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On superstability of derivations in Banach algebras

  • Ick-Soon Chang , Hark-Mahn Kim and Jaiok Roh EMAIL logo
Published/Copyright: June 16, 2025

Abstract

In this article, we consider some types of derivations in Banach algebras. In detail, we investigate the question of whether the superstability can be achieved under some conditions for some types of derivations, such as Jordan derivations, generalized Lie 2-derivations, and generalized Lie derivations.

MSC 2010: 16N60; 16W80; 39B72; 39B82; 46H40

1 Introduction

Let A be an algebra, not necessarily with unit e , with center Z ( A ) . For all x , y A , the symbol [ x , y ] will denote the commutator x y y x and the symbol x y will write the anticommutator x y + y x . A derivation is an additive mapping δ : A A satisfying δ ( x y ) = δ ( x ) y + x δ ( y ) for all x , y A . A Jordan derivation is an additive mapping δ : A A satisfying δ ( x y ) = δ ( x ) y + x δ ( y ) for all x , y A . This concept has been generalized in many ways. For example, a Lie derivation defined as an additive mapping δ : A A satisfying δ ( [ x , y ] ) = [ δ ( x ) , y ] + [ x , δ ( y ) ] for all x , y A . In addition, an additive mapping δ : A A is called linear if δ ( t x ) = t δ ( x ) for all x A and all t C .

A type of stability was studied by Bake et al. [1]. Indeed, they proved that if a function is approximately exponential, then it is either a true exponential function or bounded. Then the exponential functional equation is said to be superstable. It was the first result concerning the superstability phenomenon of functional equations. Baker [2] generalized this result as follows: Let ( S , ) be an arbitrary semigroup, and let f map S into the field C . Assume that f is an approximately exponential function, i.e., there exists a nonnegative number ε > 0 such that

f ( x y ) f ( x ) f ( y ) ε ,

for all x , y S . Then f is either bounded or exponential.

Later, the superstability for derivations between operator algebras was investigated by Šemrl [3]. Badora presented the stability concerning derivations in [4]. The study of the stability mentioned earlier has its origin in the famous talk of Ulam [5]. Hyers [6] had answered affirmatively the question of Ulam for Banach spaces. After then, many authors have generalized Hyers’ result; see, for example, [79]. A great amount of subsequent studies of stability to various functional equations involving derivations are still being done. The main objective of the present article is to investigate some types of derivations in Banach algebras. We first try to prove some theorems related to superstability of these derivations in Banach algebras. In addition, we considered the continuity of these derivations.

2 Jordan derivations

In this article, we set T ε { e i θ : 0 θ ε } for a given ε > 0 . As an example of a Jordan derivation in Banach algebra, we can consider the following:

Let A = M 2 ( C ) be the Banach algebra of all 2 × 2 upper triangle matrices over the complex field C . We define a map δ : A A by

δ a b 0 c = 0 b 0 0 .

Then, we see that δ is a Jordan derivation.

Next, we introduce the following lemma necessary to prove theorem on Jordan derivations.

Lemma 2.1

Let be a linear mapping on a Banach algebra A and let τ and δ be mappings such that

(2.1) ( x y ) = τ ( x ) y + x δ ( y ) for a l l x , y A .

If A is semiprime, then τ and δ satisfy

τ ( t x ) t τ ( x ) Z ( A ) , τ ( x + y ) τ ( x ) τ ( y ) Z ( A ) ( x , y A , t C ) , δ ( t x ) t δ ( x ) Z ( A ) , δ ( x + y ) δ ( x ) δ ( y ) Z ( A ) ( x , y A , t C ) .

In particular, if A has a unit, the mappings τ and δ are linear.

Proof

It follows from (2.1) that for t C and all x , y A ,

t τ ( x ) y + t x δ ( y ) = t ( x y ) = ( x t y ) = t τ ( x ) y + x δ ( t y ) .

Hence, we have

(2.2) x ( t δ ( y ) δ ( t y ) ) = 0 for all x , y A ,

which gives that

(2.3) x ( t δ ( y ) δ ( t y ) ) = ( t δ ( y ) δ ( t y ) ) x for all x , y A .

