Home Random attractors of Kirchhoff-type reaction–diffusion equations without uniqueness driven by nonlinear colored noise
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Random attractors of Kirchhoff-type reaction–diffusion equations without uniqueness driven by nonlinear colored noise

  • Zhang Zhang and Xiaobin Yao EMAIL logo
Published/Copyright: November 15, 2024

Abstract

In this article, we consider the asymptotic behavior of solutions for the Kirchhoff-type reaction–diffusion equations driven by a nonlinear colored noise defined on unbounded domains. We prove the existence and uniqueness of pullback random attractors by the uniformly estimate.

MSC 2010: 35B40; 35B41

1 Introduction

Ornstein and Uhlenbeck were the first to propose and name the colored noise. In [1,2], first constructed colored noise to approximate the description of velocity stochastic behavior is used to determine the position of particles. Colored noise is applied in complex systems [3,4]. Colored noise is usually used to study the physical system [38]. Recently, there have been new advances in the pathwise dynamics of random systems, which has been proved by smooth approximations of nonlinear noise [5,914].

Consider the reaction–diffusion equations defined on R n :

(1.1) u t + λ u M ( u 2 ) Δ u = f ( x , u ) + g ( t , x ) + G ( x , u ) ζ δ ( θ t ω ) u ( μ , x ) = u μ ( x ) ,

where μ R , x R n , λ > 0 are positive constants, a non-autonomous deterministic external term g L loc 2 ( R , L 2 ( R n ) ) , nonlinear functions f and G satisfy certain conditions, M is a scale function, and the colored noise ζ δ with δ > 0 . When M = 1 , the existence of random attractors of equation (1.1) was proved in [15]. Up to now, the existence of attractors for (1.1) has not been studied by any predecessors when M is a scale function. In this article, we will study the dynamics of (1.1).

Throughout the article, we suppose that both f and g are continuous functions, but not necessarily Lipschitz continuous, this brings without uniqueness of solutions for (1.1). Many authors have studied of asymptotic behavior of multivalued dynamical systems [1620]. Zhao had considered asymptotic behavior of reaction–diffusion equations driven by white noise (additive and linear multiplicative) on unbounded domains [8,21]. The study of random equations can become deterministic ones when the system is driven by white noise, but this transformation cannot be applied to stochastic equations driven by nonlinear white noise, so we cannot obtain the existence of random attractors in systems with nonlinear white noise [57,2224]. Therefore, this article focuses on Kirchhoff-type reaction–diffusion equations driven by nonlinear colored noise.

In this article, in order to prove the uniqueness of equation (1.1), we need to prove the asymptotic compactness of the random attractors. In this article, we need to solve the following 2 questions:

  1.   the study of random attractor of multi-valued dynamical systems is more complex;

  2.   the Sobolev embeddings on unbounded domains are no longer compact;

  3.   the emergence of Kirchhoff-type term makes the estimates more complicated.

To solve the above difficulties, we discuss the measurability of the random attractor of (1.1) by the method of weak upper semicontinuity in [2]. To solve the no longer compact Sobolev embedding in unbounded domains, we use the idea of the Ball energy equation in [25,26] to derive the asymptotic compactness of the solution of problem (1.1).

This article is organized as follows: we will present some results about the pullback random attractors of multivalued non-autonomous random dynamical systems in Section 2. In Section 3, we will prove the existence of the generated random dynamical systems for (1.1) and structure weak and strong upper semicontinuity of multivalued solutions. At last, we will prove the existence of the pullback random attractors for (1.1) by uniform estimates of the solution in Section 4.

2 Preliminaries

Let X ¯ and Y ¯ be the metric space and ( X ¯ ) and ( Y ¯ ) be Borel σ -algebras. We will denote all subsets of Y ¯ as 2 Y ¯ . Let G : X ¯ 2 Y ¯ be measurable in ( X ¯ ) .

Let ( Ω , , P ) be a probability space, where Ω = { ω C ( R , R ) : ω ( 0 ) = 0 } with the open compact topology, is the Borel σ -algebra, and P is the Wiener measure. Let W be a bilateral real valued Wiener process defined on the probability space ( Ω , , P ) . The classical transformation { θ t } t R on Ω is given by θ t ω ( ) = ω ( t + ) ω ( t ) , ω Ω for ω Ω . Suppose ζ δ : Ω R by ζ δ ( ω ) = 1 δ 0 e s δ d W for δ > 0 . Then, the process O δ ( t , ω ) = ζ δ ( θ t ω ) is called the O-U process (i.e. the colored noise), which is a stationary Gaussian process with E ( ζ δ ) = 0 and is the unique stationary solution of the stochastic equation:

d ζ δ + 1 δ ζ δ d t = 1 δ d W .

We will often use the following theorems and lemmas.

Lemma 2.1

Suppose x ¯ 0 X ¯ and y ¯ n G ( x ¯ n ) , if x ¯ n x ¯ 0 in X ¯ , there exists y ¯ 0 G ( x ¯ 0 ) and a subsequence { y ¯ n k } of { y ¯ n } in Y ¯ , then G is upper semicontinuous at x ¯ 0 .

Lemma 2.2

Suppose Φ ¯ ( t , μ , , ) : Ω × X ¯ 2 X ¯ is a multi-valued function. A metric space Ω and a separable Banach space X ¯ . For t R + , μ R , the mapping Φ ¯ ( t , μ , , ) is weakly upper semicontinuous and is ( Ω ) × ( X ¯ ) -measurable.

Theorem 2.3

Suppose Φ ¯ : ( Ω , , P , { θ } t R ) be a multi-valued non-autonomous cocycle on X ¯ with D being an inclusion-closed collection of some families of nonempty subsets of X ¯ , we have the following assumptions

  1. Φ ¯ is D -pullback asymptotically compact in X ¯ ;

  2. For all t R + , μ R , ω Ω , then Φ ¯ ( t , μ , ω , ) : X ¯ 2 Y ¯ is upper semicontinuous;

  3. K = { K ( μ , ω ) : μ R , ω Ω } D is a closed D -pullback absorbing set of Φ ¯ ;

  4. For each m N , t R + , μ R , Φ ¯ ( t , μ , , K ( μ , ) ) : Ω m 2 Y ¯ is weakly upper semicontinuous.

Let A ¯ be a unique D -pullback attractor in D for Φ ¯ that has

A ¯ ( μ , ω ) = r 0 t r Φ ¯ ( t , μ t , θ t ω , K ( μ t , θ t ω ) ) ¯ .

