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Coding of hypersurfaces in Euclidean spaces by a constant vector

  • Sharief Deshmukh and Mohammed Guediri EMAIL logo
Published/Copyright: December 17, 2024

Abstract

An n -dimensional Riemannian manifold ( N n , g ) isometrically immersed in Euclidean space R n + 1 with unit normal ζ and shape operator S , for a fixed constant unit vector a in R n + 1 induces a vector field v and a smooth function ρ on N n called its code vector and coding function, respectively. The sextuple ( N n , g , ζ , S , v , ρ ) is called a coded hypersurface of Euclidean space R n + 1 . In the first result of this article, we show that a compact and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of R n + 1 has integral of Ricci curvature Ric ( v , v ) with a suitable lower bound if and only if it is isometric to the sphere S b n of constant curvature b . In the second result, we show that a complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of R n + 1 of positive Ricci curvature, with shape operator S invariant under its code vector field v and coding function ρ satisfying the static perfect fluid equation is isometric to S b n and the converse also holds. Finally, we show that a complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of R n + 1 has a point p N n with Ric ( v , v ) ( p ) > 0 and has mean curvature H constant along integral curves of code vector v satisfies H 2 c for a positive constant c , and the coding function ρ satisfies Δ ρ = n c ρ if and only if it is isometric to S c n .

MSC 2010: 53C42; 53C45

1 Introduction

In differential geometry, the most studied topic is the geometry of hypersurfaces in Euclidean space. There is a trend of studying biharmonic hypersurfaces and hypersurfaces of finite type in Euclidean space (cf. [14]). Moreover, there is an interesting class of hypersurfaces having two distinct principal curvatures in Euclidean space, and these hypersurfaces are classified in [5,6].

Given an n -dimensional Riemannian manifold ( N n , g ) that is isometrically immersed in Euclidean space R n + 1 , in this article, we observe that each unit constant vector field a on Euclidean space R n + 1 watches the hypersurface ( N n , g ) through two quantities it assigns to the hypersurface ( N n , g ) : one is a vector field v that is tangential component of a called the code vector, and the other is the function ρ that is the normal component of a called the coding function. These two quantities, the code vector v and coding function ρ of the hypersurface ( N n , g ) with respect to the constant unit vector field a on Euclidean space R n + 1 , play an important role in shaping the geometry of the hypersurface, which we wish to explore in this article.

Let ( N n , g ) be an n -dimensional Riemannian manifold isometrically immersed in Euclidean space R n + 1 with unit normal ζ and shape operator S . Throughout this article, we fix a constant unit vector field a on Euclidean space R n + 1 and express its restriction to the hypersurface ( N n , g ) as follows:

(1.1) a = v + ρ ζ , ρ = a , ζ .

As mentioned earlier, we call the vector field v in equation (1.1) as the code vector and ρ as the coding function of the hypersurface. Grouping these all together, we call the sextuple ( N n , g , ζ , S , v , ρ ) a coded hypersurface of Euclidean space R n + 1 with respect to the constant unit vector a .

Consider the sphere ( S b n , g ) of constant curvature b as an embedded hypersurface of R n + 1 given by

S b n = u R n + 1 : u , u = 1 b .

Then the shape operator S and the unit normal ζ of ( S b n , g ) are given by S = b I , and ζ = b φ , where φ : S b n R n + 1 is φ ( u ) = u . The code vector v and the coding function ρ of ( S b n , g ) gives a coded hypersurface ( S b n , g , b φ , b I , v , ρ ) , of the Euclidean space R n + 1 , whose code vector v and coding function ρ satisfy (owing to Gauss-Weingarten formulae):

X v = b ρ X , ρ = b v ,

where X is the directional derivative with respect to the metric g and ρ is the gradient of coding function ρ . The aforementioned equation conveys that for the coded hypersurface ( S b n , g , b φ , b I , v , ρ ) , we have

(1.2) Hess ( ρ ) = b ρ g , Δ ρ = n b ρ ,

where Hess ( ρ ) is the Hessian of the coding function ρ and Δ ρ is its Laplacian. As the Ricci tensor Ric and the scalar curvature τ of ( S b n , g ) are given by R i c = ( n 1 ) b g , τ = n ( n 1 ) b , on employing equation (1.2), we see that the coded hypersurface ( S b n , g , b φ , b I , v , ρ ) satisfies the static perfect fluid equation (SPFE) (cf. [7])

(1.3) n ( ρ Ric-Hess ( ρ ) ) = ( τ ρ Δ ρ ) g .

