Home Mathematics Existence and multiplicity of nontrivial solutions for Schrödinger-Bopp-Podolsky systems with critical nonlinearity in ℝ3
Article Open Access

Existence and multiplicity of nontrivial solutions for Schrödinger-Bopp-Podolsky systems with critical nonlinearity in ℝ3

  • , and EMAIL logo
Published/Copyright: October 3, 2025
Become an author with De Gruyter Brill

Abstract

This article investigates the existence and multiplicity of nontrivial solutions for Schrödinger-Bopp-Podolsky systems with critical nonlinearity in R 3 . Under appropriate assumptions about the potential and nonlinear terms, the existence and multiplicity of solutions are obtained by using the concentration-compactness principle and the symmetric mountain pass theorem. To some extent, we generalize the previous results.

MSC 2010: 35J20; 35R03; 46E35

1 Introduction and main result

In this article, we intend to study the following Schrödinger-Bopp-Podolsky systems with critical nonlinearity in R 3 :

(1.1) ε 2 Δ u + A ( x ) u + Φ u = g ( u ) + u 2 * 2 u , x R 3 , Δ Φ + Δ 2 Φ = u 2 , x R 3 ,

where ε > 0 is a parameter, Φ : R 3 R and A : R 3 R 3 is a given external potential, and g : R R is a nonlinearity satisfying the appropriate assumptions given below:

  1. 0 = A ( 0 ) = min x R 3 A ( x ) A ( x ) < M ;

  2. A C ( R 3 , R ) and there exists τ > 0 such that the set A τ { x R 3 : A ( x ) < τ } has a finite Lebesgue measure;

  3. g ( x ) = 0 for s 0 and g ( s ) = o ( s ) as s 0 ;

  4. lim s 0 g ( s ) s = 0 and there exist some constants C 0 > 0 and q ( 2 , + ) such that

    g ( s ) C 0 ( 1 + s q 1 ) , s R ;

  5. there is 4 < θ < 2 * such that 0 < θ G ( s ) s g ( s ) for all s > 0 , where

    G ( s ) = 0 s g ( t ) d t .

In recent years, d’Avenia and Siciliano [1] have attracted their attention on a new kind of elliptic system, called the Schrödinger-Bopp-Podolsky system, which, as far as we know, was never been considered before in the mathematical literature, although it was known among the physicists. The Schrödinger-Bopp-Podolsky system has the following form:

(1.2) Δ v + ω v + q 2 ϕ v = v v p 2 , β 2 Δ 2 ϕ Δ ϕ = 4 π v 2 ,

where β , ω > 0 . As for the physical meaning of this system, if v , ϕ : R 3 R solve system (1.2), then v describes the spatial profile of a standing wave ψ ( t x ) = e i ω t v ( x ) . We refer to articles [2,3] for more details. The Bopp-Podolsky theory is a second-order gauge theory for the electromagnetic field. As the Mie theory [4] and its generalizations given by Born [5,6] and Born and Infeld [7,8], it was introduced to solve the so-called infinity problem that appears in the classical Maxwell theory [9,10]. In addition, the Bopp-Podolsky theory can be explained as an effective theory for short distances [11]. For long distances, it cannot be distinguished experimentally from Maxwell’s theory. Therefore, the Bopp-Podolsky parameter a > 0 , which has a dimension of the inverse of mass, can be interpreted as a cut-off distance or can be linked to an effective radius for the electron. For more physical features, one can refer to recent papers [1217] and references therein.

In recent years, many interesting results for problem (1.1) have been obtained by using different methods. For example, using variational methods, d’Avenia and Siciliano [1] proved that equation (1.2) has a nontrivial solution at p ( 3,6 ) and q > 0 or p ( 2,3 ] and q > 0 small enough and obtained that, in the radial case, this solution converges to solution of the classical Schrödinger-Poisson system when β 0 . Siciliano and Silva [18] obtained the existence and nonexistence of solutions for a nonlinear Schrödinger equation coupled with the electromagnetic field by using Pohožaev’s fibering method. Mascaro and Siciliano [19], proved the number of positive solutions by the Ljusternick-Schnirelmann category. Figueiredo and Siciliano [20] studied the multiple solutions of the prior given “interaction energy” by using the Ljusternick-Schnirelmann category and Morse theory.

For the critical case, Chen and Tang [21] studied the following Schrödinger-Bopp-Podolsky system with general nonlinearity of the form:

(1.3) Δ u + V ( x ) u + ϕ u = μ f ( u ) + u 5 in R 3 , 2 Δ ϕ + a 2 Δ 2 ϕ = 4 π u 2 in R 3 ,

where a > 0 , V C ( R 3 , [ 0 , ) ) with V lim y V ( y ) sup x R 3 V ( x ) > 0 , and f C ( R , R ) satisfying 0 t f ( s ) d s t p with p ( 2,6 ) for all t 0 . The authors used some new analytical techniques and inequalities to prove that system (1.3) admits ground-state solutions for all μ > 0 when p ( 4,6 ) , and for all μ > μ 0 when p ( 2,4 ] , where μ 0 is a positive constant determined by a , V , and p . Li et al. [22] proved the existence of a nontrivial ground state solution for a class of critical nonlinear Schrödinger-Bopp-Podolsky system by using the method of the Pohožaev-Nehari manifold, the arguments of Bréis-Nirenberg, the monotonicity trick, and a global compactness lemma. Very recently, Damian and Siciliano [23] considered the following critical Schrödinger-Bopp-Podolsky system:

(1.4) ε 2 Δ u + V ( x ) u + Q ( x ) ϕ u = h ( x , u ) + K ( x ) u 4 u in R 3 , Δ ϕ + a 2 Δ 2 ϕ = 4 π Q ( x ) u 2 in R 3 .

Given the right conditions for the functions V and K , the authors showed the existence of small solutions in the semiclassical limit for any fixed a > 0 . Moreover, when a 0 , they also proved that with ε fixed and suitably small, the solutions strongly converge to solutions of the Schrödinger-Poisson system.

Inspired by the above literature, this article will focus on a class of Schrödinger-Bopp-Podolsky systems with critical nonlinearity. More specifically, our article was primarily inspired by Damian and Siciliano [23], Ding and Lin [24], and Yang and Ding [25]. We will prove the compactness condition by the concentration-compactness principle. Moreover, some existence results of solutions for problem (1.1) are obtained with the help of the variational method. Now, we present the main conclusions of this article as follows:

Theorem 1.1

Let ( A 1 ) , ( A 2 ) , and ( g 1 ) ( g 3 ) be satisfied. Then, for any δ > 0 , there is λ * > 0 such that problem (1.1) has at least one nontrivial solution u λ that satisfies the following properties:

  1. 1 2 1 θ R 3 ( u λ 2 + A ( x ) u λ 2 ) d x δ λ 2 2 2 * ;

  2. λ 4 λ 2 * R 3 u λ 2 * d x + λ θ 4 1 R 3 G ( u λ ) d x δ λ 2 2 2 * .