By substituting w x in place of x in equation (2.2) and using (2.3), we obtain

(2.4) w [ x , t δ ( y ) δ ( t y ) ] = 0 ,

that is, [ x , t δ ( y ) δ ( t y ) ] lies in the right annihilator ran ( A ) of A . If A is semiprime, we have from (2.4) that [ x , t δ ( y ) δ ( t y ) ] = 0 . So we arrive at δ ( t y ) t δ ( y ) Z ( A ) . If A has a unit, set x = e in (2.2). Then δ ( t y ) = t δ ( y ) is true.

In view of (2.1), we have

(2.5) ( x ( y + z ) ) = τ ( x ) y + τ ( x ) z + x δ ( y + z ) .

Again, by (2.1) and additivity of , we obtain

(2.6) ( x ( y + z ) ) = ( x y ) + ( x z ) = τ ( x ) y + τ ( x ) z + x ( δ ( y ) + δ ( z ) ) .

By combining (2.5) and (2.6), we see that

(2.7) x ( δ ( y + z ) ( δ ( y ) + δ ( z ) ) ) = 0 .

By using (2.7), we obtain similar results to (2.3) and (2.4). As a result, if A is smiprime, then we have δ ( y + z ) δ ( y ) δ ( z ) Z ( A ) . Moreover, if A contains the unit, then we have δ ( y + z ) = δ ( y ) + δ ( z ) . It can be proved in a similar way for τ . The lemma is completely established.□

Bhushan et al. [10] introduce the notion of centrally-extended Jordan derivation (CE-Jordan derivation) of a ring A as a mapping δ : A A satisfying

δ ( x + y ) δ ( x ) δ ( y ) Z ( A ) for all x , y A , δ ( x y ) δ ( x ) y x δ ( y ) Z ( A ) for all x , y A .

In [10, Lemma 3.4], it is proved that if A is a 2-torsion free ring with no nonzero central ideals, then every CE-Jordan derivation is additive. Due to this fact and Lemma 2.1, we obtain the following result.

Theorem 2.2

Let A be a semiprime Banach algebra with no nonzero central ideals. Assume that mappings Φ : A × A [ 0 , ) and φ : A × A [ 0 , ) satisfy

  1. σ ( x , y ) j = 0 1 2 j Φ ( 2 j x , 2 j y ) < ( x , y A ) ,

  2. lim n 1 2 n φ ( 2 n x , y ) = lim n 1 2 n φ ( x , 2 n y ) = 0 ( x , y A ) .

Suppose that δ : A A is a mapping subjected to

(2.8) δ ( x + y ) δ ( x ) δ ( y ) Φ ( x , y ) ( x , y A ) ,

(2.9) δ ( x y ) δ ( x ) y x δ ( y ) φ ( x , y ) ( x , y A ) .

Then δ is a Jordan derivation. Moreover, δ is a derivation.

Proof

It follows from (2.8) and the Găvruta theorem [8] that there exists a unique additive mapping : A A satisfying δ ( x ) ( x ) 1 2 σ ( x , x ) for all x A . In this case, the mapping is defined as follows:

(2.10) ( x ) lim n δ ( 2 n x ) 2 n for all x A .

We then have by (2.9) that

( x y ) ( x ) y x ( y ) = lim n 1 2 2 n δ ( 2 n x 2 n y ) δ ( 2 n x ) 2 n y 2 n x δ ( 2 n y ) lim n 1 2 2 n φ ( 2 n x , 2 n y ) = 0 ,

which implies that

(2.11) ( x y ) = ( x ) y + x ( y ) for all x , y A .

By (2.9), we see that

( x y ) ( x ) y x δ ( y ) = lim n 1 2 n δ ( 2 n x y ) δ ( 2 n x ) y 2 n x δ ( y ) lim n 1 2 n φ ( 2 n x , y ) = 0 .

Hence, we obtain

(2.12) ( x y ) = ( x ) y + x δ ( y ) for all x , y A .

So, by virtue of Lemma 2.1, we find that

(2.13) δ ( x + y ) δ ( x ) δ ( y ) Z ( A ) for all x , y A .

By combining (2.11) and (2.12), we obtain

(2.14) x ( y ) = x δ ( y ) for all x , y A .

But then, we found that

( x y ) δ ( x ) y x ( y ) = lim n 1 2 n δ ( x 2 n y ) δ ( x ) 2 n y x δ ( 2 n y ) lim n 1 2 n φ ( x , 2 n y ) = 0 .

