( x ) u 2 * * 1 φ d x ( 2 p ) u 2 ( 2 * * p ) Ω V ( x ) u 2 * * d x ,

for every φ C 0 ( Ω ) .

Proof

For each u O μ i , define a function F u : R × H 0 2 ( Ω ) R , given by

F u ( ζ , ϖ ) = I μ ( ζ ( u ϖ ) ) , ζ ( u ϖ ) = ζ 2 u ϖ 2 μ ζ p Ω Q ( x ) ( u ϖ ) p d x ζ 2 * * Ω V ( x ) ( u ϖ ) 2 * * d x .

Then, F u ( 1 , 0 ) = I μ ( u ) , u = 0 , and

d d t F u ( 1 , 0 ) = 2 Ω Δ u 2 d x p μ Ω Q ( x ) u p d x 2 * * Ω V ( x ) u 2 * * d x = ( 2 p ) Ω Δ u 2 d x ( 2 * * p ) Ω V ( x ) u 2 * * d x < 0 .

According to the implicit function theorem, there exist τ > 0 , and a differentiable function ζ : B ( 0 ; τ ) H 0 2 ( Ω ) R + such that ζ ( 0 ) = 1

ζ ( 0 ) , φ = 2 Ω ( Δ u , Δ φ ) d x p μ Ω Q ( x ) u p 1 φ d x 2 * * Ω V ( x ) u 2 * * 1 φ d x ( 2 p ) u 2 ( 2 * * p ) Ω V ( x ) u 2 * * d x ,

for all v B ( 0 ; τ ) , and

F u ( ζ ( v ) , v ) = 0 , for all v B ( 0 ; τ ) ,

for all v B ( 0 ; τ ) , which is equivalent to

I μ ( ζ ( v ) ( u v ) ) , ζ ( v ) ( u v ) = 0 .

That is, ζ ( v ) ( u v ) O μ i .□

Lemma 2.5

For each 1 i k , 0 < μ < Γ * = min { Γ , Γ 0 } , there is a ( P S ) β μ i sequence { u n } O μ i for I μ .

Proof

First, we prove the following conclusion, suppose that ( Q ) and ( V ) hold, then

(2.8) sup t 0 I μ ( t v ε i ) < 2 N S N 4 ,

where 1 i k .

According to [19], we have the following results:

(2.9) v ε i 2 * * 2 = U 2 * * 2 + O ( ε N ) ,

(2.10) v ε i 2 = U 2 + O ( ε N 4 ) .

Hence,

I μ ( t v ε i ) = t 2 2 v ε i 2 μ t p p Ω Q ( x ) v ε i p d x t 2 * * 2 * * Ω V ( x ) v ε i 2 * * d x ,

then, I μ ( t v ε i ) 0 as t 0 , and I μ ( t v ε i ) as t + . Moreover

d I μ ( t v ε i ) d t = t v ε i 2 μ t p 2 Ω Q ( x ) v ε i p d x t 2 * * 2 Ω V ( x ) v ε i 2 * * d x ,

then there exists a unique t ε > 0 such that I μ ( t v ε i ) achieves its maximum. Therefore, there exist two constants T 0 ¯ > 0 and T 0 ̲ > 0 , with T 0 ̲ < t ε < T 0 ¯ . Actually, from lim t 0 + I μ ( t v ε i ) = 0 for all ε , we choose ξ = I μ ( t ε v ε i ) 4 > 0 , then, there exists T 0 ̲ > 0 such that

I μ ( T 0 ̲ v ε i ) = I μ ( T 0 ̲ v ε i ) I μ ( 0 ) < ξ = I μ ( t ε v ε i ) 4 .

Due to the monotonicity of I μ ( t v ε i ) near t = 0 , we have t ε > T 0 ̲ . Similarly, obtain t ε < T 0 ¯ . We set

(2.11) I 0 ( t v ε i ) = t 2 2 v ε i 2 t 2 * * 2 * * Ω Q ( x ) ( v ε i ) 2 * * d x .