Theorem 1.2

Let ( A 1 ) , ( A 2 ) , and ( g 1 ) ( g 3 ) be satisfied and g ( t ) is odd in t. Then, for any m * N and σ > 0 , there is Λ m * , σ > 0 such that if λ Λ m * , σ , problem (1.1) has at least m * pairs of solutions u ± λ , m * , which satisfy the estimates ( i ) and ( i i ) in Theorem 1.1.

Remark 1.1

We should also point out that compared to previous papers, this article has several important characteristics. First, let us emphasize that the work presented in this article is completely different from previous papers, such as [2125], they used decomposing the corresponding functional and truncating techniques to prove the compactness condition. However, in this article, we attempt to prove the compactness condition by using the concentration-compactness principle, which is entirely distinct from the prior methods. Second, the main difficulty of this article is caused by the nonlinear term, which has critical growth and can lead to the loss of compactness. Another difficulty we encounter is the lack of compactness due to unbounded domains and Poisson terms. In order to prove the symmetric mountain path theorem, we must establish some tools and technological achievements. In a sense, we have generalized and improved the previous results.

This article is organized as follows: In Section 2, we will review some basic definitions and key prerequisites to our main proof. In Section 3, we will prove that the energy functional I ε satisfies the mountain pass structure. In addition, we prove ( PS ) c condition by applying the concentration-compactness principle. In Section 4, we will prove the main conclusions of this article.

Notations 1.1

Now, let us explain some symbols of the article, while others will be provided when we use them:

  • H 1 ( R 3 ) is the usual Sobolev space with norm ;

  • u p is the usual L p -norm ( R 3 u p d x ) 1 p ;

  • for any number r > 0 , B r ( 0 ) denotes a sphere of radius r centered on 0 with respect to the norm topology in D 1 , 2 ( R 3 ) ;

  • o n ( 1 ) represents a vanishing sequence;

  • the arrows , denote weak convergence and strong convergence, respectively;

  • C , C * , C i , i = 1 , 2 , , denote generic constants, which may change from line to line.

2 Preliminaries and variational setting

First, looking back at our problem, by setting λ = 1 ε 2 , we obtain the following equivalent system:

(2.1) Δ u + λ A ( x ) u + λ Φ u = λ g ( u ) + λ u 2 * 2 u , x R 3 , Δ Φ + Δ 2 Φ = u 2 , x R 3 .

In a sense, once the solution ( u , Φ ) of problem (2.1) is found, the solution to problem (1.1) can be obtained by substituting appropriate variables.

Now, we review the definition of Sobolev space. Let

D 1 , 2 ( R 3 ) = { u L 2 * ( R 3 ) : R 3 u 2 d x < }

which is equipped with the norm

u D 1 , 2 ( R 3 ) R 3 u 2 d x 1 2 .

The best embedding constant from D 1 , 2 ( R 3 ) into L 2 * ( R 3 ) is defined as

S = inf u D 1 , 2 ( R 3 ) \ { 0 } , u 2 * = 1 R 3 u 2 d x .

The natural functional space of problem (2.1) is as follows:

W λ { u H 1 ( R 3 ) : R 3 A ( x ) u 2 d x < + }

and

D { Φ D 1 , 2 ( R 3 ) : Δ Φ L 2 ( R 3 ) } = C 0 ( R 3 ) ¯ 2 + 2 .

The space W λ is a Hilbert space with norm

u λ R 3 u 2 + λ R 3 A ( x ) u 2 1 2

and is continuously embedded into H 1 ( R 3 ) . The space D has been introduced and deeply studied by Alves et al. [26], where it is proved that D L p ( R 3 ) for p [ 6 , + ) . Note that the norm W 1 , 2 ( R 3 ) is equivalent to W λ . It is obvious that the embedding W λ W 1 , 2 ( R 3 ) L γ ( R 3 ) is continuous for any γ [ 2 , 2 * ] due to [27, Lemma 1]. Furthermore, there exists a constant c γ > 0 such that

(2.2) u L γ ( R 3 ) c γ u λ for all u W λ .

In fact, problem (2.1) can be simplified. In fact, similar to the discussion in the study of D’Avenia and Siciliano [1], we can reduce the problem to finding solutions of the following non-local equation:

(2.3) Δ u + λ A ( x ) u + λ Φ u u = λ g ( u ) + λ u 2 * 2 u in R 3 ,

where

(2.4) Φ u ( x ) = R 3 1 e ( x y ) x y u 2 ( y ) d y .

Below, we can obtain that the functional Φ u has the following properties.

Lemma 2.1

(see [1, Lemma 3.4]) For every u H 1 ( R 3 ) , we have the following properties:

  1. for every y R 3 , Φ u ( + y ) = Φ u ( + y ) ;

  2. Φ u 0 ;

  3. for every s ( 3 , + ] , Φ u L s ( R 3 ) C 0 ( R 3 ) ;

  4. for every s ( 3 2 , + ] , Φ u L s ( R 3 ) C 0 ( R 3 ) ;

  5. Φ u 6 C u 2 for some constant C > 0 .

  6. Moreover, if u is radial also Φ u is, and if u n u in H rad 1 ( R 3 ) , then

  7. Φ u n Φ u in D ;

  8. R 3 Φ u n u n 2 d x R 3 Φ u u 2 d x ;

  9. R 3 Φ u n u n v d x R 3 Φ u u v d x for any v H 1 ( R 3 ) .

Now, we will always refer to problem (2.3) in terms of the unknown u , because Φ u is determined by u of the above formula. We note that the energy functional associated with problem (2.3) is given as follows:

(2.5) I λ ( u ) = 1 2 R 3 u 2 d x + 1 2 R 3 λ A ( x ) u 2 d x + λ 4 R 3 Φ u u 2 d x λ 2 * R 3 u 2 * d x λ R 3 G ( u ) d x .

Moreover, by a weak solution u of problem (2.3), we mean for any v W λ such that

(2.6) R 3 u v d x + R 3 λ A ( x ) u v d x + λ R 3 Φ u u v d x = λ R 3 u 2 * 2 u v d x λ R 3 g ( u ) v d x .

3 Proof of ( PS ) c condition

In this section, we will prove that I λ has the mountain pass structure and satisfies the ( PS ) c condition. To this end, we first prove the following lemma.

Lemma 3.1

Assume ( A 1 ) , ( A 2 ) , and ( g 1 ) ( g 3 ) hold. For any finite-dimensional subspace F E , there is e F such that the functional defined in (2.5) satisfies the following properties:

  1. For each λ > 0 there is α λ > 0 and ρ λ > 0 such that I λ ( u ) > 0 for u B ρ λ \ { 0 } . Moreover, I λ ( u ) > α λ for all u W λ with u = ρ λ , where B ρ λ = { u W λ : u < ρ λ } .

  2. There is e W λ with e λ > ρ λ such that I λ ( e ) < 0 for all λ > 0 .

Proof

(i) First, by conditions ( g 2 ) and ( g 3 ) , we obtain that for any κ > 0 there is C κ > 0 such that

(3.1) G ( s ) κ s 2 + C κ s q for s R .