Observe that on ( S b n , g ) , one has Ric ( v , v ) = ( n 1 ) b v 2 and the mean curvature H = b , and therefore,

(1.4) Ric ( v , v ) = ( n 1 ) H 2 v 2 .

Also, on ( S b n , g ) , by equation (1.2), one has ρ Δ ρ = n b ρ 2 , and by integrating this equation while using equation (1.1), we have

b S b n v 2 = n b S b n ρ 2 .

By integrating equation (1.4) and using the aforementioned equation, with ( S b n , g ) , we obtain

(1.5) S b n Ric ( v , v ) = n ( n 1 ) S b n H 2 ρ 2 .

The aforementioned equation holds for code vector v and the coding function ρ and the mean curvature H of the sphere ( S b n , g ) as hypersurface of Euclidean space R n + 1 . This raises a question: Is equation (1.5) a characteristic property of the sphere ( S b n , g ) ? In other words, is a compact and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) with mean curvature H satisfying equation (1.5) necessarily isometric to ( S b n , g ) ? We answer this question in affirmative and show that a a compact and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 with mean curvature H satisfies

N n Ric ( v , v ) n ( n 1 ) N n H 2 ρ 2 ,

if and only if the mean curvature H is a constant and that ( N n , g , ζ , S , v , ρ ) is isometric to ( S b n , g ) with b = H 2 (Theorem 1).

In other consideration, we observe for the coded hypersurface ( S b n , g , b φ , b I , v , ρ ) , the coding function ρ satisfies the SPFE, that is, equation (1.3). Moreover, the shape operator S = b I is invariant under the code vector v , that is, it satisfies

(1.6) £ v S = 0 ,

where £ v is the Lie derivative with respect to code vector v . One observes that equations (1.3) and (1.6) are characteristics of the coded hypersurface ( S b n , g , b φ , b I , v , ρ ) of the Euclidean space R n + 1 . This raises another question: Is a complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space with coding function ρ satisfying SPFE and shape operator S invariant under the code vector v isometric to a sphere? We show that the answer to aforementioned question is in affirmative provided the coded hypersurface is not minimal, that is, H 0 (Theorem 2).

Next, in this article, we show that a complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) , having a point p N n , where Ric ( v , v ) ( p ) > 0 , the coding function ρ satisfying Δ ρ = n c ρ for a positive constant c , mean curvature H satisfying H 2 c , and H is a constant along integral curves of the code vector v , necessarily implies that ( N n , g , ζ , S , v , ρ ) is isometric to the sphere S c n and the converse also holds (Theorem 3).

2 Preliminaries

Let ( N n , g , ζ , S , v , ρ ) a coded hypersurface of Euclidean space R n + 1 with respect to the constant unit vector a . We denote by X the directional derivative with respect to the vector field X D ( N n ) corresponding to the Levi-Civita connection of the induced metric g on the coded hypersurface ( N n , g , ζ , S , v , ρ ) , where D ( N n ) is the set of all smooth vector fields on N n . Differentiating equation (1.1), while using Gauss and Weingarten formulas, and equating like parts, we obtain

(2.1) X v = ρ S X , ρ = S v , X D ( N n ) ,

where ρ is the gradient of the coding function. The mean curvature function H of ( N n , g , ζ , S , v , ρ ) is given by

(2.2) H = 1 n j g ( S E j , E j ) ,

where { E j } 1 n is a local frame on ( N n , g , ζ , S , v , ρ ) . The curvature tensor R , Ricci tensor Ric, and scalar curvature τ of ( N n , g , ζ , S , v , ρ ) are given by

(2.3) R ( X 1 , X 2 ) X 3 = g ( S X 2 , X 3 ) S X 1 g ( S X 1 , X 3 ) S X 2 , X 1 , X 2 , X 3 D ( N n ) ,

(2.4) Ric ( X 1 , X 2 ) = n H g ( S X 1 , X 2 ) g ( S X 1 , S X 2 ) , X 1 , X 2 D ( N n ) ,

and

(2.5) τ = n 2 H 2 S 2 ,

where

S 2 = j g ( S E j , S E j ) .