Then, we have

d I 0 ( t v ε i ) d t = t v ε i 2 t 2 * * 2 Ω V ( x ) v ε i 2 * * d x .

Let d I 0 ( t v ε i ) d t = 0 , there holds

t max = v ε i 2 Ω V ( x ) ( v ε i ) 2 * * d x 1 2 * * 2 ,

such that d I 0 ( t v ε i ) d t > 0 for each 0 < t < t max , and d I 0 ( t v ε i ) d t < 0 for all t > t max , so I 0 ( t v ε i ) attains its maximum at t max . By V is nonnegative continuous on Ω ¯ and ( V ) , letting ε 0 + , we see that

(2.12) Ω V ( x ) ( v ε i ) 2 * * d x 2 2 * * = v ε i 2 * * 2 + o ( ε N 4 2 ) .

For every ε > 0 , x b i δ ˜ , one has

(2.13) Ω V ( x ) ( v ε i ) 2 * * d x Ω V ( b i ) ( v ε i ) 2 * * d x Ω V ( x ) V ( b i ) ( v ε i ) 2 * * d x { x Ω : x b i δ ˜ } V ( x ) V ( b i ) ( v ε i ) 2 * * d x .

For each ε > 0 , by ( V ) , there exists δ > 0 such that

V ( x ) V ( b i ) < η x b i N 4 2 , for all 0 < x b i < δ .

When ε > 0 small enough, for δ > ε 1 2 , it follows from (2.13) and ( V ) that

Ω V ( x ) ( v ε i ) 2 * * d x Ω V ( b i ) ( v ε i ) 2 * * d x { x Ω : x b i δ ˜ } V ( x ) V ( b i ) ( v ε i ) 2 * * d x < { x Ω : x b i δ } η x b i N 4 2 [ N ( N + 2 ) ( N 2 ) ( N 4 ) ε 4 ] N 4 [ ε 2 + x b i 2 ] N d x + { x Ω : δ < x b i δ ˜ } [ N ( N + 2 ) ( N 2 ) ( N 4 ) ε 4 ] N 4 [ ε 2 + x b i 2 ] N d x = c N η 0 δ r 3 N 6 2 ε N ( ε 2 + r 2 ) N d r + c N δ δ ˜ ε N r N 1 ( ε 2 + r 2 ) N d r C η ε N 4 2 + C ε N 2 ,

where c N = ( N 2 ) N 2 [ N ( N + 2 ) ( N 4 ) ] N 4 , and C , C > 0 are constants. As a result, we deduce that

Ω V ( x ) ( v ε i ) 2 * * d x Ω V ( b i ) ( v ε i ) 2 * * d x ε N 4 2 C η + C ε 2 ,

which implies that

limsup ε 0 + Ω V ( x ) ( v ε i ) 2 * * d x Ω V ( b i ) ( v ε i ) 2 * * d x ε N 4 2 C η .

Thus, due to the arbitrariness of η , we obtain (2.12). Combining with (2.9) and (2.12), it holds that

Ω V ( x ) ( v ε i ) 2 * * d x 2 2 * * = U 2 * * 2 + o ( ε N 4 2 ) .

Consequently, from (2.10), it follows that

v ε i 2 Ω V ( x ) ( v ε i ) 2 * * d x 2 2 * * = U 2 + O ( ε N 4 ) U 2 * * 2 + o ( ε N 4 2 ) = S + o ( ε N 4 2 ) ,

thus

I 0 ( t max ) = v ε i 2 Ω V ( x ) ( v ε i ) 2 * * d x 2 2 * * 2 v ε i 2 2 v ε i 2 2 * * = 2 N v ε i 2 Ω V ( x ) ( v ε i ) 2 * * d x 2 2 * * N 4 2 N S N 4 + o ε N 4 2 .