So, for every u W λ , let κ ( 0 , 1 4 λ c 2 * 2 * ) , we have that

I λ ( u ) = 1 2 R 3 u 2 d x + λ R 3 A ( x ) u 2 d x + λ 4 R 3 Φ u u 2 d x λ 2 * R 3 u 2 * d x λ R 3 G ( u ) 1 2 u λ 2 λ 2 * u 2 * 2 * λ κ u 2 * 2 λ C κ u 2 * q 1 2 u λ 2 λ 2 * C 2 * 2 * u λ 2 * λ κ C 2 2 * u λ 2 λ C κ C 2 * q u λ q 1 4 λ C 2 * 2 * 2 * u λ 2 * 2 λ C κ C 2 * q u λ q 2 u λ 2 .

Let

f ( t ) 1 4 λ C 2 * 2 * 2 * t 2 * 2 λ C κ C 2 * q t q 2 for all t > 0 .

Clearly, lim t 0 + f ( t ) = 1 4 > 0 , because 2 * > 2 and q > 2 . So, we can choose ρ λ u small enough such that

λ c 2 * 2 * 2 * ρ λ 2 * 2 + λ C κ C 2 * q ρ λ q 2 < 1 4 .

So, we conclude

I λ ( u ) f ( ρ λ ) ρ λ 2 α λ .

This completes the proof of Lemma 3.1 (i).

(ii) We note that conditions ( g 2 ) and ( g 3 ) mean that for every ϱ > 0 , there is C ϱ > 0 such that

(3.2) G ( s ) ϱ s p C ϱ s 2 , s R .

Let u 0 W λ with u 0 = 1 , by Lemma 2.1- ( Φ 5 ) , we have

I λ ( t u 0 ) t 2 2 R 3 u 0 2 d x + λ R 3 A ( x ) u 0 2 d x + λ 4 t 2 R 3 Φ u 0 u 0 2 d x λ t 2 * 2 * R 3 u 0 2 * d x λ R 3 G ( t u 0 ) d x t 2 2 u 0 λ 2 + λ 4 t 2 C u 0 2 * 4 λ t * 2 * u 0 2 * 2 * λ ϱ t p u 0 2 * p + λ C ϱ t 2 u 0 2 * 2 t 2 2 u 0 λ 2 + λ 4 t 2 C C 2 * 4 u 0 λ 4 λ t 2 * 2 * C 2 * 2 * u 0 λ 2 * λ ϱ t p C 2 * p u 0 λ p + λ C ϱ C 2 * 2 t 2 u 0 λ 2 .

For all u W λ due to 2 * > 2 and p > 4 , we can choose t 1 large enough such that t u 0 > ρ λ and I λ ( t u 0 ) < 0 . It is easy to obtain this conclusion by letting e = t u 0 and this means that the proof of Lemma 3.1 (ii) is completed.□

Next, we will use the second concentration-compactness principle and the concentration-compactness principle at infinity to prove that the ( PS ) c condition holds. Now, we first recall the that the ( PS ) c condition holds. Now, we first recall the definition of the Palais-Smale sequence.

Definition 3.1

Let J : E R be a C 1 functional on a Banach space E .

(1) For c R , a sequence { u n } E is called a Palais-Smale sequence at level c (in short ( PS ) c ) in E for J if J ( u n ) = c + o n ( 1 ) and J ( u n ) 0 in E * (dual of E ) as n .

(2) We say J satisfies ( PS ) c condition if for any Palais-Smale sequence { u n } in E , J has a convergent subsequence.

Now, let us prove that I λ satisfies the ( PS ) c condition.

Lemma 3.2

Suppose that ( A 1 ) , ( A 2 ) , and ( g 1 ) ( g 3 ) hold. Let { u n } W λ be any ( PS ) c sequence. The functional I λ satisfies ( PS ) c condition for all c ( 0 , α 0 λ 2 2 2 * ) , where α 0 = ( 1 2 1 θ ) S 2 * 2 * 2 .

Proof

This proof is divided into four steps.

Step I. We claim that for all c 0 , { u n } is bounded in W λ .

In fact, let { u n } W λ be a ( PS ) c sequence related to the functional I λ . By ( g 3 ) , one has

c + o n ( 1 ) ( 1 + u n λ ) = I λ ( u n ) 1 θ I λ ( u n ) , u n 1 2 1 θ R 3 u n 2 d x + λ R 3 A ( x ) u n 2 d x + λ 4 λ θ R 3 Φ u n u n 2 d x λ θ λ 2 * R 3 u n 2 * d x λ θ R 3 ( g ( u n ) u n θ G ( u n ) ) d x 1 2 1 θ u n λ 2 .

Together with 1 2 1 θ > 0 , we obtain that { u n } is bounded on W λ . This means that the proof of Step I is complete.

Step II. We claim w j = 0 for all j J .

In fact, from Step I, we know that { u n } is bounded in W λ . Hence, we can conclude that

u n u in H 1 ( R 3 )

and

u n u a.e. in R 3 .

Thus, we assume that

u n 2 ω and u n 2 * ξ

in the sense of measure. By the concentration compactness principle from Lions [28], there is at most countable sets of J , families of positive numbers { ω j : j J } , { ξ j : j J } , and sequences of point { z j } j J R 3 such that

(3.3) ω u 2 + j J ω j δ z j ,

(3.4) ξ = u 2 * + j J ν j δ z j

and

(3.5) S ξ j 2 2 * ω j ,

where δ z is Dirac mass of mass 1 concentrated at x R 3 . In addition, we can structure a smooth truncation function ϕ ε , j centered at z j so that

0 ϕ ε , j ( x ) 1 , ϕ ε , j ( x ) = 1 in B z j , ε 2

and

ϕ ε , j ( x ) = 0 in R 3 \ B ( z j , ε ) , ϕ ε , j 4 ε

for any ε > 0 small. Note that I λ ( u n ) , u n ϕ ε , j = o n ( 1 ) as n . So, we obtain

(3.6) R 3 u n 2 ϕ ε , j d x + λ R 3 A ( x ) u n 2 ϕ ε , j d x + λ R 3 Φ u n u n 2 ϕ ε , j d x = λ R 3 u n 2 * ϕ ε , j d x + λ R 3 g ( u n ) u n ϕ ε , j d x + o n ( 1 ) .

With the help of the boundedness of { u n } in W λ , we have

(3.7) lim ε 0 lim n λ R 3 g ( u n ) u n ϕ ε , j d x = 0 .

On the other hand, by (3.3), (3.4), and the Hölder inequality we find that

(3.8) lim ε 0 lim n R 3 u n 2 ϕ ε , j d x + λ R 3 A ( x ) u n 2 ϕ ε , j d x + λ R 3 Φ u n u n 2 ϕ ε , j d x lim ε 0 lim n R 3 ϕ ε , j d ω ω j

and

(3.9) lim ε 0 lim n λ R 3 u n 2 * ϕ ε , j d x = lim ε 0 λ R 3 u 2 * ϕ ε , j d x + ξ j = λ ξ j .

Now, according to (3.6), (3.7), (3.8), and (3.9), we obtain λ ξ j ω j . Combining (3.5), we have

ω j S 2 * 2 * 2 λ 2 2 2 * or ω j = 0 .