This gives that

(2.15) ( x y ) = δ ( x ) y + x ( y ) for all x , y A .

Considering (2.11) and (2.15), we are lead to

(2.16) ( x ) y = δ ( x ) y for all x , y A .

Therefore, with the help of (2.14) and (2.15), we figure out that

(2.17) ( x y ) = δ ( x ) y + x δ ( y ) for all x , y A .

The expression (2.16) can be represented as follows:

(2.18) ( ( x ) δ ( x ) ) y = 0 for all x , y A .

By replacing y by y w in (2.18) and using (2.18), we obtain

[ ( x ) δ ( x ) , y ] w = 0 for all x , y , w A .

That is, [ ( x ) δ ( x ) , y ] lies in the left annihilator lan ( A ) of A . The semiprimeness of A implies that [ ( x ) δ ( x ) , y ] = 0 . So we have

(2.19) [ ( x ) , y ] = [ δ ( x ) , y ] for all x , y A .

By applying (2.17) and (2.19), we yield that [ δ ( x y ) δ ( x ) y x δ ( y ) , z ] = 0 , that is,

(2.20) δ ( x y ) δ ( x ) y x δ ( y ) Z ( A ) for all x , y A .

Then, due to (2.13) and (2.20), we see that the mapping δ is a CE-Jordan derivation. So, based on [10, Lemma 3.4], δ is additive, hence the relation (2.10) forces to δ = . Therefore, by referring (2.17), we conclude that

δ ( x y ) = δ ( x ) y + x δ ( y ) for all x , y A .

Consequently, δ is a Jordan derivation. Moreover, since A is semiprime, δ is a derivation [11]. This proves the theorem.□

To prove the next corollary, we will use the following well-known results [12,13]. Note that semisimple algebras are semiprime and that any linear derivation on a semisimple Banach algebra is continuous.

Corollary 2.3

Let A be a semisimple Banach algebra with no nonzero central ideals. Assume that mappings Φ : A × A [ 0 , ) and φ : A × A [ 0 , ) satisfy the assumptions of Theorem 2.2. Suppose that δ : A A is a mapping such that

(2.21) δ ( t x + t y ) t δ ( x ) t δ ( y ) Φ ( x , y ) ( x , y A , t T ε ) ,

together with (2.9). Then δ is a continuous derivation.

Proof

We first consider t = 1 in (2.21). According to Theorem 2.2, we see that δ is a derivation.

Inequality (2.21) yields that for all x A and all t T ε ,

( t x ) t ( x ) = lim n 1 2 n δ ( 2 n t x ) 2 t δ ( 2 n 1 x ) lim n 1 2 n Φ ( 2 n 1 x , 2 n 1 x ) = 0 ,

where the mapping is defined as (2.10). Hence, we have ( t x ) = t ( x ) . Then the mapping is linear (refer to [14]). Therefore, since δ = , the derivation δ is also linear. The semisimplicity of A ensures that δ is continuous. This completes the proof of the corollary.□

3 Generalized Lie 2-derivations and generalized Lie derivations

We first prove Lemma 3.1 for the proof of Theorem 3.2 concerning generalized Lie 2-derivations.

Lemma 3.1

Let A be a Banach algebra and let : A A be a linear mapping. Suppose that τ : A A and δ : A A are mappings such that

(3.1) ( [ x , y ] ) = [ τ ( x ) , y ] + [ x , δ ( y ) ] for a l l x , y A .

If Z ( A ) = { 0 } holds, then the mappings τ and δ are linear.

Proof

For all x , y A and all t C ,

t [ τ ( x ) , y ] + [ x , δ ( t y ) ] = ( [ x , t y ] ) = t ( [ x , y ] ) = t [ τ ( x ) , y ] + [ x , t δ ( y ) ] .

Then δ satisfies the equation [ x , δ ( t y ) t δ ( y ) ] = 0 , that is,

δ ( t x ) t δ ( x ) Z ( A ) ( x A , t C ) .

We now have from (3.1) that

(3.2) ( [ x , y + z ] ) = [ τ ( x ) , y + z ] + [ x , δ ( y + z ) ] .