According to the definition of v ε i , we have

(2.14) μ t p p Ω Q ( x ) v ε i p d x = Ω Q ( x ) η [ N ( N + 2 ) ( N 2 ) ( N 4 ) ε 4 ] ( N 4 ) p 8 [ ε 2 + x b i 2 ] ( N 4 ) p 2 d x C 2 B δ ˜ 2 ( 0 ) ε ( N 4 ) p 2 [ ε 2 + x b i 2 ] ( N 4 ) p 2 d x = C 2 ε 2 N ( N 4 ) p 2 0 δ ˜ 2 ε r N 1 ( 1 + r 2 ) ( N 4 ) p 2 d r C 3 ε 2 N ( N 4 ) p 2 .

From the above results, one obtains

sup t 0 I μ ( t v ε i ) = sup t 0 t 2 2 v ε i 2 t 2 * * 2 * * Ω V ( x ) ( v ε i ) 2 * * d x μ t p p Ω Q ( x ) v ε i p d x v ε i 2 Ω V ( x ) ( v ε i ) 2 * * d x 2 2 * * 2 v ε i 2 2 v ε i 2 2 * * μ t p p Ω Q ( x ) v ε i p d x 2 N S N 4 + o ( ε N 4 2 ) C 3 ε 2 N ( N 4 ) p 2 < 2 N S N 4 ,

where ε is small enough, and C 3 (based on μ , Q , p ) is a positive constant. This completes the proof of (2.8).

For all 1 i k , according to Proposition 2.2 and (2.8), we have

β μ i I μ ( t ε i v ε i ) = sup t 0 I μ ( t v ε i ) < 2 N S N 4 for μ ( 0 , Γ 0 ) .

Combining with Proposition 2.3, we now have

(2.15) β μ i < 2 N S N 4 < β μ i ˜ for μ ( 0 , Γ * ) .

Then, β μ i = inf u O μ i O μ i I μ ( u ) for μ ( 0 , Γ 0 ) . Let { u n i } O μ i O μ i be a minimizing sequence for β μ i . By the Ekeland variational principle, there exists a subsequence { u n i } such that I μ ( u n i ) = β μ i + 1 n , and

(2.16) I μ ( u n i ) I μ ( ϖ ) + ϖ u n i n for any ϖ O μ i O μ i .

From (2.15), we may assume that u n i O μ i for sufficiently large n . By Lemma 2.4, there exist a τ n i > 0 , and a differentiable functional ζ n i : B ( 0 ; τ n i ) H 0 2 ( Ω ) R + such that ζ n i ( 0 ) = 1 , ζ n i ( v ) ( u n i v ) O μ i for every v B ( 0 ; τ n i ) . Let v σ = σ v with v = 1 and 0 < σ < τ n i . Then, v σ B ( 0 ; τ n i ) and ϖ σ , n i = ζ n i ( v σ ) ( u n i v σ ) O μ i . From (2.16) and by the mean value theorem, as σ 0 , we now write

ϖ σ , n i u n i n I μ ( u n i ) I μ ( ϖ σ , n i ) = I μ ( t 0 u n i + ( 1 t 0 ) ϖ σ , n i ) , u n i ϖ σ , n i = I μ ( u n i ) , u n i ϖ σ , n i + o ( u n i ϖ σ , n i ) = σ ζ n i ( v σ ) I μ ( u n i ) , v + ( 1 ζ n i ( v σ ) ) I μ ( u n i ) , u n i + o ( u n i ϖ σ , n i ) = σ ζ n i ( σ v ) I μ ( u n i ) , v + o ( u n i ϖ σ , n i ) ,

where t 0 ( 0,1 ) is a constant, and o ( u n i ϖ σ , n i ) u n i ϖ σ , n i 0 as σ 0 . Hence,

I μ ( u n i ) , v ϖ σ , n i u n i ( 1 n + o ( 1 ) ) σ ζ n i ( σ v ) u n i ( ζ n i ( σ v ) ζ n i ( 0 ) ) σ ζ n i ( σ v ) ( 1 n + o ( 1 ) ) σ ζ n i ( σ v ) u n i ζ n i ( σ v ) ζ n i ( 0 ) + σ v ζ n i ( σ v ) σ ζ n i ( σ v ) 1 n + o ( 1 ) C ( 1 + ( ζ n i ) ( 0 ) ) 1 n + o ( 1 ) ,

where o ( 1 ) 0 as σ 0 . By Lemma 2.4, there exists a positive constant M 0 such that ( ζ n i ) ( 0 ) M 0 for any n and i . Then, I ( u n i ) = o ( 1 ) strongly in ( H 0 2 ( Ω ) ) * as n .□

3 Proof of main results

Proof of Theorem 1.1

The proof of Theorem 1.1 is in three main steps.

