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Connectivity with respect to α-discrete closure operators

  • Josef Šlapal EMAIL logo
Published/Copyright: August 23, 2022

Abstract

We discuss certain closure operators that generalize the Alexandroff topologies. Such a closure operator is defined for every ordinal α > 0 in such a way that the closure of a set A is given by closures of certain α -indexed sequences formed by points of A . It is shown that connectivity with respect to such a closure operator can be viewed as a special type of path connectivity. This makes it possible to apply the operators in solving problems based on employing a convenient connectivity such as problems of digital image processing. One such application is presented providing a digital analogue of the Jordan curve theorem.

MSC 2010: 54A05; 54D05

1 Introduction

One of the basic problems of digital topology is to equip the digital plane Z 2 with a convenient connectivity, i.e., a connectivity behaving analogously to the connectivity in the Euclidean plane R 2 . In particular, such a connectivity is required to satisfy a digital analogue of the Jordan curve theorem because digital Jordan curves represent borders of objects in digital pictures. In this note, we study certain closure operators (more general than the Kuratowski ones) and show that they provide a convenient connectivity for the digital plane.

By a closure operator u on a set X , we mean a map u : exp X exp X (where exp X denotes the power set of X ), which is

  1. grounded (i.e., u = ),

  2. extensive (i.e., A X A u A ), and

  3. monotonic (i.e., A B X u A u B ).

The pair ( X , u ) is then called a closure space.

These closure operators were studied in the pioneering paper [1] by Čech published as early as in 1936.

Recall that a closure operator u on X which is

  1. additive (i.e., u ( A B ) = u A u B whenever A , B X ) and

  2. idempotent (i.e., u u A = u A whenever A X )

is called a Kuratowski closure operator or a topology, and the pair ( X , u ) is called a topological space.

In the literature, closure operators are usually understood to be idempotent and not necessarily grounded, while the ones introduced above are named preclosure operators. But, in this note, we follow the terminology of categorical topology where closure operators in the above sense are commonly used.

Given a cardinal m > 1 , a closure operator u on a set X and the closure space ( X , u ) are called an S m -closure operator and an S m -closure space (briefly, an S m -space), respectively, if the following condition is satisfied:

A X u A = { u B ; B A , card B < m } .

The closure operators usually employed in algebra are the idempotent ones. The so-called algebraic closure operators are then simply the idempotent S 0 -closure operators (cf. [2]).

In the categorical topology, an important role is played by the closure operators on categories studied, e.g., in [3]. They generalize the above closure operators by considering them on subobject lattices in a given category (instead of on power sets, i.e., the subobject lattices in the category S e t ).

In [4], (additive) S 2 -closure operators and S 2 -spaces are called quasi-discrete. S 2 -topologies ( S 2 -topological spaces) are usually called Alexandroff topologies (Alexandroff spaces) [5]. Alexandroff topologies play an important role in general topology and many other branches of mathematics, particularly in general and topological algebra (Scott topologies, monoid actions, commutative algebra) and computer science (Khalimsky topology), cf. [6,7,8, 9,10,11]. Of course, every S 2 -closure operator is additive, and every S α -closure operator is an S β -closure operator whenever α < β . Since any closure operator on a set X is obviously an S α -closure operator for each cardinal α with α > card X , there exists a least cardinal α such that u is an S α -closure operator. Such a cardinal is then an important invariant of the closure operator u . Evidently, if α 0 , then every additive S α -closure operator is an S 2 -closure operator.

We will use some known topological concepts (see, e.g., [12]) naturally extended to closure spaces. Given a closure space ( X , u ) , a subset A X is called closed if u A = A , and open if X A is closed. A closure space ( X , u ) is said to be a subspace of a closure space ( Y , v ) if u A = v A X for each subset A X . We will speak briefly about a subspace X of ( Y , v ) . A closure space ( X , u ) is said to be connected if and X are the only subsets of X to be both closed and open. A subset X Y is connected in a closure space ( Y , v ) if the subspace X of ( Y , v ) is connected. A maximal connected subset of a closure space is called a component of this space. All the basic properties of connected subsets and components in topological spaces are also preserved in closure spaces. In particular, if { A i ; i I } is a family of connected subsets with a non-empty intersection, then i I A i is connected, too.

In the paper, we will work with α -indexed sequences of points of a set X , where α is an ordinal, i.e., with sequences of the form ( x i i < α ) X α . We will write ( x i i α ) instead of ( x i i < α + 1 ) .