The colored noise ζ δ (see [27]), we have:

Lemma 2.4

If 0 < δ 1 and Ω is a { θ t } t R -invariant subset, for ω Ω ,

  1. (2.1) lim t ± ω ( t ) t = 0 ;

  2. let ( t , ω ) ζ δ ( θ t ω ) = 1 δ 2 0 e s δ θ t ω ( s ) d s is a stationary solution of d ζ δ + 1 δ ζ δ d t = 1 δ d W with continuous trajectories satisfying

    (2.2) lim t ± ζ δ ( θ t ω ) t = 0 ,

    (2.3) lim t ± 1 t 0 t ζ δ ( θ s ω ) d s = 0 ;

  3. if T > 0 , ε > 0 , there exist δ 0 = δ 0 ( μ , ω , T , ε ) > 0 such that for all 0 < δ < δ 0 and t [ μ , μ + T ] ,

    (2.4) 0 t ζ δ ( θ s ω ) d s ω ( t ) < ε .

By (2.4), there exist δ 0 = δ 0 ( μ , ω , T ) > 0 , c = c ( μ , ω , T ) , such that for 0 < δ < δ 0 and t [ μ , μ + T ] ,

(2.5) 0 t ζ δ ( θ s ω ) d s c .

Hereafter, we denote H = L 2 ( R n ) with ( , ) and and denote V = H 1 ( R n ) and V = H 1 ( R ) with V , and L p ( R n ) ( p > 2 ) with norm p . As usual, let c in the article represents a generic positive constant.

3 Construction of multi-valued non-autonomous cocycles

Defining a reaction–diffusion equation with the Kirchhoff-type driven by colored noise:

(3.1) u t + λ u M ( u 2 ) Δ u = f ( x , u ) + g ( t , x ) + G ( x , u ) ζ δ ( θ t ω ) , t > μ , x R n ,

with initial condition

(3.2) u ( μ , x ) = u μ ( x ) , x R n ,

where M is a continuous function related to s and satisfies

(3.3) M ( s ) > κ 0 .

f and G : R n × R R are nonlinear continuous functions, and for u R , y R n ,

(3.4) f ( y , u ) u α 1 u p + ψ 1 ( y ) ,

(3.5) f ( y , u ) α 2 u p 1 + ψ 2 ( y ) ,

(3.6) G ( y , u ) ψ 3 ( u q 1 + 1 ) ,

where α 1 , α 2 , and p , q ( 2 q < p ) are positive constants, ψ 1 L 1 ( R n ) , ψ 2 L p 1 ( R ) , ψ 3 L p 1 L p q ( R n ) with p 1 = p p 1 , p q = p p q .

We will prove that the solution is meaningful.

Definition 3.1

Given μ R , ω Ω , and u μ H , let a continuous function u ( , μ , ω , u τ ) : [ μ , ) H with L loc p ( ( μ , ) , L p ( R n ) ) L loc 2 ( ( μ , ) , V ) , and u t L loc 2 ( ( μ , ) , V ) + L loc p 1 ( ( μ , ) , L p 1 ( R ) ) . Then, u is called a solution of (3.1) and (3.2) with initial data u τ if u ( μ , μ , ω , u μ ) = u μ and for every k V L p ( R n ) ,

(3.7) ( u t , k ) + λ ( u , k ) + ( M ( u 2 ) Δ u , k ) = ( g ( t , ) , k ) + R ( f ( x , u ) + ζ δ ( θ t ω ) G ( x , u ) ) k d x

in the sense of distribution on ( μ , ) .

Then, we will discuss the existence of the solution to problems (3.1) and (3.2) on unbounded domains. First, we will consider the situation in bounded domains. Furthermore, we assume ξ N , define O ξ = { x R : x < ξ } ,

(3.8) u ξ t + λ u ξ M ( u ξ 2 ) Δ u ξ = f ( x , u ξ ) + g ( t , x ) + G ( x , u ξ ) ζ δ ( θ t ω ) , t > μ , x O ξ , u ξ ( t , x ) = 0 , t > τ , x = ξ , u ξ ( μ , x ) = u τ ( x ) , x O ξ .

Similarly [28], under conditions (3.3)–(3.6), one can easily obtain that for every μ R , ω Ω , and u μ H , problem (3.8) has at least one solution u ξ C ( [ μ , ) , H ) L loc p ( ( μ , ) , L p ( R n ) ) L loc 2 ( ( μ , ) , V ) . As ξ , we can obtain the following result for (3.1) and (3.2).

Lemma 3.2

If (3.3)–(3.6) hold and g L loc 2 ( R , H ) . Then, for each μ R , ω Ω , and u μ H , problems (3.1) and (3.2) in the sense of Definition 3.1, there exists a solution u ( , μ , ω , u μ ) and for all t μ , which satisfies the energy equation

(3.9) d d t u ( t , μ , ω , u μ ) 2 + 2 λ u ( t , μ , ω , u μ ) 2 + 2 M ( u 2 ) u 2 = 2 R 2 f ( x , u ( t , μ , ω , u μ ) ) u d x + 2 ( g , u ( t , μ , ω , u μ ) ) + 2 ζ δ ( θ t ω ) R n G ( x , u ( t , μ , ω , u μ ) ) u d x .

In order to obtain the weak semicontinuity and strong upper semicontinuity of the solutions of (3.1) and (3.2), for all m N , we suppose

(3.10) Ω ¯ m = { ω Ω ¯ : ω ( t ) t , t m } ,

which obtain properties as follows:

Lemma 3.3

[15] If the colored noise ζ δ with δ ( 0 , 1 ] , and Ω ¯ m Ω ¯ with m N from (3.10).

  1. Let ω n ω with ω n , ω Ω ¯ m , for t in a compact interval as n , then ζ δ ( θ t ω n ) ζ δ ( θ t ω ) .

  2. If each m N , Ω ¯ m is a closed subset of Ω ¯ with Ω ¯ = m = 1 Ω ¯ m .

  3. Taken m N and ω Ω ¯ m , for every t m , we obtain

    (3.11) ζ δ ( θ t ω ) 2 δ t + 1 .

We will discuss the uniform estimates of solutions for problems (3.1) and (3.2) as follows.

Lemma 3.4

If (3.3)–(3.6) hold. Suppose δ > 0 , μ R , L > 0 , T > 0 , and ω n ω with ω n , ω Ω ¯ m and c = c ( δ , μ , T , L , m , ω ) > 0 , then the solutions of (3.1) and (3.2) satisfy

(3.12) u ¯ ( t , μ , ω n , u μ ) 2 + μ t e λ ( s t ) ( 2 M ( u ( s , μ , ω n , u μ ) 2 ) u ( s , μ , ω n , u μ ) 2 + λ 2 u ( s , μ , ω n , u μ ) 2 + u ( s , μ , ω n , u μ ) p p ) d s c ,

which n N , t [ μ , μ + T ] , and u μ H with u μ L .