We claim that the first case is not valid. If not, then there is j 0 J such that ω j 0 S 2 * 2 * 2 λ 2 2 2 * , we have

c = lim n I λ ( u n ) 1 θ I ( u n ) , u n

= lim n 1 2 1 θ R 3 u n 2 d x + 1 2 1 θ λ R 3 A ( x ) u n 2 d x + λ 4 λ θ R 3 Φ u n u n 2 d x + λ θ λ 2 * R 3 u n 2 * d x + λ θ R 3 g ( u n ) u n θ G ( u n ) d x lim n 1 2 1 θ R 3 u n 2 d x 1 2 1 θ S 2 * 2 * 2 λ 2 2 2 * .

Due to θ > 2 , this gives a contradiction with c ( 0 , α 0 ) , and we obtain that

ω j = 0 for all j J .

Step III. We claim that ω = 0 .

In fact, in order to prove this claim, we can define a truncation function ϕ R C ( R 3 ) so that ϕ R ( x ) = 1 on x > R + 1 , ϕ R ( x ) = 0 on x < R and ϕ R 2 R . Let

ω lim R limsup n x > R u n 2 d x , ξ lim R limsup n x > R u n 2 * d x

and

(3.10) S ξ 2 2 * ω .

On the one hand, by applying the fact I λ ( u n ) , u n ϕ R = o n ( 1 ) , we have

(3.11) R 3 u n 2 ϕ R d x + λ R 3 A ( x ) u n 2 ϕ R d x + λ R 3 Φ u n u n 2 ϕ R d x = λ R 3 u n 2 * 2 u n ϕ R d x + λ R 3 g ( u n ) u n ϕ R d x + o n ( 1 ) .

On the other hand, similar to Step II, we can obtain

(3.12) lim R lim n λ R 3 g ( u n ) u n ϕ R d x = 0 ,

(3.13) lim R lim n λ R 3 u n 2 * ϕ R d x = λ ξ

and

(3.14) lim R lim n R 3 u n 2 ϕ R d x + λ R 3 A ( x ) u n 2 ϕ R d x + λ R 3 Φ u n u n 2 ϕ R d x lim R lim n R 3 u n 2 ϕ R d x ω .

According to (3.11), (3.12), (3.13), and (3.14), we obtain λ ξ ω . Together with (3.10), we have

ω S 2 * 2 * 2 λ 2 2 2 * or ω = 0 .

If ω S 2 * 2 * 2 holds. Similarly, we obtain

c = lim R lim n I λ ( u n ) 1 θ I λ ( u n ) , u n lim R lim n 1 2 1 θ R 3 u n 2 d x + 1 2 1 θ λ R 3 A ( x ) u n 2 d x + λ 4 λ θ R 3 Φ u n u n 2 d x + λ θ λ 2 * R 3 u n 2 * d x + λ θ R 3 ( g ( u n ) u n θ G ( u n ) ) d x lim R lim n 1 2 1 θ R 3 u n 2 d x 1 2 1 θ S 2 * 2 2 λ 2 2 2 * .

From the definition of c , we can obtain

ω = 0 .

Step IV. We claim that u n u strongly in W λ . In fact, by Steps II and III, we have

(3.15) R 3 u n u 2 * d x 0 as n ,

(3.16) R 3 Φ ( u n u ) u n u 2 d x 0 as n

and

(3.17) R 3 g ( u n u ) u n u d x 0 as n .

By (3.3), we have

(3.18) I λ ( u n u ) , u n u = R 3 u n u 2 d x + λ R 3 A ( x ) u n u 2 d x + λ R 3 Φ ( u n u ) u n u 2 d x + λ R 3 u n u 2 * d x λ R 3 g ( u n u ) ( u n u ) d x .

Now, from (3.8), (3.9), and (3.15)–(3.18), we have

R 3 u n u 2 d x + λ R 3 A ( x ) ( u n u ) 2 d x 0 as n .

The Brézis-Lieb lemma [29] means that u n u in W λ . This completes the proof of Lemma 3.2.□

4 The proofs of our main results

Now, we can prove our main results. We note that the functional I ε satisfying the ( PS ) c condition does not apply to every c > 0 . Therefore, we should construct a sufficiently small minimax level below to find a special finite-dimensional subspace. By conditions ( A 1 ) , ( g 2 ) , and ( g 3 ) , we have

(4.1) I λ ( u ) 1 2 R 3 u 2 d x + λ R 3 A ( x ) u 2 d x + λ 4 R 3 Φ u u 2 d x λ 2 * R 3 u 2 * d x λ ϱ R 3 u p d x + λ C ϱ R 3 u 2 d x 1 2 u ε 2 + λ 4 C u 2 * 4 λ 2 * u 2 * 2 * λ ϱ u 2 * p + λ C ϱ u 2 * 2

for all u W λ . We can define the functional J λ : W λ R by

J λ ( u ) = 1 2 u λ 2 + λ 4 C u 2 * 4 λ 2 * u 2 * 2 * λ ϱ u 2 * p + λ C ϱ u 2 * 2 .

Then, I λ ( u ) J λ ( u ) for any u W λ . Therefore, it is sufficient to construct a sufficiently small minimax level for J λ ( u ) . For every 0 < σ < 1 , one can select φ σ C 0 ( R 3 ) with φ σ r = 1 . Let us define

e λ ( x ) = φ σ ( λ 2 * 3 ( 2 2 * ) x ) .

Then, we obtain supp e λ B λ 2 * 3 ( 2 2 * ) , r σ ( 0 ) . Obviously,

(4.2) J λ ( t e λ ) = t 2 2 R 3 ( e λ 2 + λ A ( x ) e λ 2 ) d x + λ 4 C t 4 e λ 2 * 4 λ t 2 * 2 * R 3 e λ 2 * d x λ ϱ t p R 3 e λ p d x + λ C ϱ t 2 R 3 e λ 2 d x λ 2 2 2 * t 2 2 R 3 ( φ σ 2 + A ( λ 2 * 3 ( 2 2 * ) x ) φ σ 2 ) d x + 1 4 C t 4 φ σ 2 * 4 t 2 * 2 * R 3 φ σ 2 * d x ϱ t p R 3 φ σ p d x + C ϱ t 2 R 3 φ σ 2 d x = λ 2 2 2 * Ψ λ ( t φ σ ) ,

where Ψ λ C 1 ( W λ , R 3 ) and

(4.3) Ψ λ ( u ) 1 2 R 3 ( u 2 + A ( λ 2 * 3 ( 2 2 * ) x ) u p ) d x + 1 4 C u 2 * 4 1 2 * R 3 u 2 * d x ϱ R 3 u p d x + C ϱ R 3 u 2 d x .