2 α -discrete closure operators

In the sequel, α > 0 will be an ordinal.

Definition 2.1

Let ( X , u ) be a closure space. A sequence ( x i i α ) X α + 1 is called a u-connected element if x j u { x i ; i < j } for each j , 0 < j α . The elements x 0 and x α are called the end points of the u -connected element ( x i i α ) .

Definition 2.2

A closure operator u on a set X is called α -discrete if the following condition is fulfilled:

For any A X and any x u A , there exists a u -connected element ( x i i α ) such that ( x i i < α ) A α and x α = x .

Thus, every α -discrete closure operator is an S α -space, where α denotes the least of all cardinals that are greater than α . The 1-discrete closure operators coincide with the S 2 -closure operators so that idempotent 1-discrete closure operators are simply Alexandroff topologies, i.e., topologies with completely additive closures.

Example 2.3

Let u be the closure operator on the set X = { a , b , c } given by u { a } = { a , b } , u { b } = { b } , u { c } = { c } , u { a , b } = u { a , c } = X , and u { b , c } = { b , c } . Then, u is a 2-discrete closure operator on X (which is not 1-discrete). This results from the fact that the sequences ( a , a , a ) , ( b , b , b ) , ( c , c , c ) , ( a , a , b ) , and ( a , b , c ) are u -connected elements and, for every A X and x u A , there exists ( x i i 2 ) { ( a , a , a ) , ( b , b , b ) , ( c , c , c ) , ( a , a , b ) , ( a , b , c ) } such that ( x i i < 2 ) A 2 and x 2 = x .

For a closure operator u on a set X , we denote by u α the closure operator on X given by u α A = { x X ; there is a u -connected element ( x i i α ) such that x = x i 0 for some i 0 , 0 < i 0 α , and x i A for all i < i 0 } .

Proposition 2.4

A closure operator u on a set X is α -discrete if and only if u = u α .

Proof

Let u be a closure operator on X . Let u be α -discrete and let A X be a subset. It is evident that u A u α A . To show the converse inclusion, let x u α A . Then, there is a u -connected element ( x i i α ) such that x = x i 0 for some i 0 , 0 < i 0 α , and x i A for all i < i 0 . Thus, x u { x i ; i < i 0 } u A . Therefore, u = u α .

Conversely, let u = u α . Let A X and x u A . Then, there exists a u -connected element ( x i i α ) such that x = x i 0 for some i 0 , 0 < i 0 α , and x i A for all i < i 0 . Put x i = x i for all i < i 0 , x i = x 0 for all i , i 0 i < α , and x α = x i 0 . Then, ( x i i α ) is a u -connected element such that ( x i i < α ) A α and x α = x . Therefore, u is α -discrete.□

Example 2.5

As usual, we denote by ω the least infinite ordinal. Let u be the closure operator on the set (ordinal) ω + 1 given by u A = { α ; α is an ordinal such that min A α ω } . Let x u A be a point. Then, the points y A with y < x form an increasing sequence ( y i i < α ) , where α ω , y 0 = min A , and x j u { x i ; i < j } for each j , 0 < j < α . Put y i = y i for all i < α and y i = x for all i , α i ω . Then, ( y i i ω ) is a u -connected element such that x = y α and y i A for all i < α . Therefore, u = u ω . By Proposition 2.4, u is an ω -discrete closure operator (which is not α -discrete for any finite ordinal α ).

Proposition 2.6

Let u be an α -discrete closure operator on a set X. Then:

  1. The union of a system of closed subsets of ( X , u ) is a closed subset of ( X , u ) .

  2. u is idempotent if and only if ( X , u ) is an Alexandroff space.

Proof

(1) Let { A j ; j J } be a system of closed subsets of ( X , u ) and let x u j J A j . Then, there exists a u -connected element ( x i i α ) such that x = x α and x i j J A j for all i < α . In particular, we have x 0 j J A j , and so there exists j 0 J such that x 0 A j 0 . Suppose that { x i ; i < α } is not a subset of A j 0 . Then, there is the smallest ordinal i 1 < α such that x i 1 A j 0 . Consequently, 0 < i 1 and x i A j 0 for all i < i 1 . Thus, we have x i 1 u { x i ; i < i 1 } u A j 0 = A j 0 , which is a contradiction. Therefore, { x i ; i < α } A j 0 , and hence, x u { x i ; i < α } u A j 0 j J u A j . We have shown that u j J A j j J u A j . As the converse inclusion is obvious, the proof is complete.