The shape operator S of the coded hypersurface ( N n , g , ζ , S , v , ρ ) satisfies the Codazzi equation:

(2.6) ( S ) ( X 1 , X 2 ) = ( S ) ( X 2 , X 1 ) , X 1 , X 2 D ( N n ) ,

where ( S ) ( X 1 , X 2 ) = X 1 S X 2 S ( X 1 X 2 ) . Combining equations (2.2) and (2.6), while using the symmetry of the operator S , it is easy to arrive at

(2.7) n H = j ( S ) ( E j , E j ) .

For a smooth function φ on the coded hypersurface ( N n , g , ζ , S , v , ρ ) , the Hessian operator φ is defined by

(2.8) φ ( X ) = X φ , X D ( N n )

and the Hessian Hess ( φ ) is given by

(2.9) Hess ( φ ) ( X 1 , X 2 ) = g ( φ ( X 1 ) , X 2 ) , X 1 , X 2 D ( N n )

and the Laplacian Δ φ of φ is defined as Δ φ = div ( φ ) , which also satisfies

Δ φ = j g ( φ ( E j ) , E j ) .

For more information on the concepts discussed earlier, we recommend consulting the books [8,9].

3 A coded hypersurface with restricted Ric ( v , v )

Let ( N n , g , ζ , S , v , ρ ) a coded hypersurface of the Euclidean space R n + 1 with respect to the constant unit vector a and mean curvature H . In this section, we show that a proper lower bound on the integral of the Ricci curvature R ( v , v ) gives a characterization of a sphere ( S b n , g ) , as shown in the following result:

Theorem 1

A compact and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 , n > 1 , with mean curvature H satisfies

N n Ric ( v , v ) n ( n 1 ) N n ρ 2 H 2 ,

if and only if H is a constant and ( N n , g , ζ , S , v , ρ ) is isometric to ( S b n , g ) with b = H 2 .

Proof

If ( N n , g , ζ , S , v , ρ ) is a coded hypersurface of Euclidean space R n + 1 , then by equation (2.1), the divergence of the code vector is given by

(3.1) div v = n ρ H .

Again by using equation (2.1), we have

ρ S X ρ H X = X v ρ H X , X D ( N n ) ,

that is,

ρ ( S H I ) ( X ) = X v ρ H X , X D ( N n ) .

As the operator S H I is symmetric, taking a local frame { E j } 1 n and employing aforementioned equation, we confirm

ρ 2 S H I 2 = j g ( E j v ρ H E j , E j v ρ H E j ) = v 2 2 ρ H div ( v ) + n ρ 2 H 2

and plugging equation (3.1) with aforementioned equation, yields

(3.2) ρ 2 S H I 2 = v 2 n ρ 2 H 2 .

We know the following integral formula by Yano (cf. [10])

(3.3) N n v 2 = N n Ric ( v , v ) + 1 2 £ v g 2 ( div v ) 2 .

We compute the Lie derivative £ v g using equation (2.1) to arrive at

( £ v g ) ( X 1 , X 2 ) = 2 ρ g ( S X 1 , X 2 ) , X 1 , X 2 D ( N n ) ,

and it implies

1 2 £ v g 2 = 2 ρ 2 S 2 .

By inserting this value and equation (3.1), in equation (3.3), we reach

(3.4) N n v 2 = N n ( Ric ( v , v ) + 2 ρ 2 S 2 n 2 ρ 2 H 2 ) .

Next, observe that

S H I 2 = j g ( S E j H E j , S E j H E j ) = S 2 + n H 2 2 j g ( S E j , H E j ) ,

that is,

(3.5) S H I 2 = S 2 n H 2 .

The equation (3.4) can be rearranged as follows:

N n v 2 = N n ( Ric ( v , v ) + 2 ρ 2 ( S 2 n H 2 ) + 2 n ρ 2 H 2 n 2 ρ 2 H 2 ) ,

and by using equation (3.5), we have

N n v 2 = N n ( Ric ( v , v ) + 2 ρ 2 S H I 2 + 2 n ρ 2 H 2 n 2 ρ 2 H 2 ) .

Now, by integrate in equation (3.2) and using the aforementioned equation, we obtain

N n ρ 2 S H I 2 = N n n ( n 1 ) ρ 2 H 2 N n Ric ( v , v ) .

By using the condition in the hypothesis, the aforementioned equation, yields

(3.6) ρ 2 S H I 2 = 0 .