Proof

By (3.3), (3.4), (3.6), (3.8), and applying Young’s inequality, we obtain

(3.13) d d t u 2 + 3 2 λ u 2 + 2 M ( u 2 ) u 2 + α 1 u p p c ( 1 + ζ δ ( θ t ) ω p q + ζ δ ( θ t ) ω p 1 + g ( t , ) 2 ) .

By Gronwall’s inequality, we have

(3.14) u ( t , μ , ω n , u μ ) 2 + μ t e λ ( s t ) ( 2 M ( u ( s ) 2 ) u ( s ) 2 + λ 2 u ( s ) 2 + α 1 u ( s ) p p ) d s e λ ( μ t ) u μ 2 + c 1 μ t ( 1 + ζ δ ( θ s ω n ) p q + ζ δ ( θ s ω n ) p 1 + g ( s , ) 2 ) d s .

For s [ μ , μ + T ] as n and ω n ω , we know that ζ δ ( θ s ω n ) ζ δ ( θ s ω ) . Suppose there exists N 1 = N 1 ( T , μ , ω ) 1 , for every n N 1 and s [ μ , μ + T ] , ζ δ ( θ s ω n ) 1 + ζ δ ( θ s ω ) , then ζ δ ( θ s ω ) is continuity in s and exists c ¯ 1 = c 1 ( δ , T , μ , ω ) > 0 , for every n N 1 and s [ μ , μ + T ] ,

(3.15) ζ δ ( θ s ω ) c ¯ 1 , ζ δ ( θ s ω n ) 1 + c ¯ 1 ,

along with (3.14) and (3.15) to obtain (3.12).□

Now, we discuss the weak continuity and strong continuity of solutions of (3.1) and (3.2).

Lemma 3.5

If (3.3)–(3.6) hold, for μ R , t τ , and ω n ω with ω n , ω Ω ¯ m . Suppose a solution u ^ ( , μ , ω n , u τ , n ) of (3.1) and (3.2) with initial data u μ , n .

  1. If u μ , n u μ in H, then a solution u ^ of problems (3.1) and (3.2) with u μ such that

    (3.16) u ( t , μ , ω n , u μ , n ) u ^ ( t , μ , ω , u μ ) in H

    and

    (3.17) u ^ ( , μ , ω n , u μ , n ) u ^ ( , μ , ω , u μ ) in L 2 ( ( μ , μ + T ) , V ) .

  2. If u μ , n u μ strongly in H, then a solution u ^ of problem (3.1) and (3.2) with u μ such that

    u ^ ( t , μ , ω n , u μ , n ) u ^ ( t , μ , ω , u μ ) in H .

Proof

(1) By u μ , n u μ in H , there exists c 1 > 0 such that u μ , n c 1 for every n N . Denote u n ( m ) = u ( m , μ , ω n , u μ , n ) for m [ μ , μ + T ] . If ω n ω with ω n , ω Ω ¯ , by (3.3), (3.5), and Lemma 3.4, for all n N , we have

(3.18) { u n } n = 1 is bounded in L ( μ , μ + T ; H ) L 2 ( μ , μ + T ; V ) L p ( μ , μ + T ; L p ( R n ) ) ,

(3.19) { M ( u n 2 ) } n = 1 is bounded in L 2 ( μ , μ + T , V ) ,

(3.20) { f ( x , u n ) } n = 1 and ζ δ ( θ t ω n ) G ( x , u n ) n = 1 is bounded in L p 1 ( μ , μ + T ; L p 1 ( R n ) ) ,

(3.21) u n t n = 1 is bounded in L 2 ( μ , μ + T ; V ) L p 1 ( μ , μ + T ; L p 1 ( R n ) ) .

Then, there exist u L ( μ , μ + T ; H ) L 2 ( μ , μ + T ; V ) L p ( μ , μ + T ; L p ( R n ) ) , χ L p 1 ( μ , μ + T ; L p 1 ( R n ) ) , and u ¯ ( t 0 ) H for t 0 [ μ , μ + T ] , such that, up to a subsequence

(3.22) u n * u ^ in L ( μ , μ + T ; H ) ,

(3.23) u n u in L p ( μ , μ + T ; L p ( R n ) ) and L 2 ( μ , μ + T ; V ) ,

(3.24) M ( u n 2 ) M ( u 2 ) in L 2 ( μ , μ + T , V ) ,

(3.25) f ( x , u n ) + ζ δ ( θ t ω n ) G ( x , u n ) χ in L p 1 ( μ , μ + T ; L p 1 ( R n ) ) ,

(3.26) u n t u t in L 2 ( μ , T ; V ) L p 1 ( μ , T ; L p 1 ( R n ) ) ,

(3.27) u n ( t 0 , μ , ω , u μ ) u ^ ( t 0 ) in H .

We obtain u is a solution of (3.1) and (3.2) with initial data u ( μ ) = u μ by the standard method. Further

u n ( m ) u ^ ( m ) in  H , for m [ μ , μ + T ] .

(2) Denote u ^ ( t ) = u ^ ( t , μ , ω , u μ ) . By the weak convergence in (1), we have

(3.28) liminf n u n ( t ) u ^ ( t ) .

Next, we prove strong convergence

(3.29) limsup n u n ( t ) u ^ ( t ) .

Taking t μ , T > 0 , such that t [ μ , μ + T ] , by (3.9), we find any weak solution of (3.1) and (3.2) for t [ μ , μ + T ] ,

(3.30) d d t u ^ 2 + 2 λ u ^ 2 + 2 M ( u ^ 2 ) u ^ 2 = 2 ( f ( x , u ^ ) , u ^ ) + 2 ( g , u ^ ) + 2 ζ δ ( θ t ω ) ( G ( x , u ^ ) , u ^ ) .

Applying Gronwall’s inequality, we find

(3.31) u ^ ( t , μ , ω , u μ ) 2 = e λ ( t μ ) u μ 2 μ t e λ ( s t ) ( λ u ( s ) 2 + 2 M ( u ( s ) 2 ) u ( s ) 2 ) d s + 2 μ t e λ ( s t ) ( g ( s ) , u ( s ) ) d s + 2 μ t e λ ( s t ) ( ( f ( x , u ( s ) ) , u ( s ) ) + ζ δ ( θ s ω n ) ( G ( x , u ( s ) ) , u ( s ) ) ) d s .