On the other hand, if we calculate in a different way, we obtain

(3.3) ( [ x , y + z ] ) = ( [ x , y ] ) + ( [ x , z ] ) = [ τ ( x ) , y + z ] + [ x , δ ( y ) + δ ( z ) ] .

By combining (3.2) and (3.3) gives [ x , δ ( y + z ) δ ( y ) δ ( z ) ] = 0 , which forces to

δ ( x + y ) δ ( x ) δ ( y ) Z ( A ) ( x , y A ) .

It can be similarly proved that τ also satisfies the following relation:

τ ( t x ) t τ ( x ) Z ( A ) , τ ( x + y ) τ ( x ) τ ( y ) Z ( A ) ( x , y A , t C ) .

Therefore, if Z ( A ) = { 0 } , then τ and δ are linear, which is the assertion of Lemma.□

A generalized Lie 2-derivation δ 0 : A A associated with the Lie derivation δ 1 means that A generalized Lie 2-derivation δ 0 : A A is a linear mapping satisfying δ 0 ( [ x , y ] ) = [ δ 0 ( x ) , y ] + [ x , δ 1 ( y ) ] for all x , y A , where δ 1 : A A is a Lie derivation, that is, δ 1 is a linear mapping such that δ 1 ( [ x , y ] ) = [ δ 1 ( x ) , y ] + [ x , δ 1 ( y ) ] for all x , y A , see to paper [15,16].

Theorem 3.2

Let A be a Banach algebra. Assume that mappings Φ : A × A [ 0 , ) , φ 0 : A × A [ 0 , ) and φ 1 : A × A [ 0 , ) satisfy

  1. σ ( x , y ) j = 0 1 2 j Φ ( 2 j x , 2 j y ) < ( x , y A ) ,

  2. lim n 1 2 n φ k ( 2 n x , y ) = lim n 1 2 n φ k ( x , 2 n y ) = 0 ( k = 0 , 1 ; x , y A ) .

Suppose that δ 0 : A A and δ 1 : A A are mappings such that for each k = 0 , 1,

(3.4) δ k ( t x + t y ) t δ k ( x ) t δ k ( y ) Φ ( x , y ) ( x , y A , t T ε )

and the following inequalities

(3.5) δ 0 ( [ x , y ] ) [ δ 0 ( x ) , y ] [ x , δ 1 ( y ) ] φ 0 ( x , y ) ( x , y A ) ,

(3.6) δ 1 ( [ x , y ] ) [ δ 1 ( x ) , y ] [ x , δ 1 ( y ) ] φ 1 ( x , y ) ( x , y A ) .

If Z ( A ) = { 0 } , then δ 0 is a generalized Lie 2-derivation associated with the Lie derivation δ 1 .

Proof

Employing the same method as in the proof of Corollary 2.3, for each k = 0 , 1, there exists a unique linear mapping k : A A satisfying δ k ( x ) k ( x ) 1 2 σ ( x , x ) for all x A , where the mapping k is defined as (2.10).

It follows from (3.5) that

0 ( [ x , y ] ) [ 0 ( x ) , y ] [ x , 1 ( y ) ] = lim n 1 2 2 n δ 0 ( [ 2 n x , 2 n y ] ) [ δ 0 ( 2 n x ) , 2 n y ] [ 2 n x , δ 1 ( 2 n y ) ] lim n 1 2 2 n φ 0 ( 2 n x , 2 n y ) = 0 .

This means that

(3.7) 0 ( [ x , y ] ) = [ 0 ( x ) , y ] + [ x , 1 ( y ) ] for all x , y A .

Moreover, we have by (3.5) that

0 ( [ x , y ] ) [ 0 ( x ) , y ] [ x , δ 1 ( y ) ] = lim n 1 2 n δ 0 ( [ 2 n x , y ] ) [ δ 0 ( 2 n x ) , y ] [ 2 n x , δ 1 ( y ) ] lim n 1 2 n φ 0 ( 2 n x , y ) = 0 ,

which implies that

(3.8) 0 ( [ x , y ] ) = [ 0 ( x ) , y ] + [ x , δ 1 ( y ) ] for all x , y A .

It follows from (3.5) that

0 ( [ x , y ] ) [ δ 0 ( x ) , y ] [ x , 1 ( y ) ] = lim n 1 2 n δ 0 ( [ x , 2 n y ] ) [ δ 0 ( 2 n x ) , 2 n y ] [ 2 n x , δ 1 ( 2 n y ) ] lim n 1 2 n φ 0 ( x , 2 n y ) = 0 .