Since p > 4 and 2 * > 2 , there is a finite constant t 0 [ 0 , + ) so that

(4.4) max t 0 0 Ψ λ ( t 0 φ σ ) = t 0 2 2 R 3 ( φ σ 2 + A ( λ 2 * 3 ( 2 2 * ) x ) φ σ 2 ) d x + 1 4 C t 0 4 φ σ 2 * 4 t 0 2 * 2 * R 3 φ σ 2 * d x ϱ t 0 p R 3 φ σ p d x + C ϱ t 0 2 R 3 φ σ 2 d x t 0 2 2 R 3 ( φ σ 2 + A ( λ 2 * 3 ( 2 2 * ) x ) φ σ 2 ) d x + 1 4 C t 0 4 φ σ 2 * 4 + C ϱ t 0 2 R 3 φ σ 2 d x .

On the other side, due to A ( 0 ) = 0 and supp φ σ B r σ ( 0 ) , there is a constant Λ σ > 0 so that

0 A ( λ 2 * 3 ( 2 2 * ) x ) σ φ σ 2 2

for all x r σ and λ > Λ σ . This means that

max t 0 Ψ λ ( t φ σ ) t 0 2 2 ( 2 σ ) + 1 4 C t 0 4 σ 2 + C ϱ t 0 2 σ .

Therefore,

(4.5) max t 0 I λ ( t e λ ) ( t 0 2 + C ϱ t 0 2 ) σ + 1 4 C t 0 4 σ 2 λ 2 2 2 *

for all λ > Λ σ .

Now, we have the following conclusion.

Lemma 4.1

Under the assumptions of Lemma 3.2, for any δ > 0 , there is a constant Λ ¯ > 0 such that for any fixed λ > Λ ¯ , there is e ¯ λ with e ¯ λ > ρ λ , I λ ( e ¯ λ ) < 0 and

max t 0 I λ ( t e ¯ λ ) δ λ 2 2 2 * .

Proof

Let σ > 0 small enough that

( 1 + C ϱ ) t 0 2 σ + 1 4 C t 0 2 σ 2 δ .

Take Λ ¯ = Λ σ and select t ¯ λ > 0 so that t ¯ λ e λ λ > ρ λ and I λ ( t ¯ e λ ) 0 for all t t ¯ λ . Set e ¯ λ t ¯ λ e λ to obtain the desired result.□

For any m * N , we select function φ σ i C 0 ( R 3 ) , φ σ i r = 1 and supp φ σ i supp φ σ k = for all 1 i j m * such that φ σ i 2 2 < σ . Let r σ m * > 0 so that supp φ σ i B r σ m * ( 0 ) for i = 1 , 2 , , m * . Let

(4.6) e λ i = φ σ i ( λ 2 * 3 ( 2 2 * ) x )

for i = 1 , 2 , , m * and

H λ , σ m * = span { e λ 1 , e λ 2 , , e λ m * } .

Obviously, for each u = i = 1 m * c i e λ i H λ , σ m * , we have

I λ ( u ) C * i = 1 m * I λ ( c i e λ i ) ,

where C * is a constant. Similar to before, we know that

I λ ( c i e λ i ) λ 2 2 2 * Φ λ ( c i e λ i ) .

Set

β σ max { φ δ i 2 2 : i = 1 , 2 , , m * }

and select Λ m * , σ > 0 such that

V ( λ 2 * 3 ( 2 2 * ) x ) σ β σ for all x r σ m * and λ Λ m * , σ .

Analogously, we obtain

(4.7) max u H λ , σ m * I λ ( u ) ( 1 + C ϱ ) t 0 2 σ + 1 4 C t 0 4 σ 2 C * λ 2 2 2 *

for all λ > Λ m * , σ . Furthermore, we obtain the following lemma.

Lemma 4.2

Under the same assumptions as in Lemma 3.2, then, for all m * N , there exists Λ ¯ m * > 0 such that for each λ > Λ ¯ m * , there is an m * -dimensional subspace H λ m * satisfying

(4.8) max u H λ m * I λ ( v ) δ λ 2 2 2 * .

Proof

We select σ > 0 so small that

( 1 + C ϱ ) t 0 2 σ + 1 4 C t 0 4 σ 2 C * δ

and take H λ , σ m * = H λ m * . From the definition of H λ , σ m * , we can come to the desired conclusion.□

Proof of Theorem 1.1

Considering the function I λ , for any 0 < δ < α 0 , and with the help of Lemma 4.1, we select λ * = Λ σ and define for each λ Λ σ the min-max value

c λ inf τ Γ λ max t [ 0 , 1 ] I λ ( t e ¯ λ ) ,

where

Γ λ = { τ C ( [ 0 , 1 ] , W λ ) : τ ( 0 ) = 0 and τ ( 1 ) = e ¯ λ } .

By Lemmas 3.2 and 4.2, we gain α λ c λ α 0 C * λ 2 2 2 * . By Lemma 3.2 that I λ satisfies the ( PS ) c condition, the mountain-pass theorem states that there exists u λ W λ so that I λ ( u λ ) = c λ and I λ ( u λ ) = 0 . So, u λ is the solution of problem (2.5). Noting that u λ is the critical point of I λ , q 0 [ 2 , 2 * ] , one has

δ λ 2 2 2 * I λ ( u λ ) = I λ ( u λ ) 1 q 0 I λ ( u λ ) , u λ 1 2 1 q 0 R 3 u λ 2 + λ A ( x ) u λ 2 d x + λ 4 λ q 0 R 3 Φ u λ u λ 2 d x + λ q 0 λ 2 * R 3 u λ 2 * d x + λ θ q 0 1 R 3 G ( u ) d x .

Now, we choose q 0 = θ , then

1 2 1 θ R 3 ( u λ 2 + λ A ( x ) u λ 2 ) d x δ λ 2 2 2 * .

Meanwhile, let q 0 = 4 , then

λ 4 λ 2 * R 3 u λ 2 * d x + λ θ 4 1 R 3 G ( u λ ) d x δ λ 2 2 2 * .

By Lemma 4.2, we select σ > 0 small enough that ( 1 + C ϱ ) t 0 2 σ + 1 4 C t 0 4 σ 2 C * δ . So, for any m * N and δ ( 0 , α 0 ) , there is Λ m * , σ such that for each λ > Λ m * , σ , we can select a m * -dimensional subspace H λ m * with max I λ ( H λ m * ) δ λ 2 2 2 * . This completes the proof of Theorem 1.1.□

Proof of Theorem 1.2

Next, let

Γ { h C ( W λ , W λ ) : h is an odd homeomorphism }

and for every A Σ , we define

i ( A ) min h Γ γ ( h ( A ) B ρ λ ) ,

where ρ λ > 0 is a constant defined in Lemma 4.1. Therefore, i ( A ) is a version of Benci pseudo-index [30].

Let

c j inf i ( A ) j sup u A I λ ( u ) , j = 1 , 2 , , m * .

Clearly, c 1 c 2 c m * . Due to α λ c 1 and c m * sup u H λ m * I λ , where α λ is defined as in Lemma 4.1. For any A with i ( A ) 1 , we gain γ ( A B ρ λ ) 1 , which means A B ρ λ . It yields from Lemma 4.1 that

I λ ( u ) α λ , u λ = ρ λ .