Step 1. For c ( , 2 N S N 4 ) , the functional I μ satisfies the ( P S ) c condition.

In fact, let { u n } H 0 2 ( Ω ) be a ( P S ) c sequence satisfying I μ ( u n ) c = o ( 1 ) and I μ ( u n ) = o ( 1 ) . Then, { u n } is bounded in H 0 2 ( Ω ) ; for all μ > 0 , and n large enough, one has

c + 1 + o ( u n ) I μ ( u n ) 1 2 * * I μ ( u n ) , u n 2 N u n 2 μ 2 * * p 2 * * p S p 2 f r u n p ,

that is, { u n } is bounded in H 0 2 ( Ω ) . Suppose that there exists a subsequence, still denoted by { u n } , and there exists u * H 0 2 ( Ω ) , as n , we obtain

(3.1) u n u * weakly in H 0 2 ( Ω ) , u n u * strongly in L p ( Ω ) ( 1 p < 2 * * ) , u n ( x ) u * ( x ) a.e. in Ω .

Next, we will show that u n u * strongly in H 0 2 ( Ω ) . We set v n = u n u * . According to the Brézis-Lieb lemma (see [20]), one has

(3.2) v n 2 + u * 2 = u n 2 + o ( 1 ) ,

(3.3) Ω V ( x ) v n 2 * * d x + Ω V ( x ) u * 2 * * d x = Ω V ( x ) u n 2 * * d x + o ( 1 ) .

In addition, by the Vitali theorem (see [21,22]), we claim that

(3.4) lim n Ω Q ( x ) u n p d x = Ω Q ( x ) u * p d x .

Consequently, from (3.4), and we obtain

v n 2 + u * 2 = μ Ω Q ( x ) u * p d x + Ω V ( x ) v n 2 * * d x + Ω V ( x ) u * 2 * * d x + o ( 1 )

and

(3.5) lim n I μ ( u n ) , u * = 0 .

Since I μ ( u n ) = c + o ( 1 ) , I μ ( u n ) = o ( 1 ) , combining with (3.1)–(3.3) and (3.5), we can see

(3.6) I μ ( u * ) + 1 2 v n 2 = 1 2 * * Ω V ( x ) v n 2 * * d x + c + o ( 1 ) ,

v n 2 Ω V ( x ) v n 2 * * d x = o ( 1 ) .

Now, we may assume that

(3.7) v n 2 l and Ω V ( x ) v n 2 * * d x l ,

as n . According to the Sobolev inequality, we have

v n 2 S v n 2 * * 2 .

Thus, l S l 2 2 * * , which implies that either l = 0 or l S N 4 . If l S N 4 , by (3.6) and (3.7), we have

c = 1 2 1 2 * * l + I μ ( u * ) 2 N S N 4 + I μ ( u * ) .

One aspect, by the definition of c , is that we know

I μ ( u * ) c 2 N S N 4 < 0 .

Another aspect, from (3.5) and 1 < p < 2 < 2 * * , is that we see

I μ ( u * ) = 1 2 1 2 * * u n 2 + 1 2 * * μ p Ω Q ( x ) u n p d x 0 ,

which implies a contradiction. So, l = 0 and u n u * strongly in H 0 2 ( Ω ) .

Step 2. We demonstrate that u 0 serves as a local minimizer of I μ on N μ , then I μ ( u 0 ) = 0 in ( H 0 2 ( Ω ) ) * .