Replacing ω by ω n and u μ by u μ , n in (3.31), we have

(3.32) u n ( t ) 2 = e λ ( t μ ) u μ , n 2 μ t e λ ( s t ) ( λ u n ( s ) 2 + 2 M ( u n ( s ) 2 ) u n ( s ) 2 ) d s + 2 μ t e λ ( s t ) ( g ( s ) , u n ( s ) ) d s + 2 μ t e λ ( s t ) ( ( f ( x , u n ( s ) ) , u n ( s ) ) + ζ δ ( θ s ω n ) ( G ( x , u n ( s ) ) , u n ( s ) ) ) d s i = 1 4 I i ( n ) .

Next, we will estimate each term in (3.32). First, since u μ , n u μ in H , we find

(3.33) lim n I 1 ( n ) = e λ ( t μ ) u μ 2 .

By (3.16) and (3.17), we have

(3.34) limsup n I 2 ( n ) λ μ t e λ ( s t ) u ^ ( s ) 2 2 μ t e λ ( s t ) M ( u ^ ( s ) 2 ) ( u ^ ( s ) 2 ) d s .

By (3.17), we obtain

(3.35) lim n I 3 ( n ) = 2 μ t e λ ( s t ) ( g ( s ) , u ^ ( s ) ) d s .

Next, we estimate I 4 ( n ) , for k N , we obtain

(3.36) I 4 ( n ) = 2 μ t e λ ( s t ) x k ( f ( x , u n ( s ) ) u n ( s ) + ζ δ ( θ s ω n ) G ( x , u n ( s ) ) u n ( s ) ) d x d s + 2 μ t e λ ( s t ) O k ( f ( x , u n ( s ) ) u n ( s ) + ζ δ ( θ s ω n ) G ( x , u n ( s ) ) u n ( s ) ) d x d s I 41 ( n ) + I 42 ( n ) .

By (3.4), (3.6), and Young’s inequality, such that for k N , N ( ε ) > 0 , we have

(3.37) I 41 ( n ) = c 1 μ t e λ ( s t ) x k ( ψ 1 ( x ) + ψ 3 ( x ) p 1 + ψ 3 ( x ) p q ) d x d s ε .

By (3.22), (3.23), and (3.26), a diagonal process and a compactness argument, we can obtain a subsequence, for k N ,

u n u ^ in L 2 ( μ , μ + T ; L 2 ( O k ) ) .

For any ( t , x ) ( μ , μ + T ) × O k , u ^ n ( t , x ) u ^ ( t , x ) . Since f ( x , u ^ ) + ζ δ ( θ t ω ) G ( x , u ^ ) is continuous in u ^ , we have

f ( x , u n ) + ζ δ ( θ t ω n ) G ( x , u n ) f ( x , u ^ ) + ζ δ ( θ t ω ) G ( x , u ^ ) .

By (3.4) and (3.6), we obtain

(3.38) ψ 1 + c 1 ( ψ 3 p 1 + ψ 3 p q ) f ( x , u ^ ) u ^ ζ δ ( θ t ω ) G ( x , u ^ ) u ^ 0 .

By applying Fatou’s lemma and by Lemma 3.3 (1), we find

(3.39) liminf n ( I 42 ( n ) ) 2 μ t e λ ( s t ) O k ( ( f ( x , u ¯ ( s ) ) , u ¯ ( s ) + G ( x , u ¯ ( s ) ) , u ¯ ( s ) ) ) d x d s ,

together with (3.37) to obtain

(3.40) limsup n I 4 ( n ) 2 μ t e λ ( s t ) O k ( ( f ( x , u ^ ( s ) ) , u ^ ( s ) ) + ζ δ ( θ s ω ) ( G ( x , u ^ ( s ) ) , u ^ ( s ) ) ) d x d s + ε .

Let k , by (3.33), (3.34), and (3.31), we have

limsup n u n ( t ) 2 u ^ ( t ) 2 + ε .

If ε 0 , we obtain (3.29).□

By the consequence Lemma 3.5, we will prove the weak continuity of solution of (3.1) and (3.2) as follows.

Lemma 3.6

If (3.3)–(3.6) hold, μ R and ω Ω . Let a solution u ¯ ( , μ , ω ) of (3.1) and (3.2) with initial date u μ , n . If u μ , n u μ in H, then a solution of problems (3.1) and (3.2) u ^ ( , μ , ω , u μ ) with initial condition u μ such that

u ^ ( t , μ , ω , u μ , n ) u ^ ( t , μ , ω , u μ ) in H f o r t μ

and

u ^ ( , μ , ω , u μ , n ) u ^ ( , μ , ω , u μ ) in L 2 ( ( μ , μ + T ) , V ) for T > 0 .

Denote U ( t + μ , μ , ω , u μ ) be the collection of all solutions of (3.1) and (3.2) at time t + μ with initial condition u μ and initial time μ ; that is

U ( t + μ , μ , ω , u μ ) = { ξ ( t + μ , μ , ω , u μ ) : ξ is a solution of (3.1 ) and ( 3.2) } .

By Lemmas 2.4, 3.3, and 3.5, we have the following result.

Lemma 3.7

If (3.3)–(3.6) hold, μ R , the mapping

U ( t , μ , , ) : Ω ¯ × H 2 H

is measurable in ( Ω ¯ ) × ( H ) .

By Lemmas 3.3 and 3.5, we obtain the following lemma.

Lemma 3.8

Let (3.3)–(3.6) hold. If t R + , μ R , ω Ω ¯ , and u μ H , then the U ( t + μ , μ , ω , u μ ) is a set closed in H.

Proof

If ϕ n U ( t + μ , μ , ω , u μ ) and ϕ H , we will prove ϕ n ϕ , then ϕ U ( t + μ , μ , ω , u μ ) . Since ϕ n U ( t + μ , μ , ω , u μ ) , there exists u n ( t + μ , μ , ω , u μ ) U ( t + μ , μ , ω , u μ ) such that

(3.41) ϕ n = u n ( t + μ , μ , ω , u μ ) .

We know that there exists m N such that ω Ω ¯ m . We have that problems (3.1) and (3.2) have a solution u ^ ( t , μ , ω , u μ ) with initial data u μ by Lemma 3.5 (1) such that

u n ( t + μ , μ , ω , u μ ) u ^ ( t + μ , μ , ω , u μ ) in H ,

from (3.41), we obtain that

(3.42) ϕ n u ^ ( t + μ , μ , ω , u μ ) .