So, sup u A I λ ( u ) α λ means c 1 α λ . Considering that the Krasnoselskii genus satisfies the Benci [30] dimension property, we obtain

γ ( h ( H λ m * ) B ρ λ ) = dim H λ m * = m * , h Γ

which means i ( H λ m * ) = m * . So, c m * sup u H λ m * I λ ( u ) . Meanwhile,

(4.9) α λ c 1 c 2 c m * sup u H λ m * I λ ( u ) δ λ 2 2 2 * .

Therefore, problem (1.1) has at least m * pairs of solutions.□

Acknowledgements

The authors thank the reviewers for their constructive remarks on their work.

  1. Funding information: D. Zhang was supported by the National Natural Science Foundation of China (No. 12371455) and the Science and Technology Development Plan Project of Jilin Province, China (Grant No. 20230101182JC). S. Liang was supported by the Young outstanding talents project of Scientific Innovation and entrepreneurship in Jilin (No. 20240601048RC) and the National Natural Science Foundation of China (No. 12571114).

  2. Author contributions: All authors contributed to the study conception, design, material preparation, data collection, and analysis. All authors read and approved the final manuscript.

  3. Conflict of interest: The authors state that there is no conflict of interest.

  4. Data availability statement: Data sharing is not applicable to this article as no data sets were generated or analyzed during the current study.

References

[1] P. d’Avenia and G. Siciliano, Nonlinear Schrödinger equation in the Bopp-Podolsky electrodynamics: solutions in the electrostatic case, J. Differential Equations 267 (2019), 1025–1065, DOI: https://doi.org/10.1016/j.jde.2019.02.001. 10.1016/j.jde.2019.02.001Search in Google Scholar

[2] F. Bopp, Eine lineare Theorie des Elektrons, Ann. Phys. 38 (1940), 345–384, DOI: https://doi.org/10.1002/andp.19404300504. 10.1002/andp.19404300504Search in Google Scholar

[3] B. Podolsky, A generalized electrodynamics. I. Nonquantum, Phys. Rev. 62 (1942), no. 2, 68–71, DOI: https://doi.org/10.1103/PhysRev.62.68. 10.1103/PhysRev.62.68Search in Google Scholar

[4] G. Mie, Grundlagen einer Theorie der Materie, Ann. Phys. 345 (1913), 1–66, DOI: https://doi.org/10.1002/andp.19133450102. 10.1002/andp.19133450102Search in Google Scholar

[5] M. Born, Modified field equations with a finite radius of the electron, Nature 132 (1933), 282, DOI: https://doi.org/10.1038/132282a0. 10.1038/132282a0Search in Google Scholar

[6] M. Born, On the quantum theory of the electromagnetic field, Proc. R. Soc. Lond. Ser. 143 (1934), 410–437, DOI: https://doi.org/10.1098/rspa.1934.0010. 10.1098/rspa.1934.0010Search in Google Scholar

[7] M. Born and L. Infeld, Foundations of the new field theory, Nature 132 (1933), 1004, DOI: https://doi.org/10.1038/1321004b0. 10.1038/1321004b0Search in Google Scholar

[8] M. Born and L. Infeld, Foundations of the new field theory, Proc. R. Soc. Lond. Ser. A Math. Phys. Eng. Sci. 144 (1934), 425–451, DOI: https://doi.org/10.1098/rspa.1934.0059. 10.1098/rspa.1934.0059Search in Google Scholar

[9] A. Azzollini, P. D’Avenia, and A. Pomponio, On the Schrödinger-Maxwell equations under the effect of a general nonlinear term, Ann. Inst. H. Poincaré Anal. Non Linéaire 27 (2010), no. 2, 779–791, DOI: https://doi.org/10.1016/j.anihpc.2009.11.012. 10.1016/j.anihpc.2009.11.012Search in Google Scholar

[10] P. D’Avenia, L. Pisani, and G. Siciliano, Klein-Gordon-Maxwell systems in a bounded domain, Discrete Contin. Dyn. Syst. 26 (2010), 135–149, DOI: https://doi.org/10.3934/dcds.2010.26.135. 10.3934/dcds.2010.26.135Search in Google Scholar

[11] J. Frenkel, 43 problem in classical electrodynamics, Phys. Rev. E 54 (1996), 5859–5862, DOI: https://doi.org/10.1103/PhysRevE.54.5859. 10.1103/PhysRevE.54.5859Search in Google Scholar

[12] M. C. Bertin, B. M. Pimentel, C. E. Valcárcel, and G. E. R. Zambrano, Hamilton-Jacobi formalism for Podolskyas electromagnetic theory on the null-plane, J. Math. Phys. 58 (2017), 082902, DOI: https://doi.org/10.1063/1.4999846. 10.1063/1.4999846Search in Google Scholar

[13] R. Bufalo, B. M. Pimentel, and D. E. Soto, Causal approach for the electron-positron scattering in generalized quantum electrodynamics, Phys. Rev. D 90 (2014), 085012, DOI: https://doi.org/10.1103/PhysRevD.90.085012. 10.1103/PhysRevD.90.085012Search in Google Scholar

[14] R. Bufalo, B. M. Pimentel, and D. E. Soto, Normalizability analysis of the generalized quantum electrodynamics from the causal point of view, Int. J. Modern Phys. A 32 (2017), 1750165, DOI: https://doi.org/10.1142/S0217751X17501652. 10.1142/S0217751X17501652Search in Google Scholar

[15] R. R. Cuzinatto, C. A. M. de Melo, L. G. Medeiros, B. M. Pimentel, and P. J. Pompeia, Bopp-podolsky black holes and the no-hair theorem, Eur. Phys. J. C 78 (2018), 43, DOI: https://doi.org/10.1140/epjc/s10052-018-5525-6. 10.1140/epjc/s10052-018-5525-6Search in Google Scholar

[16] R. R. Cuzinatto, E. M. de Melo, L. G. Medeiros, C. N. D. Souza, and B. M. Pimentel De Broglie-Proca and Bopp-Podolsky massive photon gases in cosmology, Europhys. Lett. 118 (2017), 19001, DOI: https://dx.doi.org/10.1209/0295-5075/118/19001. 10.1209/0295-5075/118/19001Search in Google Scholar

[17] G. Fibich, B. Ilan, and G. Papanicolaou, Self-focusing with fourth-order dispersion, SIAM J. Appl. Math. 62 (2002), 1437–1462, DOI: https://doi.org/10.1137/S0036139901387241. 10.1137/S0036139901387241Search in Google Scholar

[18] G. Siciliano and K. Silva, The fibering method approach for a non-linear Schrödinger equation coupled with the electromagnetic field, Publ. Mat. 64 (2020), 373–390, DOI: https://doi.org/10.5565/PUBLMAT6422001. 10.5565/PUBLMAT6422001Search in Google Scholar

[19] B. Mascaro and G. Siciliano, Positive solutions For a Schrödinger-Bopp-Podolsky system in R3, Commun. Math. 31 (2023), 237–249, DOI: https://doi.org/10.46298/cm.10363. 10.46298/cm.10363Search in Google Scholar

[20] G. M. Figueiredo and G. Siciliano, Multiple solutions for a Schrödinger-Bopp-Podolsky system with positive potentials, Math. Nac. 296 (2023), 2332–2351, DOI: https://doi.org/10.1002/mana.202100308. 10.1002/mana.202100308Search in Google Scholar