Hence, we have

(3.9) 0 ( [ x , y ] ) = [ δ 0 ( x ) , y ] + [ x , 1 ( y ) ] for all x , y A .

Expressions (3.8), (3.9), and Lemma 3.1 ensure that δ 0 and δ 1 are linear. Then by (2.10), we are lead to δ 0 = 0 and δ 1 = 1 . Thus, we obtain by (3.7) that

δ 0 ( [ x , y ] ) = [ δ 0 ( x ) , y ] + [ x , δ 1 ( y ) ] for all x , y A .

The following equation δ 1 ( [ x , y ] ) = [ δ 1 ( x ) , y ] + [ x , δ 1 ( y ) ] can be proved in a similar way to the one proved above. Hence, δ 1 is a Lie derivation. Therefore, δ 0 is a generalized Lie 2-derivation associated with the Lie derivation δ 1 . This completes the proof.□

We consider the following property regarding Lie derivations.

Theorem 3.3

Let A be a semisimple Banach algebra. Assume that mappings Φ : A × A [ 0 , ) and φ : A × A [ 0 , ) satisfy the assumptions of Theorem 3.2. Suppose that δ : A A is a mapping subjected to the inequality (2.21) and

[ δ ( [ x , y ] ) [ δ ( x ) , y ] [ x , δ ( y ) ] Φ ( x , y )

for all x , y A . If Z ( A ) = { 0 } , then δ is a continuous Lie derivation.

Proof

By similar approach to the proof of Corollary 2.3 and Theorem 3.2, we can see that δ is a Lie derivation. Also, it is known that every Lie derivation on a semisimple Banach algebra A is continuous if Z ( A ) = 0 (refer to [17]). Therefore, we complete the proof.□

The concept of generalized Lie derivation can be found in [15,16]: A linear mapping δ 0 : A A is called a generalized Lie derivation with the associated derivation δ 1 if there exists a derivation δ 1 : A A such that

(3.10) δ 0 ( [ x , y ] ) = δ 0 ( x ) y δ 0 ( y ) x + x δ 1 ( y ) y δ 1 ( x ) for all x , y A .

For an example of a generalized Lie derivation in Banach algebra, we have the following:

Let A = M 2 ( C ) be the Banach algebra of all 2 × 2 upper triangle matrices over the complex field C . We define a map δ 0 : A A by

δ 0 a b 0 c = a 2 b 0 0 .

Then, we see that δ 0 is a generalized Lie derivation with an associated derivation δ 1 , where δ 1 is a map defined by

δ 1 a b 0 c = 0 b 0 0 .

Note that the definition of the generalized Lie derivation should not be confused with the concept of the generalized Lie 2-derivation. Now we consider superstability of generalized Lie derivation.

Theorem 3.4

Let A be either a semiprime Banach algebra or a unital Banach algebra. Assume that mappings Φ : A × A [ 0 , ) , φ 0 : A × A [ 0 , ) and φ 1 : A × A [ 0 , ) satisfy the assumptions of Theorem 3.2. If δ 0 : A A and δ 1 : A A are mappings such that the inequality (3.4) and

(3.11) δ 0 ( [ x , y ] ) δ 0 ( x ) y + δ 0 ( y ) x x δ 1 ( y ) + y δ 1 ( x ) φ 0 ( x , y ) ( x , y A ) ,

(3.12) δ 1 ( x y ) δ 1 ( x ) y x δ 1 ( y ) φ 1 ( x , y ) ( x , y A )

are fulfilled, then δ 0 is a generalized Lie derivation associated with the derivation δ 1 .

Proof

As we did in the proof of Corollary 2.3, for each k = 0,1 , there exists a unique linear mapping k : A A satisfying δ k ( x ) k ( x ) 1 2 σ ( x , x ) for all x A . Here, the mapping k is defined as (2.10).

It follows from (3.11) that

0 ( [ x , y ] ) δ 0 ( x ) y + 0 ( y ) x x 1 ( y ) + y δ 1 ( x ) = lim n 1 2 n δ 0 ( [ x , 2 n y ] ) 2 n δ 0 ( x ) y + δ 0 ( 2 n y ) x x δ 1 ( 2 n y ) + 2 n y δ 1 ( x ) lim n 1 2 n φ 0 ( x , 2 n y ) = 0 .