In fact, Lemma 2.1 implies that u 0 is a local minimizer of I μ on N μ , by J u ( t ) , there exists a neighborhood U of u 0 in H 0 2 ( Ω ) that satisfies

I μ ( u 0 ) = min u N μ I μ ( u ) = min u U \ { 0 } , J u ( 1 ) = 0 I μ ( u ) ,

where

J u ( 1 ) = I μ ( u ) , u = u 2 μ Ω Q ( x ) u p d x Ω V ( x ) u 2 * * d x .

It follows from Lemma 2.1 and J u ( 1 ) = 0 that

J u ( 1 ) = u 2 ( p 1 ) μ Ω Q ( x ) u p d x ( 2 * * 1 ) Ω V ( x ) u 2 * * d x = ( p 2 ) μ Ω Q ( x ) u p d x ( 2 * * 2 ) Ω V ( x ) u 2 * * d x < 0 .

Furthermore, according to the theory of Lagrange multipliers, there exists a θ R such that I μ ( u 0 ) = θ J u 0 . By u 0 N μ , we obtain

0 = I μ ( u 0 ) , u 0 = θ J u 0 ( 1 ) , u 0 ,

which implies that θ = 0 . Hence, we obtain I μ ( u 0 ) = 0 in ( H 0 2 ( Ω ) ) * .

Step 3. We prove the existence of k nontrivial solutions.

In fact, from the boundedness of { u n i } and { ( ζ n i ) ( 0 ) } , we infer that I μ ( u n i ) 0 as n . Then, { u n i } be a ( P S ) β μ i sequence for I μ at the level β μ i . From Step 1, there exists a subsequence of { u n i } , still denoted by { u n i } , and a function u i H 0 2 ( Ω ) such that u n i u i strongly in H 0 2 ( Ω ) for 1 i k as n . So, by Proposition 2.2, we obtain lim n ( u n i ) = I μ ( u i ) = β μ i > 0 , which implies that u i 0 . Consequently, based on Step 2, we conclude that problem (1.1) has at least k nontrivial solutions u i ( 1 i k ) for each μ ( 0 , Γ * ) .□

Acknowledgements

The authors are grateful for the reviewer’s valuable comments that improved the manuscript.

  1. Funding information: This work was supported by the Education Department Youth Science Fund Project of Guizhou Province (No. QJJ[2022]404), the Science and Technology Project of Bijie (Nos. BKH [2023]26, BKH [2025]13) and the Disciplinary Construction Project of Mathematics of Guizhou University of Engineering Science (2022).

  2. Author contributions: GT: conceptualization; methodology; writing – original draft; JL: writing – review and editing, YA: writing – review and editing. All authors have accepted responsibility for the entire content of this manuscript and consented to its submission to the journal, reviewed all the results and approved the final version of the manuscript.

  3. Conflict of interest: The authors state no conflict of interest.

  4. Data availability statement: Data sharing does not apply to this article as no datasets were generated or analysed during the current study.

References

[1] X. Dou, X. He, and V. D. Radulescu, Multiplicity of positive solutions for the fractional Schrödinger-Poisson system with critical nonlocal term, Bull. Math. Sci. 14 (2024), 23500121, DOI: https://doi.org/10.1142/S1664360723500121. 10.1142/S1664360723500121Suche in Google Scholar

[2] C. L. Liu and X. Y. Zhang, Existence and multiplicity of solutions for a quasilinear system with locally superlinear condition, Adv. Nonlinear Anal. 12 (2023), 20220289, DOI: https://doi.org/10.1515/anona-2022-0289. 10.1515/anona-2022-0289Suche in Google Scholar

[3] J. Giacomoni, L. M. Santos, and C. A. Santos, Multiplicity for a strongly singular quasilinear problem via bifurcation theory, Bull. Math. Sci. 13 (2023), 2250013, DOI: http://doi.org/10.1142/S1664360722500138. 10.1142/S1664360722500138Suche in Google Scholar