[21] S. Chen and X. Tang, On the critical Schrödinger-Bopp-Podolsky system with general nonlinearities, Nonlinear Anal. 195 (2020), 111734, 25 pp, DOI: https://doi.org/10.1016/j.na.2019.111734. 10.1016/j.na.2019.111734Search in Google Scholar

[22] L. Li, P. Pucci, and X. Tang, Ground state solutions for the nonlinear Schrödinger-Bopp-Podolski system with critical Sobolev exponent, Adv. Nonlinear Stud. 20 (2020), 511–538, DOI: https://doi.org/10.1515/ans-2020-2097. 10.1515/ans-2020-2097Search in Google Scholar

[23] H. M. Damian and G. Siciliano, Critical Schrödinger-Bopp-Podolsky systems: solutions in the semiclassical limit, Calc. Var. Partial Differential Equations 63 (2024), 55. DOI: https://doi.org/10.1007/s00526-024-02775-9. 10.1007/s00526-024-02775-9Search in Google Scholar

[24] Y. Ding and F. Lin, Solutions of perturbed Schrodinger equations with critical nonlinearity, Calc. Var. Partial Differ Equations 30 (2007), 231–249, DOI: https://doi.org/10.1007/s00526-007-0091-z. 10.1007/s00526-007-0091-zSearch in Google Scholar

[25] M. Yang and Y. Ding, Existence of semiclassical states for a quasilinear Schrödinger equation with critical exponent in RN, Ann. Mat. Pura Appl. 192 (2013), no. 4, 783–804, DOI: https://doi.org/10.1007/s10231-011-0246-6. 10.1007/s10231-011-0246-6Search in Google Scholar

[26] C. O. Alves, G. M. Figueiredo, and U. B. Severo, A result of multiplicity of solutions for a class of quasilinear equations, Proc. Edinb. Math. Soc. 55 (2012), 291–309, DOI: https://doi.org/10.1017/S001309151000043X. 10.1017/S001309151000043XSearch in Google Scholar

[27] P. L. Lions, The concentration-compactness principle in the calculus of variations, the locally compact case II, Ann. Inst. H. Poincaré Anal. Non Linéaire. 1 (1984), 223–283, DOI: https://doi.org/10.1016/s0294-1449(16)30422-x. 10.1016/s0294-1449(16)30422-xSearch in Google Scholar

[28] M. Poppenberg, K. Schmitt, and Z. Wang, On the existence of soliton solutions to quasilinear Schrödinger equations, Calc. Var. Partial Differential Equations 14 (2002), 329–344, DOI: https://doi.org/10.1007/s005260100105. 10.1007/s005260100105Search in Google Scholar

[29] H. Brézis, Sobolev spaces and partial differential equations, Functional analysis. Universitext Springer, New York, 2011, DOI: https://doi.org/10.1007/978-0-387-70914-7. 10.1007/978-0-387-70914-7Search in Google Scholar

[30] V. Benci, On critical point theory for indefinite functionals in the presence of symmetries, Trans. Amer. Math. Soc. 274 (1982), 533–572, DOI: https://doi.org/10.2307/1999120. 10.1090/S0002-9947-1982-0675067-XSearch in Google Scholar

Received: 2024-01-21
Revised: 2025-05-31
Accepted: 2025-08-19
Published Online: 2025-10-03