Hence, we figure out that

(3.13) 0 ( [ x , y ] ) = δ 0 ( x ) y 0 ( y ) x + x 1 ( y ) y δ 1 ( x ) for all x , y A .

On the other hand, in view of (3.12), we see that

1 ( x y ) 1 ( x ) y x δ 1 ( y ) = lim n 1 2 n δ 1 ( 2 n x y ) δ 1 ( 2 n x ) y 2 n x δ 1 ( y ) lim n 1 2 n φ 1 ( 2 n x , y ) = 0 ,

which implies that

1 ( x y ) = 1 ( x ) y + x δ 1 ( y ) for all x , y A .

Then we have by [18, Lemma 2.1] that δ 1 is linear. Considering (2.10) gives δ 1 = 1 and then, δ 1 is a derivation.

Equation (3.13) can be expressed as follows:

(3.14) 0 ( [ x , y ] ) = δ 0 ( x ) y 0 ( y ) x + x δ 1 ( y ) y δ 1 ( x ) for all x , y A .

Hence, by linearity of δ 1 , we obtain

(3.15) 0 ( [ t x , y ] ) = δ 0 ( t x ) y t 0 ( y ) x + t x δ 1 ( y ) t y δ 1 ( x )

for all x , y A and all t C . Furthermore, due to (3.14), we have

(3.16) 0 ( [ t x , y ] ) = t 0 ( [ x , y ] ) = t δ 0 ( x ) y t 0 ( y ) x + t x δ 1 ( y ) t y δ 1 ( x )

for all x , y A and all t C . By combining (3.15) and (3.16), we are lead to

(3.17) ( δ 0 ( t x ) t δ 0 ( x ) ) y = 0 ( x , y A , t C ) .

This means that δ 0 ( t x ) t δ 0 ( x ) lies in the left annihilator lan ( A ) of A . If A is semiprime, expression (3.17) ensures that δ 0 ( t x ) = t δ 0 ( x ) . If A has a unit, set y = e in (3.17). Then we arrive at δ 0 ( t x ) = t δ 0 ( x ) .

But then, we have by (3.14) and by additivity of δ 1 , that

(3.18) 0 ( [ x + z , y ] ) = δ 0 ( x + z ) y 0 ( y ) x 0 ( y ) z + x δ 1 ( y ) + z δ 1 ( y ) y δ 1 ( x ) y δ 1 ( z ) .

Another way to compute this is

(3.19) 0 ( [ x + z , y ] ) = 0 ( [ x , y ] ) + 0 ( [ z , y ] ) = δ 0 ( x ) y 0 ( y ) x + x δ 1 ( y ) y δ 1 ( x ) + δ 0 ( z ) y 0 ( y ) z + z δ 1 ( y ) y δ 1 ( z ) .

Combining (3.18) and (3.19) yields

(3.20) ( δ 0 ( x + z ) δ 0 ( x ) δ 0 ( z ) ) y = 0 for all x , y A .

That is, δ 0 ( x + z ) δ 0 ( x ) δ 0 ( z ) lies in the left annihilator lan ( A ) of A . If A is semiprime, then by (3.20), δ satisfies δ 0 ( x + z ) = δ 0 ( x ) + δ 0 ( z ) . If A has a unit, let y = e in (3.20). Then δ 0 ( x + z ) = δ 0 ( x ) + δ 0 ( z ) .

Thus, δ 0 is linear, hence we are forced to conclude that δ 0 = 0 . Therefore, expression (3.14) guarantees that δ 0 satisfies (3.10). Consequently, δ 0 is a generalized Lie derivation with the associated derivation δ 1 . The theorem is proved.□

Acknowledgment

We would like to thank reviewers for taking the time and effort necessary to review the manuscript. We sincerely appreciate all valuable comments and suggestions, which helped us to improve the quality of the manuscript.

  1. Funding information: This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2021R1A2C109489611).

  2. Author contributions: All authors contributed to the writing, review, and editing of this paper. 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: No data were gathered for this article.

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Received: 2024-11-13
Revised: 2025-02-13
Accepted: 2025-03-31
Published Online: 2025-06-16

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  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
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