[4] L. S. Wang, T. Yang, and X. L. Yang, A global compactness result with applications to a Hardy-Sobolev critical elliptic system involving coupled perturbation terms, Adv. Nonlinear Anal. 12 (2023), 20220276, DOI: https://doi.org/10.1515/anona-2022-0276. 10.1515/anona-2022-0276Suche in Google Scholar

[5] P. McKenna and W. Walter, Traveling waves in a suspension bridge, SIAM J. Appl. Math. 50 (1990), no. 3, 703–715, DOI: https://doi.org/10.1137/0150041. 10.1137/0150041Suche in Google Scholar

[6] I. Abrahams and A. M. J. Davis, Deflection of a partially clamped elastic plate, in: I. D. Abrahams, P. A. Martin, M. J. Simon (eds.), IUTAM Symposium on Diffraction and Scattering in Fluid Mechanics and Elasticity, Fluid Mechanics and Its Applications, vol. 68, Springer, Dordrecht, 2002, pp. 303–312, DOI: https://doi.org/10.1007/978-94-017-0087-0_33. 10.1007/978-94-017-0087-0_33Suche in Google Scholar

[7] X. Y. Cheng, Z. S. Feng, and L. Wei, Existence and multiplicity of nontrivial solutions for a semilinear biharmonic equation with weight functions, Discrete Contin. Dyn. Syst. 14 (2021), no. 9, 3067–3083, DOI: https://doi.org/10.3934/dcdss.2021078. 10.3934/dcdss.2021078Suche in Google Scholar

[8] Y. B. Deng and S. Wei, Non-trivial solutions for a semilinear biharmonic problem with critical growth and potential vanishing at infinity, Proc. Roy. Soc. Edinburgh Sect. A. 145 (2015), 281–299, DOI: https://doi.org/10.1017/S0308210513001170. 10.1017/S0308210513001170Suche in Google Scholar

[9] A. Harrabi, Fourth-order elliptic equations, Adv. Nonlinear Stud. 14 (2014), 593–604, DOI: https://doi.org/10.1515/ans-2014-0304. 10.1515/ans-2014-0304Suche in Google Scholar

[10] S. Hu and L. Wang, Existence of nontrivial solutions for fourth-order asymptotically linear elliptic equations, Nonlinear Anal. 94 (2014), 120–132, DOI: http://doi.org/10.1016/j.na.2013.08.008. 10.1016/j.na.2013.08.008Suche in Google Scholar

[11] J. F. Liao, Y. Pu, and C. L. Tang, Multiplicity of positive solutions for a class of concave-convex elliptic equations with critical growth, Acta Math. Sci. Ser. B (Engl. Ed.) 38 (2018), 497–518, DOI: https://doi.org/10.1016/S0252-9602(18)30763-X. 10.1016/S0252-9602(18)30763-XSuche in Google Scholar

[12] X. Liu and Y. Huang, On sign-changing solution for a fourth-order asymptotically linear elliptic problem, Nonlinear Anal. 72 (2010), 2271–2276, DOI: https://doi.org/10.1016/j.na.2009.11.001. 10.1016/j.na.2009.11.001Suche in Google Scholar

[13] M. Ramos, H. Tavares, and W. Zou, A Bahri-Lions theorem revisited, Adv. Math. 222 (2009), 2173–2195, DOI: https://doi.org/10.1016/j.aim.2009.07.013. 10.1016/j.aim.2009.07.013Suche in Google Scholar

[14] J. Zhang and S. Li, Multiple nontrivial solutions for some fourth-order semilinear elliptic problems, Nonlinear Anal. 60 (2005), 221–230, DOI: https://doi.org/10.1016/j.na.2004.07.047. 10.1016/S0362-546X(04)00313-XSuche in Google Scholar

[15] S. N. Ezzat, A. S. Charles, and J. F. Yang, Critical semilinear biharmonic equations in RN, Proc. Roy. Soc. Edinburgh Sect. A 121 (1992), 139–148, DOI: https://doi.org/10.1017/S0308210500014189. 10.1017/S0308210500014189Suche in Google Scholar