By (3.42), since ξ n ξ in H , we have

ϕ = u ^ ( t + μ , μ , ω , u μ ) U ( t + μ , μ , ω , u μ ) .

This proof is complete.□

Next, we define a multi-valued non-autonomous random dynamical system for (3.1) and (3.2). Denote multi-valued mapping Φ ¯ : R + × R × Ω × H 2 H

(3.43) Φ ¯ ( t , μ , ω , u μ ) = U ( t + μ , μ , θ μ ω , u μ ) = { u ( t + μ , μ , θ μ ω , u μ ) : u is a solution of (3.1) and (3.2) } ,

where ( t , μ , ω , u μ ) R + × R × Ω × H . Since θ μ : Ω Ω is measurable, from Lemma 3.7 we obtain that for μ R , Φ ¯ ( , μ , , ) : R + × Ω × H 2 h is measurable. Then, Φ ¯ is a multi-valued non-autonomous cocycle in H by Lemma 3.8.

From the result of Lemma 3.5(2) and Lemma 2.1, we can obtain the upper semicontinuity of Φ ¯ as follows.

Lemma 3.9

If (3.3)–(3.6) hold. The mapping Φ ¯ ( t , μ , ω , ) : H 2 H is upper semicontinuous for t R + , μ R , ω Ω .

4 Existence and uniqueness of D -pullback random attractors

In this section, we discuss the existence of the D -pullback random attractor of Φ ¯ , where D = { D = { D ( μ , ω ) : μ R , ω Ω ¯ } } satisfying for μ R , ω Ω ¯ , and γ > 0 ,

(4.1) lim t e γ t D ( τ + t , θ t ω ) 2 = 0 .

For this purpose, we consider that g satisfies

(4.2) 0 e λ r g ( r + μ , ) 2 d r , μ R ,

and for c > 0 ,

(4.3) lim t e c t 0 e λ r g ( r + t , ) 2 d r = 0 .

Then, we will obtain uniform estimates of the solutions in H .

Lemma 4.1

If (3.3)–(3.6) hold. Suppose μ R , ω Ω , D = D ( μ , ω ) : μ R , ω Ω D . For every t T and s [ t , 0 ] , there exists T = T ( μ , ω , D , δ ) > 0 such that the solution of problems (3.1) and (3.2) satisfies

(4.4) u ( μ + s , μ t , θ μ ω , u μ t ) 2 + μ t μ + s e λ ( r μ s ) ( 2 M ( u 2 ) u ( r ) 2 + λ 2 u ( r ) 2 + α 1 u ( r ) p p ) d r e λ s ( μ , ω ) ,

where u μ t D ( μ t , θ t ω ) and

(4.5) ( μ , ω ) = 0 e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r ,

where is a positive constant and independent of s , μ , ω , D , and δ .

Proof

By multiplying e λ t to (3.13) and integrating from μ t to μ + s with t 0 and s [ t , 0 ] , then there exists T 1 = T ( μ , ω , D , δ ) > 0 for every t T 1 and s [ t , 0 ] ,

u ( μ + s , μ t , θ μ ω , u μ t ) 2 + μ t μ + s e λ ( r μ s ) ( 2 M ( u 2 ) u ( r ) 2 + λ 2 u ( r ) 2 + α 1 u ( r ) p p ) d r e λ ( t + s ) u μ t 2 + c 1 μ t μ + s e λ ( r μ s ) ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r e λ ( t + s ) D ( μ t , θ t ω ) 2 + c 1 t s e λ ( r s ) ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r = e λ s ( e λ t D ( μ t , θ t ω ) 2 + c 1 t s e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r ) c 2 e λ s 0 e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r .

Due to u μ t D ( μ t , θ t ω ) , we obtain

(4.6) e λ t D ( μ t , θ t ω ) 2 0 as t .

From the consequence of Lemma 4.1, we will prove the existence of the D -pullback absorbing set for Φ ¯ .

Lemma 4.2

If (3.3)–(3.6) and (4.2)–(4.3) hold, then K D is the D -pullback absorbing set of Φ ¯ :

(4.7) K ( μ , ω ) = { u H : u 2 ( μ , ω ) , μ L , ω Ω ¯ } ,

where ( μ , ω ) from (4.5).

Lemma 4.3

If (3.3)–(3.6) and (4.2)–(4.3) hold and Φ ¯ has a closed D -pullback absorbing set K . For m N , t R + , and μ R , the mapping Φ ¯ ( t , μ , , K ( ) ) : Ω ¯ m 2 H is weakly upper semicontinuous.

Proof

Suppose ω n ω in Ω ¯ m and u ˜ n Φ ¯ ( t , μ , ω n , K ( μ , ω n ) ) . We have u ˜ Φ ¯ ( t , μ , ω , K ( μ , ω ) ) such that

(4.8) u ˜ n u ˜ in H .

Due to u ˜ n Φ ¯ ( t , μ , ω n , K ( μ , ω n ) ) and n N , there exist u μ , n K ( μ , ω n ) and a solution u n ( , μ , θ μ ω n , u μ , n ) with u ˜ μ , n such that

(4.9) u ˜ μ , n 2 ( μ , ω n ) = 0 e λ r ( 1 + ζ δ ( θ r ω n ) p q + ζ δ ( θ r ω n ) p 1 + g ( r + μ , ) 2 ) d r

and

(4.10) u ˜ n = u ˜ n ( t + μ , μ , θ μ ω n , u μ , n ) .

By (3.11), for n R , r m and take δ ( 0 , 1 ] , then there have c 1 > 0 such that

(4.11) ζ δ ( θ r ω n ) p q c 1 ( r p q + 1 ) ζ δ ( θ r ω n ) p 1 c 1 ( r p 1 + 1 ) .

Applying the dominated convergence theorem, by Lemma 3.1 and (4.11), which obtain

lim n m e λ r ( 1 + ζ δ ( θ r ω n ) p q + ζ δ ( θ r ω n ) p 1 + g ( r + μ , ) 2 ) d r = m e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r ,

together with Lemma 3.1 (1), we obtain

(4.12) lim n 0 e λ r ( 1 + ζ δ ( θ r ω n ) p q + ζ δ ( θ r ω n ) p 1 + g ( r + μ , ) 2 ) d r = 0 e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r .

By (4.9) and (4.12), we have

(4.13) limsup n u μ , n 2 L 0 e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r ,

then we know that the bounded subsequence { u μ , n } n = 1 in H , thus there exists u μ H

(4.14) u μ , n u μ in H

and

(4.15) u μ 2 0 e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r .