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

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

Articles in the same Issue

  1. Research Articles
  2. On approximation by Stancu variant of Bernstein-Durrmeyer-type operators in movable compact disks
  3. Circular n,m-rung orthopair fuzzy sets and their applications in multicriteria decision-making
  4. Grand Triebel-Lizorkin-Morrey spaces
  5. Coefficient estimates and Fekete-Szegö problem for some classes of univalent functions generalized to a complex order
  6. Proofs of two conjectures involving sums of normalized Narayana numbers
  7. On the Laguerre polynomial approximation errors and lower type of entire functions of irregular growth
  8. New convolutions for the Hartley integral transform imbedded in the Banach algebras and convolution-type integral equations
  9. Some inequalities for rational function with prescribed poles and restricted zeros
  10. Lucas difference sequence spaces defined by Orlicz function in 2-normed spaces
  11. Evaluating the efficacy of fuzzy Bayesian networks for financial risk assessment
  12. Fixed point results for contractions of polynomial type
  13. Estimation for spatial semi-functional partial linear regression model with missing response at random
  14. Investigating the controllability of differential systems with nonlinear fractional delays, characterized by the order 0 < η ≤ 1 < ζ ≤ 2
  15. New forms of bilateral inequalities for K-g-frames
  16. Rate of pole detection using Padé approximants to polynomial expansions
  17. Existence results for nonhomogeneous Choquard equation involving p-biharmonic operator and critical growth
  18. Note on the shape-preservation of a new class of Kantorovich-type operators via divided differences
  19. Geršhgorin-type theorems for Z1-eigenvalues of tensors with applications
  20. New topologies derived from the old one via operators
  21. Blow up solutions for two-dimensional semilinear elliptic problem of Liouville type with nonlinear gradient terms
  22. Infinitely many normalized solutions for Schrödinger equations with local sublinear nonlinearity
  23. Nonparametric expectile shortfall regression for functional data
  24. Advancing analytical solutions: Novel wave insights and methodologies for beta fractional Kuralay-II equations
  25. A generalized p-Laplacian problem with parameters
  26. A study of solutions for several classes of systems of complex nonlinear partial differential difference equations in ℂ2
  27. Towards finding equalities involving mixed products of the Moore-Penrose and group inverses by matrix rank methodology
  28. ω -biprojective and ω ¯ -contractible Banach algebras
  29. Coefficient functionals for Sakaguchi-type-Starlike functions subordinated to the three-leaf function
  30. Solutions of several general quadratic partial differential-difference equations in ℂ2
  31. Inequalities for the generalized trigonometric functions with respect to weighted power mean
  32. Optimization of Lagrange problem with higher-order differential inclusion and special boundary-value conditions
  33. Hankel determinants for q-starlike functions connected with q-sine function
  34. System of partial differential hemivariational inequalities involving nonlocal boundary conditions
  35. A new family of multivalent functions defined by certain forms of the quantum integral operator
  36. A matrix approach to compare BLUEs under a linear regression model and its two competing restricted models with applications
  37. Weighted composition operators on bicomplex Lorentz spaces with their characterization and properties
  38. Behavior of spatial curves under different transformations in Euclidean 4-space
  39. Commutators for the maximal and sharp functions with weighted Lipschitz functions on weighted Morrey spaces
  40. A new kind of Durrmeyer-Stancu-type operators
  41. A study of generalized Mittag-Leffler-type function of arbitrary order
  42. On the approximation of Kantorovich-type Szàsz-Charlier operators
  43. Split quaternion Fourier transforms for two-dimensional real invariant field
  44. Quantum injectivity of G-frames in Hilbert spaces
  45. Some results on disjointly weakly compact sets
  46. On Motzkin sequence spaces via q-analog and compact operators
  47. Existence and multiplicity of nontrivial solutions for Schrödinger-Bopp-Podolsky systems with critical nonlinearity in ℝ3
  48. Stability analysis of linear time-invariant difference-differential system with constant and distributed delays
  49. The discriminant of quasi m-boundary singularities
  50. Norm constrained empirical portfolio optimization with stochastic dominance: Robust optimization non-asymptotics
  51. Fuzzy stability of multi-additive mappings
  52. On inequalities involving n-polynomial exponential-type convex functions
  53. Singularities of multiplicative spherical Darboux image and multiplicative rectifying developable surface
  54. A golden ratio technique for equilibrium problem in reflexive Banach spaces
  55. A parallel inertial three-step iteration monotone hybrid algorithm for a finite family of G-nonexpansive mappings in Hilbert spaces endowed with graphs applicable to signal recovery problems
  56. Multiple and unique nontrivial solutions for fractional differential equations with singular property and derivatives contained in the nonlinear term
  57. New soliton solutions for a nonlinear complex hyperbolic Schrödinger dynamical equation with a truncated M-fractional derivative
  58. On a generalization of derangement polynomials and numbers
  59. The description of entire solutions of complex PDEs and PDDEs
  60. A modified RMIL conjugate gradient-based projection algorithm for constrained nonlinear equations: application to image denoising
  61. Fast solution strategies for time-space fractional linear complementarity problems governing American options pricing
  62. Existence results for Robin problems involving p(x)-Laplacian-like operators with convection term
  63. On asymptotic behaviors of a specific cubic functional equation and its hyperstability
  64. The description of entire solutions for some class of complex nonlinear partial differential equation (systems) in C 2
  65. Variations in the geometry of the basins of escape in a modified Hénon–Heiles potential
  66. A Rothe method for a viscoelastic contact problem involving time-fractional derivatives in locking materials
  67. Upper and lower solution method for a higher order ϕ-Laplacian BVPs on an infinite interval
  68. Weyl almost periodic functions on time scales and their Fourier series
  69. Integrable system of null curve and Betchov-Da Rios equation
  70. Fekete–Szegö problems for (β, Φ)-spirllike mapping of complex order γ in Banach space
  71. Modulated convergence: a deferred approach
  72. Infinitely many solutions for an instantaneous and non-instantaneous fourth-order differential system with local assumptions
  73. Existence and nonexistence of normalized solutions for the Biharmonic equation with combined nonlinearities
  74. Ekeland’s variational principle for interval-valued functions with an α-level set in Kaleva-Seikkala’s type fuzzy metric spaces
  75. On Kurzweil integral of fuzzy number valued functions with two variables
  76. On split common null point and common fixed point problems for multivalued demicontractive mappings
  77. Approximation by weighted Durrmeyer-type max-product neural network operators
  78. A new predictor-corrector interior-point algorithm for semidefinite optimization
  79. Densities of measures: fine properties and examples
  80. Review Articles
  81. Characterization generalized derivations of tensor products of nonassociative algebras
  82. On the performance of the new minimax shrinkage estimators for a normal mean vector
  83. Special Issue on Differential Equations and Numerical Analysis - Part II
  84. Existence and optimal control of Hilfer fractional evolution equations
  85. Persistence of a unique periodic wave train in convecting shallow water fluid
  86. Existence results for critical growth Kohn-Laplace equations with jumping nonlinearities
  87. Monotonicity and oscillation for fractional differential equations with Riemann-Liouville derivatives
  88. Nontrivial solutions for a generalized poly-Laplacian system on finite graphs
  89. Stability and bifurcation analysis of a modified chemostat model
  90. Some new quantum derivatives and integrals with their applications in integral error bounds
  91. Special Issue on Nonlinear Evolution Equations and Their Applications - Part II
  92. Analytic solutions of a generalized complex multi-dimensional system with fractional order
  93. Extraction of soliton solutions and Painlevé test for fractional Peyrard-Bishop DNA model
  94. Special Issue on Recent Developments in Fixed-Point Theory and Applications - Part II
  95. Some fixed point results with the vector degree of nondensifiability in generalized Banach spaces and application on coupled Caputo fractional delay differential equations
  96. On the sum form functional equation related to diversity index
  97. Special Issue on International E-Conference on Mathematical and Statistical Sciences - Part II
  98. Simpson, midpoint, and trapezoid-type inequalities for multiplicatively s-convex functions
  99. Converses of nabla Pachpatte-type dynamic inequalities on arbitrary time scales
  100. Special Issue on Blow-up Phenomena in Nonlinear Equations of Mathematical Physics - Part II
  101. Energy decay of a coupled system involving a biharmonic Schrödinger equation with an internal fractional damping
  102. Special Issue on Some Integral Inequalities, Integral Equations, and Applications - Part II
  103. Nonlinear heat equation with viscoelastic term: Global existence and blowup in finite time
  104. New Jensen's bounds for HA-convex mappings with applications to Shannon entropy
  105. Special Issue on Approximation Theory and Special Functions 2024 conference
  106. Ulam-type stability for Caputo-type fractional delay differential equations
  107. Faster approximation to multivariate functions by combined Bernstein-Taylor operators
  108. (λ, ψ)-Bernstein-Kantorovich operators
  109. Some special functions and cylindrical diffusion equation on α-time scale
  110. (q, p)-Mixing Bloch maps
  111. Orthogonalizing q-Bernoulli polynomials
  112. On better approximation order for the max-product Meyer-König and Zeller operator
  113. Moment-based approximation for a renewal reward process with generalized gamma-distributed interference of chance
  114. A note on linear compositions of the Mellin convolution operators in the weighted Mellin-Lebesgue spaces
  115. A new perspective on generalized Laguerre polynomials
  116. Global existence of semilinear system of Klein-Gordon equations in anti-de Sitter spacetime
  117. Estimates for Durrmeyer-type exponential sampling series in Mellin-Orlicz spaces
  118. -αβ-statistical relative uniform convergence for double sequences and its applications
  119. New developments for the Jacobi polynomials
  120. Generalization of Sheffer-λ polynomials
  121. Fractional calculus containing certain bivariate Mittag-Leffler kernel with respect to function
  122. A new type of soft multi rough sets
  123. Special Issue on Variational Methods and Nonlinear PDEs
  124. A note on mean field type equations
  125. Ground states for fractional Kirchhoff double-phase problem with logarithmic nonlinearity
  126. Solution of nonlinear Langevin equations involving Hilfer-Hadamard fractional order derivatives and variable coefficients
  127. Bifurcation, quasi-periodic, and wave solutions to the fractional model of optical fibers in communication systems
  128. Multiplicity and concentration behavior of solutions for the generalized quasilinear Schrödinger equation with critical growth
  129. Ground state solutions to singularly perturbed Chern-Simons-Schrödinger systems with a neutral scalar field
  130. Weak solutions to an asymptotic equation of the variational sine-Gordon equation
  131. Multiplicity of positive solutions for a concave-convex fractional elliptic system with critical growth
Downloaded on 27.3.2026 from https://www.degruyterbrill.com/document/doi/10.1515/dema-2025-0170/html
Scroll to top button