If ρ = 0 , then equation (2.1) implies X v = 0 for all X D ( N n ) , which in particular implies

R ( X , v ) v = 0 ,

that is, all the sectional curvatures R ( X , v ; v , X ) = 0 . However, on compact hypersurface ( N n , g , ζ , S , v , ρ ) , there exists a point x N n , where all sectional curvatures are positive. Thus, we must have at this point x N n , v x = 0 , that is, ρ = 0 and v x = 0 with equation (1.1) would imply a x = 0 , and that is contrary to our assumption that a is a constant unit vector in R n + 1 . Hence, ρ 0 , and as N n is simply connected, it is connected, and therefore, equation (3.6) confirms a wonderful conclusion

(3.7) S = H I .

This equation on differentiation takes form

( S ) ( X 1 , X 2 ) = X 1 ( H ) X 2 , X 1 , X 2 D ( N n ) ,

and employing a local frame { E j } 1 n in the aforementioned equation, we arrive at

j ( S ) ( E j , E j ) = H .

Treating this equation with equation (2.7) and using the fact that n > 1 , we are left with the only choice that H is a constant. Also, note that this constant H 0 due to the fact that Euclidean space does not admit a compact minimal hypersurface. Now, by using equation (2.3), we conclude that

R ( X 1 , X 2 ) X 3 = H 2 { g ( X 2 , X 3 ) X 1 g ( X 1 , X 3 ) X 2 } , X 1 , X 2 , X 3 D ( N n ) ,

is the coded hypersurface ( N n , g , ζ , S , v , ρ ) that has constant positive sectional curvature H 2 , and it being simply connected, we see it is isometric to ( S b n , g ) with b = H 2 . The converse follows by equation (1.5).□

4 A coded hypersurface with shape operator invariant under code vector

Let ( N n , g , ζ , S , v , ρ ) be a coded hypersurface of Euclidean space R n + 1 with respect to the constant unit vector a and mean curvature H and scalar curvature τ . We say that the shape operator S is invariant under the code vector v if

d f t S = S d f t

holds, where { f t } is the local flow of v , or equivalently

(4.1) £ v S = 0 ,

where £ v is the Lie differentiation in the direction of v . We also ask that the coding function ρ satisfies SPFE(static perfect fluid equation),

(4.2) n ( ρ Ric Hess ( ρ ) ) = ( τ ρ Δ ρ ) g .

It is interesting to observe that the combination (4.1) and (4.2) for a complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of positive Ricci curvature gives a characterization of the sphere ( S b n , g ) as seen in the following result:

Theorem 2

A complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 , n > 1 , with positive Ricci curvature has the shape operator S invariant under the code vector v and the coding function ρ satisfies SPFE if and only if the mean curvature H is a constant and ( N n , g , ζ , S , v , ρ ) is isometric to ( S b n , g ) with b = H 2 .

Proof

Suppose the coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 has positive Ricci curvature and satisfies equations (4.1) and (4.2), that is, the shape operator S is invariant under v and that the coding function ρ satisfies SPFE. Note that equation (4.1) implies

[ v , S X ] = S [ v , X ] , X D ( N n ) ,

that is,

( S ) ( v , X ) = S X v S ( X v ) , X D ( N n ) .

By utilizing equations (2.1) and (2.6) in the aforementioned equation, we confirm that

(4.3) ( S ) ( v , X ) = ( S ) ( X , v ) = 0 , X D ( N n ) .

Now, from equation (2.1), we have ρ = S v , and we differentiate this equation to conclude

ρ ( X ) = X S v = ( S ) ( X , v ) S ( X v ) , X D ( N n ) .

By using equations (2.1) and (4.3), we obtain

(4.4) ρ ( X ) = ρ S 2 X , X D ( N n ) .

On plugging the aforementioned equation into equations (2.4) and (2.9), we conclude

Hess ( ρ ) ( X 1 , X 2 ) = ρ ( n H g ( S X 1 , X 2 ) Ric ( X 1 , X 2 ) ) , X 1 , X 2 D ( N n ) ,

that is,

( ρ Ric Hess ( ρ ) ) ( X 1 , X 2 ) = ρ n H g ( S X 1 , X 2 ) .

Next, by using equation (4.2) with the aforementioned equation, we have

(4.5) ( τ ρ Δ ρ ) g ( X 1 , X 2 ) = ρ n 2 H g ( S X 1 , X 2 ) , X 1 , X 2 D ( N n ) .