By (4.14) and Lemma 3.5(1), we find that problems (3.1) and (3.2) with initial data u μ have a solution u ¯ = u ¯ ( , μ , θ μ ω , u μ ) for s μ , such that

(4.16) u ¯ n ( s , μ , θ μ ω n , u μ , n ) u ¯ ( s , μ , θ μ ω , u μ ) in H ,

according to (4.10) for t R + , we have

(4.17) u ˜ n u ¯ ( t + μ , μ , θ μ ω , u μ ) in H .

From (4.15) and (4.16), we obtain (4.8) with u ˜ = u ¯ ( t + μ , μ , θ μ ω , u μ ) , which completes the proof.□

Next, we will discuss the asymptotic compactness of solutions of (3.1) and (3.2).

Lemma 4.4

If (3.3)–(3.6) and (4.2) and (4.3) hold, then for every μ R and ω Ω , the sequence

{ u ¯ ( μ , μ t n , θ μ ω , u μ t n ) } n = 1

has a convergent subsequence in H of solutions of (3.1) and (3.2), if t n and u μ t n D ( μ t n , θ t n ω ) with D D .

Proof

When s = 0 , we have that u ¯ ( μ , μ t n , θ μ ω , u μ t n ) is bounded in H by Lemma 4.1. Then, there exist u ˜ H such that a subsequence

(4.18) u ¯ ( μ , μ t n , θ μ ω , u μ t n ) u ˜ .

Hence,

(4.19) liminf n u ¯ ( μ , μ t n , θ μ ω , u μ t n ) u ˜ .

In addition, we need to prove

(4.20) limsup n u ¯ ( μ , μ t n , θ μ ω , u μ t n ) u ˜ ,

which together with (4.19) proves the strong convergence of u ( μ , μ t n , θ μ ω , u μ t n ) in H . Next, we show (4.20) by energy equation (3.30). By Lemma 4.1, there exists N 1 = N 1 ( μ , ω , D ) 1 , such that for all n N 1 , s [ t n , 0 ] ,

(4.21) u ¯ ( μ + s , μ t n , θ μ ω , u μ t n ) 2 e λ s ( μ , ω ) .

Suppose i be a positive integer and N 2 = N 2 ( μ , ω , D , i ) N 1 and t n i for every n N 2 . By (4.21), we find for n N 2 ,

(4.22) u ¯ ( μ i , μ t n , θ μ ω , u μ t n ) 2 e λ i ( μ , ω ) .

Therefore, the sequence { u ¯ ( μ i , μ t n , θ μ ω , u μ t n ) } n = 1 is bounded in H , we obtain u ˜ i H by a diagonal process for all i N such that

(4.23) u ¯ ( μ i , μ t n , θ μ ω , u μ t n ) u ˜ i in H , as n .

As r [ i , 0 ] ,

(4.24) u ¯ ( μ + r , μ t n , θ μ ω , u μ t n ) = u ¯ ( μ + r , μ i , θ μ ω , u ( μ i , μ t n , θ μ ω , u μ t n ) ) .

A subsequence ( t n , u μ t n ) (may depend on i ) and a solution u ¯ i ( , μ i , θ μ ω , u ˜ i ) of problems (3.1) and (3.2) with initial data u i ˜ for i N , for every s [ i , 0 ] , as n , we obtain

u ¯ ( μ + s , μ t n , θ μ ω , u μ t n ) u ¯ i ( μ + s , μ i , θ μ ω , u ˜ i ) in H

and

u ¯ ( , μ i , θ μ ω , u ¯ ( μ i , μ t n , θ μ ω , u μ t n ) ) u ¯ i ( , μ i , θ μ ω , u ˜ i ) in L 2 ( ( μ i , μ ) , V )

Nevertheless, applying a diagonal process, for each one i N , s [ i , 0 ] , as n , we can obtain a common subsequence

(4.25) u ¯ ( μ + s , t n , θ μ ω , u μ t n ) u ¯ i ( μ + s , μ i , θ μ ω , ) in H

and

(4.26) u ¯ ( , μ i , θ μ ω , u ¯ ( μ i , μ t n , θ μ ω , u μ t n ) ) u ¯ i ( , μ i , θ μ ω , u ¯ i ) in L 2 ( ( μ i , μ ) , V ) .

Combining (4.18) with (4.24) and (4.25) when s = 0 , we obtain

(4.27) u ˜ = u ¯ i ( μ , μ i , θ μ ω , u ˜ i ) .

Denote u n , μ i = u ¯ ( μ i , μ t n , θ μ ω , u μ t n ) , u n ( r ) = u ¯ ( r , μ i , θ μ ω , u n , μ i ) , and u i ( μ + s ) by u i ( μ + s , μ i , θ μ ω , u i ˜ ) . For u ¯ ( μ , μ i , θ μ ω , u n , μ i ) with initial data u n , μ i , by (4.24) and (3.31), we have

(4.28) u ( μ , μ t n , θ μ ω , u μ t n ) 2 = e λ i u n , μ i 2 2 μ i μ e λ ( s μ ) M ( u n 2 ) u n ( s ) 2 d s + 2 μ i μ e λ ( s μ ) ( f ( x , u n ( s ) , u n ( s ) ) d s ) + 2 μ i μ e λ ( s μ ) ( g ( s ) , u n ( s ) ) d s + 2 μ i μ e λ ( s μ ) ζ δ ( θ s μ ω ) ( G ( x , u n ( s ) ) , u n ( s ) ) d s λ μ i μ e λ ( s μ ) u n ( s ) 2 d s = e λ i u n , μ i 2 i 0 e λ s ( 2 M ( u n ( s + μ ) 2 ) u n ( s + μ ) 2 + λ u n ( s + μ ) 2 ) d s + 2 i 0 e λ s ( g ( s + μ ) , u n ( s + μ ) ) d s + 2 i 0 e λ s ( f ( x , u n ( s + μ ) ) + ζ δ ( θ s ω ) G ( x , u n ( s + μ ) ) , u n ( s + μ ) ) d s j = 1 4 J i ( i , n ) .

Next, we will estimate each term in (4.28). First, by (4.6) for n N 2 , we obtain that

J 1 ( i , n ) e λ t n d ( μ t n , θ t n , θ t n ω ) 2 + c 1 i e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r .

Due to D D , we obtain that

(4.29) limsup n J 1 ( i , n ) c 1 i ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + τ , ) 2 ) d r .