[16] A. Bahri and Y. Y. Li, On a min-max procedure for the existence of a positive solution for certain scalar field equations in RN, Rev. Mat. Iberoam. 6 (1990), 1–15, DOI: https://doi.org/10.4171/RMI/92. 10.4171/rmi/92Suche in Google Scholar

[17] H. Brézis and L. Nirenberg, A minimization problem with critical exponent and nonzero data, in: Symmetry in Nature, Scuola Normale Superiore Pisa, 1989, pp. 129–140. Suche in Google Scholar

[18] P. L. Lions, The concentratio-compactness principle in the calculus of variations, the limit case, Rev. Mat. Iberoam. 1 (1985), 145–201, http://eudml.org/doc/39314. 10.4171/rmi/6Suche in Google Scholar

[19] Y. X. Yao, R. X. Wang, and Y. T. Shen, Nontrivial solution for a class of semilinear biharmonic equation involving critical exponents, Acta Math. Sci. Ser. B (Engl. Ed.) 27 (2007), no. 3, 509–514, DOI: https://doi.org/10.1016/S0252-9602(07)60050-2. 10.1016/S0252-9602(07)60050-2Suche in Google Scholar

[20] H. Brézis and E. Lieb, A relation between pointwise convergence of functions and con-vergence of functionals, Proc. Amer. Math. Soc. 88 (1983), 486–490, DOI: https://doi.org/10.1090/S0002-9939-1983-0699419-3. 10.1090/S0002-9939-1983-0699419-3Suche in Google Scholar

[21] M. Willem, Minimax Theorems, Birkhauser, Basel, 1996, DOI: https://doi.org/10.1007/978-1-4612-4146-1. 10.1007/978-1-4612-4146-1Suche in Google Scholar

[22] W. Rudin, Real and Complex Analysis, McGraw-Hill, Inc., New York, 1966. Suche in Google Scholar

Received: 2024-08-14
Revised: 2025-02-24
Accepted: 2025-03-03
Published Online: 2025-04-25

© 2025 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Artikel in diesem Heft