Taking trace in equation (4.4) produces

Δ ρ = ρ S 2 .

By using equation (2.5) with the aforementioned equation, we have

( τ ρ Δ ρ ) = ρ ( n 2 H 2 S 2 ) + ρ S 2 = ρ n 2 H 2 .

By inserting this equation in equation (4.5), we obtain

n 2 ρ H ( g ( S X 1 , X 2 ) H g ( X 1 , X 2 ) ) = 0 , X 1 , X 2 D ( N n ) ,

that is,

(4.6) ρ H ( S X H X ) = 0 , X D ( N n ) .

As N n is simply connected, it is connected, and by connecting N n , we discuss possible outcomes of the aforementioned equation. If ρ = 0 , then equation (2.1) implies S v = 0 , and this will imply by equation (2.4) Ric ( v , v ) = 0 , which is not allowed by the hypothesis. Hence, ρ 0 . If H = 0 , it will make scalar curvature τ 0 by equation (2.5), and again it is not allowed as the Ricci curvatures are positive make τ > 0 . Hence, H 0 , and we are left with the only the following choice:

S = H I .

The rest of the proof follows from the proof of previous result. The converse is trivial as the sphere ( S b n , g ) has positive Ricci curvature satisfies equations (1.3) and (1.6), that is, the shape operator is invariant under code vector and the coding function satisfies SPFE.□

5 A coded hypersurface with coding function eigenvalue of Laplace operator

Let ( N n , g , ζ , S , v , ρ ) be a coded hypersurface of Euclidean space R n + 1 with respect to the constant unit vector a of mean curvature H and scalar curvature τ . In this section, we seek the result of a restriction on the Laplacian of the coding function ρ . As we know the sphere ( S b n , g ) as a coded hypersurface ( S b n , g , b φ , b I , v , ρ ) has coding function ρ satisfying Δ ρ = n b ρ , and this motivates the question: Under what conditions a complete simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of the Euclidean space R n + 1 with coding function ρ satisfying Δ ρ = n b ρ , where b is a positive constant, is isometric to ( S b n , g ) ? We answer this question through the following:

Theorem 3

A complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 , n > 1 , with a point p N n , where Ric ( v , v ) ( p ) > 0 , mean curvature H a constant along the integral curves of the code vector v and the coding function ρ satisfies Δ ρ = n b ρ for a positive constant b H 2 , if and only if, the mean curvature H is a constant and ( N n , g , ζ , S , v , ρ ) is isometric to ( S b n , g ) .

Proof

Suppose ( N n , g , ζ , S , v , ρ ) is a coded hypersurface of the Euclidean space R n + 1 , n > 1 , with mean curvature H a constant along the integral curves of the code vector v , that is,

(5.1) g ( v , H ) = 0 ,

and the coding function ρ satisfies

(5.2) Δ ρ = n b ρ ,

for a positive constant b such that

(5.3) b H 2 .

On differentiating the relation ρ = S v from equation (2.1), we have

ρ ( X ) = ( S ) ( X , v ) S ( ρ S X ) , X D ( N n ) ,

where we used equation (2.1). By employing a local frame { E j } 1 n to take trace in above equation, while using symmetry of S and equation (2.7), we conclude

Δ ρ = n g ( v , H ) ρ S 2 ,

and by plugging the aforementioned equation with equations (5.1) and (5.2), we reach

n b ρ 2 = ρ 2 S 2 .

By rearranging the aforementioned equation, we have

(5.4) ρ 2 ( S 2 n H 2 ) = n ( b H 2 ) ρ 2 .

By subjecting the aforementioned to the inequality (5.3), we arrive at

ρ 2 ( S 2 n H 2 ) 0 .

Note that the Schwarz inequality S 2 n H 2 forces the aforementioned inequality to yield

(5.5) ρ 2 ( S 2 n H 2 ) = 0 .

If ρ = 0 , then equation (2.1) would imply S v = 0 and inserting it in equation (2.4), we obtain Ric ( v , v ) = 0 , which is contrary to the assumption that there is a point p N n , where Ric ( v , v ) ( p ) > 0 . Hence, ρ 0 , and therefore, with ( N n , g , ζ , S , v , ρ ) , equation (5.5) yields

S 2 = n H 2 .