By (4.25) and (4.26), we have

(4.30) limsup n J 2 ( i , n ) 2 i 0 e λ s ( 2 M ( u i ( s + μ ) 2 ) u i ( s + μ ) 2 + λ u i ( s + μ ) 2 ) d s .

By (4.26), we obtain that

(4.31) lim n J 3 ( i , n ) = 2 i 0 e λ s ( g ( s + μ ) , u i ( s + μ ) ) d s .

Furthermore, for k N , we have

(4.32) J 4 ( i , n ) = 2 i 0 x k e λ s ( f ( x , u n ( s + μ ) ) u n ( s + μ ) + ζ δ ( θ s ω ) G ( x , u n ( s + μ ) ) u n ( s + μ ) ) d x d s + 2 i 0 O k e λ s ( f ( x , u n ( s + μ ) ) u n ( s + μ ) + ζ δ ( θ s ω ) G ( x , u n ( s + μ ) ) u n ( s + μ ) ) d x d s J 41 ( i , n ) + J 42 ( i , n ) .

By (3.3)–(3.6), ψ 1 L 1 ( R n ) and ψ 3 L p 1 ( R n ) L p q ( R n ) , for η > 0 , there exist X 1 = X 1 ( η ) 1 , k X 1 , such that

(4.33) limsup n J 41 ( i , n ) η .

By a diagonal process, we prove that, for k N , such that

(4.34) limsup n J 42 ( i , n ) 2 i 0 O k e λ s ( f ( x , u i ( s + μ ) ) u i ( s + μ ) + ζ δ ( θ s ω ) G ( x , u i ( s + μ ) ) u i ( s + μ ) ) d x d s ,

which together with (4.33) implies that for k X 1 ,

limsup n J 4 ( i , n ) 2 i 0 O k e λ s ( f ( x , u i ( s + μ ) ) u i ( s + μ ) + ζ δ ( θ s ω ) G ( x , u i ( s + μ ) ) u i ( s + μ ) ) d x d s + η .

As k and η 0 , we have

(4.35) limsup n J 4 ( i , n ) 2 i 0 R n e λ s ( f ( x , u i ( s + μ ) ) u i ( s + μ ) + ζ δ ( θ s ω ) G ( x , u i ( s + μ ) ) u i ( s + μ ) ) d x d s .

From (4.28)–(4.32) and (4.35), we obtain

(4.36) limsup n u ( μ , μ t n , θ μ ω , u μ t n ) 2 c 1 i e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r 0 e λ s ( 2 M ( u i ( s + μ ) 2 ) u i ( s + μ ) 2 + λ u i ( s + μ ) 2 ) d s + 2 i 0 e λ s ( g ( s + ) , u i ( s + μ ) ) d s + 2 i 0 e λ s ( f ( x , u i ( s + μ ) ) + ζ δ ( θ s ω ) G ( x , u i ( s + μ ) ) , u i ( s + μ ) ) d s .

Applying energy equation (3.31) to u ¯ , by (3.30), we have

(4.37) u ¯ 2 = u i ( μ , μ i , θ μ ω , u i ¯ ) 2 = e λ i u ¯ i 2 2 μ i μ e λ ( s μ ) M ( u i ( s ) 2 ) u i ( s ) 2 d s + 2 μ i μ e λ ( s μ ) ( f ( x , u i ( s ) ) , u i ( s ) ) d s + 2 μ i μ e λ ( s μ ) ( g ( s ) , u i ( s ) ) d s + 2 μ i μ e λ ( s μ ) ζ δ ( θ s μ ω ) ( G ( x , u i ( s ) ) , u i ( s ) ) d s λ μ i μ e λ ( s μ ) u i ( s ) 2 d s = e λ i u ¯ i 2 i 0 e λ s ( 2 M ( u i ( s + μ ) 2 ) u i ( s + μ ) 2 + λ u i ( s + μ ) 2 ) d s + 2 i 0 e λ s ( g ( s + μ ) , u i ( s + μ ) ) d s + 2 i 0 e λ s ( f ( x , u i ( s + μ ) ) + ζ δ ( θ s ω ) G ( x , u i ( s + μ ) ) , u i ( s + μ ) ) d s .

By (4.36) and (4.37), we obtain

limsup n u ( μ , μ t n , θ μ ω , u μ t n ) 2 u ¯ 2 + c 1 i e λ r ( 1 + ζ δ ( θ r ω ) p q + ζ δ ( θ r ω ) p 1 + g ( r + μ , ) 2 ) d r .

Letting i , we obtain (4.20), which completes the proof.□

Conversely, we will prove Φ ¯ is the D -pullback compactness.

Lemma 4.5

If (3.3)–(3.6) and (4.2) and (4.3) hold, then Φ ¯ is D -pullback asymptotically compact in H.

Proof

Suppose μ R , ω Ω , D D , and u ¯ n Φ ( t n , μ t n , θ t n ω , D ( μ t n , θ t n ω ) ) with t n , we will show a convergent subsequence exists of u ¯ n . There exist u μ t n D ( μ t n , θ t n ω ) and u n ( , μ t n , θ μ ω , u μ t n ) with initial data u μ t n by assumption such that

(4.38) u ¯ n = u n ( μ , μ t n , θ μ , u μ t n ) .

The sequence { u n ( μ , μ t n , θ μ ω , u μ t n ) } n = 1 has convergent subsequence { u ˜ } n = 1 in H , which completes the proof.□

Finally, by Lemmas 3.9, 4.2, 4.3, 4.5, and Theorem 2.3, we obtain the main result of the article as follows.

Theorem 4.6

If (3.3)–(3.6) and (4.2) and (4.3) hold, then problems (3.1) and (3.2) have a unique D -pullback random attractor A ¯ D in H .

Acknowledgements

The authors would like to thank the referees for their valuable comments and suggestions.

  1. Funding information: The research was supported by the Natural Science Foundation of Qinghai Province (No. 2024-ZJ-931) and the Natural Science Foundation of China (No. 12161071).

  2. Author contributions: The whole manuscript was written by Zhang Zhang. All authors reviewed and approved the manuscript.

  3. Conflict of interest: The authors declare that there are no conflicts of interest regarding the publication of this article.