  1. Special Issue on Contemporary Developments in Graphs Defined on Algebraic Structures
  2. Forbidden subgraphs of TI-power graphs of finite groups
  3. Finite group with some c#-normal and S-quasinormally embedded subgroups
  4. Classifying cubic symmetric graphs of order 88p and 88p 2
  5. Simplicial complexes defined on groups
  6. Two-sided zero-divisor graphs of orientation-preserving and order-decreasing transformation semigroups
  7. Further results on permanents of Laplacian matrices of trees
  8. Special Issue on Convex Analysis and Applications - Part II
  9. A generalized fixed-point theorem for set-valued mappings in b-metric spaces
  10. Research Articles
  11. Dynamics of particulate emissions in the presence of autonomous vehicles
  12. The regularity of solutions to the Lp Gauss image problem
  13. Exploring homotopy with hyperspherical tracking to find complex roots with application to electrical circuits
  14. The ill-posedness of the (non-)periodic traveling wave solution for the deformed continuous Heisenberg spin equation
  15. Some results on value distribution concerning Hayman's alternative
  16. 𝕮-inverse of graphs and mixed graphs
  17. A note on the global existence and boundedness of an N-dimensional parabolic-elliptic predator-prey system with indirect pursuit-evasion interaction
  18. On a question of permutation groups acting on the power set
  19. Chebyshev polynomials of the first kind and the univariate Lommel function: Integral representations
  20. Blow-up of solutions for Euler-Bernoulli equation with nonlinear time delay
  21. Spectrum boundary domination of semiregularities in Banach algebras
  22. Statistical inference and data analysis of the record-based transmuted Burr X model
  23. A modified predictor–corrector scheme with graded mesh for numerical solutions of nonlinear Ψ-caputo fractional-order systems
  24. Dynamical properties of two-diffusion SIR epidemic model with Markovian switching
  25. Classes of modules closed under projective covers
  26. On the dimension of the algebraic sum of subspaces
  27. Periodic or homoclinic orbit bifurcated from a heteroclinic loop for high-dimensional systems
  28. On tangent bundles of Walker four-manifolds
  29. Regularity of weak solutions to the 3D stationary tropical climate model
  30. A new result for entire functions and their shifts with two shared values
  31. Freely quasiconformal and locally weakly quasisymmetric mappings in metric spaces
  32. On the spectral radius and energy of the degree distance matrix of a connected graph
  33. Solving the quartic by conics
  34. A topology related to implication and upsets on a bounded BCK-algebra
  35. On a subclass of multivalent functions defined by generalized multiplier transformation
  36. Local minimizers for the NLS equation with localized nonlinearity on noncompact metric graphs
  37. Approximate multi-Cauchy mappings on certain groupoids
  38. Multiple solutions for a class of fourth-order elliptic equations with critical growth
  39. A note on weighted measure-theoretic pressure
  40. Majorization-type inequalities for (m, M, ψ)-convex functions with applications
  41. Recurrence for probabilistic extension of Dowling polynomials
  42. Unraveling chaos: A topological analysis of simplicial homology groups and their foldings
  43. Global existence and blow-up of solutions to pseudo-parabolic equation for Baouendi-Grushin operator
  44. A characterization of the translational hull of a weakly type B semigroup with E-properties
  45. Some new bounds on resolvent energy of a graph
  46. Carmichael numbers composed of Piatetski-Shapiro primes in Beatty sequences
  47. The number of rational points of some classes of algebraic varieties over finite fields
  48. Singular direction of meromorphic functions with finite logarithmic order
  49. Pullback attractors for a class of second-order delay evolution equations with dispersive and dissipative terms on unbounded domain
  50. Eigenfunctions on an infinite Schrödinger network
  51. Boundedness of fractional sublinear operators on weighted grand Herz-Morrey spaces with variable exponents
  52. On SI2-convergence in T0-spaces
  53. Bubbles clustered inside for almost-critical problems
  54. Classification and irreducibility of a class of integer polynomials
  55. Existence and multiplicity of positive solutions for multiparameter periodic systems
  56. Averaging method in optimal control problems for integro-differential equations
  57. On superstability of derivations in Banach algebras
  58. Investigating the modified UO-iteration process in Banach spaces by a digraph
  59. The evaluation of a definite integral by the method of brackets illustrating its flexibility
  60. Existence of positive periodic solutions for evolution equations with delay in ordered Banach spaces
  61. Tilings, sub-tilings, and spectral sets on p-adic space
  62. The higher mapping cone axiom
  63. Continuity and essential norm of operators defined by infinite tridiagonal matrices in weighted Orlicz and l spaces
  64. A family of commuting contraction semigroups on l 1 ( N ) and l ( N )
  65. Pullback attractor of the 2D non-autonomous magneto-micropolar fluid equations
  66. Maximal function and generalized fractional integral operators on the weighted Orlicz-Lorentz-Morrey spaces
  67. On a nonlinear boundary value problems with impulse action
  68. Normalized ground-states for the Sobolev critical Kirchhoff equation with at least mass critical growth
  69. Decompositions of the extended Selberg class functions
  70. Subharmonic functions and associated measures in ℝn
  71. Some new Fejér type inequalities for (h, g; α - m)-convex functions
  72. The robust isolated calmness of spectral norm regularized convex matrix optimization problems
  73. Multiple positive solutions to a p-Kirchhoff equation with logarithmic terms and concave terms
  74. Joint approximation of analytic functions by the shifts of Hurwitz zeta-functions in short intervals
  75. Green's graphs of a semigroup
  76. Some new Hermite-Hadamard type inequalities for product of strongly h-convex functions on ellipsoids and balls
  77. Infinitely many solutions for a class of Kirchhoff-type equations
  78. On an uncertainty principle for small index subgroups of finite fields
Heruntergeladen am 5.9.2025 von https://www.degruyterbrill.com/document/doi/10.1515/math-2025-0141/html
Button zum nach oben scrollen