The aforementioned equality in Schwarz inequality S 2 n H 2 holds if and only if,

(5.6) S = H I .

By using n > 1 with aforementioned equation, with a similar argument as in Theorem 1, we conclude that H is a constant. Moreover, by equation (5.4), we see that b = H 2 is a positive constant. Hence, as argued in Theorem 1, ( N n , g , ζ , S , v , ρ ) is isometric to ( S b n , g ) . The converse is trivial.□

6 Conclusions

In Theorem 2, we have studied a complete and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 , n > 1 , with positive Ricci curvature that has the shape operator S invariant under the code vector v and the coding function ρ satisfies SPFE, and obtained a characterization of the sphere ( S b n , g ) . The scope of studying geometry of coded hypersurface ( N n , g , ζ , S , v , ρ ) in Euclidean space R n + 1 is quite modest. For instance, it will be interesting to study the impact of the restrictions on the code vector v , such as v is a conformal vector field or v is a geodesic vector field (cf. [11,12]). Equation (1.1) suggests that in the case, the code vector v of a compact and simply connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 being conformal vector field with suitable further restrictions could lead to a characterization of the sphere ( S b n , g ) . However, in the case the code vector v of a complete and connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 being geodesic vector field (i.e., integral curves of v are geodesics), through equation (2.2), under the assumption that coding function ρ 0 , one concludes coding function ρ is a constant and that S v = 0 . Thus, an interesting question would be to find suitable conditions under, which a complete and connected coded hypersurface ( N n , g , ζ , S , v , ρ ) of Euclidean space R n + 1 with code vector v a geodesic vector field and coding function ρ 0 is R × M n 1 , where M n 1 is a codimension 2 submanifold of R n + 1 (cf. [8]).

Acknowledgements

This work was supported by Researchers Supporting Project number (RSPD2024R1053) King Saud University, Riyadh, Saudi Arabia.

  1. Author contributions: The authors have contributed equally to this work. They 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.

  2. Conflict of interest: The authors state no conflicts of interest.

  3. Data availability statement: All data generated or analyzed during this study are included in this published article.

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Received: 2024-05-06
Revised: 2024-11-20
Accepted: 2024-11-24
Published Online: 2024-12-17

© 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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  12. Some new Hermite-Hadamard-type inequalities for strongly h-convex functions on co-ordinates
  13. Global existence and extinction for a fast diffusion p-Laplace equation with logarithmic nonlinearity and special medium void
  14. Extension of Fejér's inequality to the class of sub-biharmonic functions
  15. On sup- and inf-attaining functionals
  16. Regularization method and a posteriori error estimates for the two membranes problem
  17. Rapid Communication
  18. Note on quasivarieties generated by finite pointed abelian groups
  19. Review Articles
  20. Amitsur's theorem, semicentral idempotents, and additively idempotent semirings
  21. A comprehensive review of the recent numerical methods for solving FPDEs
  22. On an Oberbeck-Boussinesq model relating to the motion of a viscous fluid subject to heating
  23. Pullback and uniform exponential attractors for non-autonomous Oregonator systems
  24. Regular Articles
  25. On certain functional equation related to derivations
  26. The product of a quartic and a sextic number cannot be octic
  27. Combined system of additive functional equations in Banach algebras
  28. Enhanced Young-type inequalities utilizing Kantorovich approach for semidefinite matrices
  29. Local and global solvability for the Boussinesq system in Besov spaces
  30. Construction of 4 x 4 symmetric stochastic matrices with given spectra
  31. A conjecture of Mallows and Sloane with the universal denominator of Hilbert series
  32. The uniqueness of expression for generalized quadratic matrices
  33. On the generalized exponential sums and their fourth power mean
  34. Infinitely many solutions for Schrödinger equations with Hardy potential and Berestycki-Lions conditions
  35. Computing the determinant of a signed graph
  36. Two results on the value distribution of meromorphic functions
  37. Zariski topology on the secondary-like spectrum of a module
  38. On deferred f-statistical convergence for double sequences
  39. About j-Noetherian rings
  40. Strong convergence for weighted sums of (α, β)-mixing random variables and application to simple linear EV regression model
  41. On the distribution of powered numbers
  42. Almost periodic dynamics for a delayed differential neoclassical growth model with discontinuous control strategy
  43. A new distributionally robust reward-risk model for portfolio optimization
  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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