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Received: 2023-10-17
Revised: 2024-09-16
Accepted: 2024-10-01
Published Online: 2024-11-15

© 2024 the author(s), published by De Gruyter

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

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  44. Asymptotic behavior of solutions of a viscoelastic Shear beam model with no rotary inertia: General and optimal decay results
  45. Silting modules over a class of Morita rings
  46. Non-oscillation of linear differential equations with coefficients containing powers of natural logarithm
  47. Mutually unbiased bases via complex projective trigonometry
  48. Hyers-Ulam stability of a nonlinear partial integro-differential equation of order three
  49. On second-order linear Stieltjes differential equations with non-constant coefficients
  50. Complex dynamics of a nonlinear discrete predator-prey system with Allee effect
  51. The fibering method approach for a Schrödinger-Poisson system with p-Laplacian in bounded domains
  52. On discrete inequalities for some classes of sequences
  53. Boundary value problems for integro-differential and singular higher-order differential equations
  54. Existence and properties of soliton solution for the quasilinear Schrödinger system
  55. Hermite-Hadamard-type inequalities for generalized trigonometrically and hyperbolic ρ-convex functions in two dimension
  56. Endpoint boundedness of toroidal pseudo-differential operators
  57. Matrix stretching
  58. A singular perturbation result for a class of periodic-parabolic BVPs
  59. On Laguerre-Sobolev matrix orthogonal polynomials
  60. Pullback attractors for fractional lattice systems with delays in weighted space
  61. Singularities of spherical surface in R4
  62. Variational approach to Kirchhoff-type second-order impulsive differential systems
  63. Convergence rate of the truncated Euler-Maruyama method for highly nonlinear neutral stochastic differential equations with time-dependent delay
  64. On the energy decay of a coupled nonlinear suspension bridge problem with nonlinear feedback
  65. The limit theorems on extreme order statistics and partial sums of i.i.d. random variables
  66. Hardy-type inequalities for a class of iterated operators and their application to Morrey-type spaces
  67. Solving multi-point problem for Volterra-Fredholm integro-differential equations using Dzhumabaev parameterization method
  68. Finite groups with gcd(χ(1), χc (1)) a prime
  69. Small values and functional laws of the iterated logarithm for operator fractional Brownian motion
  70. The hull-kernel topology on prime ideals in ordered semigroups
  71. ℐ-sn-metrizable spaces and the images of semi-metric spaces
  72. Strong laws for weighted sums of widely orthant dependent random variables and applications
  73. An extension of Schweitzer's inequality to Riemann-Liouville fractional integral
  74. Construction of a class of half-discrete Hilbert-type inequalities in the whole plane
  75. Analysis of two-grid method for second-order hyperbolic equation by expanded mixed finite element methods
  76. Note on stability estimation of stochastic difference equations
  77. Trigonometric integrals evaluated in terms of Riemann zeta and Dirichlet beta functions
  78. Purity and hybridness of two tensors on a real hypersurface in complex projective space
  79. Classification of positive solutions for a weighted integral system on the half-space
  80. A quasi-reversibility method for solving nonhomogeneous sideways heat equation
  81. Higher-order nonlocal multipoint q-integral boundary value problems for fractional q-difference equations with dual hybrid terms
  82. Noetherian rings of composite generalized power series
  83. On generalized shifts of the Mellin transform of the Riemann zeta-function
  84. Further results on enumeration of perfect matchings of Cartesian product graphs
  85. A new extended Mulholland's inequality involving one partial sum
  86. Power vector inequalities for operator pairs in Hilbert spaces and their applications
  87. On the common zeros of quasi-modular forms for Γ+0(N) of level N = 1, 2, 3
  88. One special kind of Kloosterman sum and its fourth-power mean
  89. The stability of high ring homomorphisms and derivations on fuzzy Banach algebras
  90. Integral mean estimates of Turán-type inequalities for the polar derivative of a polynomial with restricted zeros
  91. Commutators of multilinear fractional maximal operators with Lipschitz functions on Morrey spaces
  92. Vector optimization problems with weakened convex and weakened affine constraints in linear topological spaces
  93. The curvature entropy inequalities of convex bodies
  94. Brouwer's conjecture for the sum of the k largest Laplacian eigenvalues of some graphs
  95. High-order finite-difference ghost-point methods for elliptic problems in domains with curved boundaries
  96. Riemannian invariants for warped product submanifolds in Q ε m × R and their applications
  97. Generalized quadratic Gauss sums and their 2mth power mean
  98. Euler-α equations in a three-dimensional bounded domain with Dirichlet boundary conditions
  99. Enochs conjecture for cotorsion pairs over recollements of exact categories
  100. Zeros distribution and interlacing property for certain polynomial sequences
  101. Random attractors of Kirchhoff-type reaction–diffusion equations without uniqueness driven by nonlinear colored noise
  102. Study on solutions of the systems of complex product-type PDEs with more general forms in ℂ2
  103. Dynamics in a predator-prey model with predation-driven Allee effect and memory effect
  104. A note on orthogonal decomposition of 𝔰𝔩n over commutative rings
  105. On the δ-chromatic numbers of the Cartesian products of graphs
  106. Binomial convolution sum of divisor functions associated with Dirichlet character modulo 8
  107. Commutator of fractional integral with Lipschitz functions related to Schrödinger operator on local generalized mixed Morrey spaces
  108. System of degenerate parabolic p-Laplacian
  109. Stochastic stability and instability of rumor model
  110. Certain properties and characterizations of a novel family of bivariate 2D-q Hermite polynomials
  111. Stability of an additive-quadratic functional equation in modular spaces
  112. Monotonicity, convexity, and Maclaurin series expansion of Qi's normalized remainder of Maclaurin series expansion with relation to cosine
  113. On k-prime graphs
  114. On the existence of tripartite graphs and n-partite graphs
  115. Classifying pentavalent symmetric graphs of order 12pq
  116. Almost periodic functions on time scales and their properties
  117. Some results on uniqueness and higher order difference equations
  118. Coding of hypersurfaces in Euclidean spaces by a constant vector
  119. Cycle integrals and rational period functions for Γ0+(2) and Γ0+(3)
  120. Degrees of (L, M)-fuzzy bornologies
  121. A matrix approach to determine optimal predictors in a constrained linear mixed model
  122. On ideals of affine semigroups and affine semigroups with maximal embedding dimension
  123. Solutions of linear control systems on Lie groups
  124. A uniqueness result for the fractional Schrödinger-Poisson system with strong singularity
  125. On prime spaces of neutrosophic extended triplet groups
  126. On a generalized Krasnoselskii fixed point theorem
  127. On the relation between one-sided duoness and commutators
  128. Non-homogeneous BVPs for second-order symmetric Hamiltonian systems
  129. Erratum
  130. Erratum to “Infinitesimals via Cauchy sequences: Refining the classical equivalence”
  131. Corrigendum
  132. Corrigendum to “Matrix stretching”
  133. Corrigendum to “A comprehensive review of the recent numerical methods for solving FPDEs”
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