(2) Let u be idempotent, let A X and x u A . Then, there is a u -connected element ( x i i α ) such that ( x i i < α ) A α and x α = x . Thus, we have x j u { x i ; i < j } for all j , 0 < j α , and clearly, x 0 u { x 0 } . Let j be an ordinal, 0 < j α , such that x i u { x 0 } for all i < j . Then, x j u { x i ; i < j } u u { x 0 } = u { x 0 } . Therefore, by transfinite induction, x j u { x 0 } for every j α . Consequently, x = x α u { x 0 } . Hence, u is an Alexandroff topology. The converse implication is obvious.□

Definition 2.7

Let u be an α -discrete closure operator on a set X and x , y X . A finite sequence of u -connected elements ( p j ) j = 1 k = ( ( x i j i α ) ) j = 1 k ( k a positive integer) is said to be an α -path connecting x and y if

  • x is an end point of p 1 with the other end point of p 1 coinciding with an end point of p 2 ,

  • an end point of p j coincides with an end point of p j 1 and the other end point of p j coincides with an end point of p j + 1 for j = 2 , 3 , , k 1 , and

  • y is an end point of p k and the other end point of p k coincides with an end point of p k 1 .

Thus, every u -connected element ( x i i < α ) is an α -path connecting x 0 and x α (and also an α -path connecting x α and x 0 ). Clearly, if ( p j ) j = 1 k is an α -path connecting x and y , then ( p k j + 1 ) j = 1 k is an α -path connecting y and x . It is also evident that any α -path (connecting a pair of points) ( ( x i j i α ) ) j = 1 k is a connected set, namely, the set j = 1 k { x i j ; i α } . If ( p j ) j = 1 k is an α -path connecting x and y and ( q j ) j = 1 l is an α -path connecting y and z , then the α -path ( r j ) j = 1 k + l , where r j = p j whenever 1 j k and r j = q j k whenever k < j k + l is an α -path connecting x and z .

Theorem 2.8

Let u be an α -discrete closure operator on a set X and A X a subset. Then, A is connected in ( X , u ) if and only if any two points of A can be joined by an α -path contained in A.

Proof

If A = , then the statement is trivial. Let A . In ( X , u ) , if any two points of A can be connected by an α -path, then A is clearly connected (because, choosing a point x A , we have y A { P y , P y is an α -path contained in A connecting x and y } = A , i.e., A is the union of connected sets with a non-empty intersection). Conversely, let A be connected and suppose that there are points x , y A that cannot be connected by an α -path contained in A . Let B be the set of all points of A that can be connected with x by an α -path contained in A . Let z u B A be a point. Then, there is a u -connected element ( x i i α ) such that ( x i i < α ) B α and x α = z . Hence, ( x i i α ) is a u -connected element contained in A , thus an α -path connecting the points x 0 B and z A . Since x and x 0 can also be connected by an α -path contained in A , so can x and z . Therefore, z B , i.e., u B A = B . Consequently, B is closed in the subspace A of ( X , u ) . Next, let z u ( A B ) A be a point. Then, there is a u -connected element ( x i i α ) such that ( x i i < α ) ( A B ) α and x α = z . Suppose that z B . Then, x can be connected with z by an α -path contained in A . Further, z can be connected with x 0 by an α -path – the u -connected element ( x i i α ) – contained in A . Consequently, x and x 0 can be connected by an α -path contained in A , which is a contradiction with x 0 B . Thus, z B , i.e., u ( A B ) A = A B implying that A B is closed in the subspace A of ( X , u ) . Hence, A is the union of the non-empty disjoint sets B and A B closed in the subspace A of ( x , u ) . But this is a contradiction because A is connected. Therefore, any two points of A can be connected by an α -path contained in A .□

It is well known [13] that closure operators that are more general than the Kuratowski ones have useful applications in computer science. By Theorem 2.8, connectivity with respect to an α -discrete closure operator is a certain type of path connectivity. This enables us to apply these closure operators in digital image processing because they provide connectivity structures suitable for studying the geometric and topological properties of digital images (cf. [14]). There are two well-known 1-discrete topologies on Z 2 employed in digital image processing, Marcus topology [15] and Khalimsky topology [16]. In [17], a 2-discrete closure operator on Z 2 is used to formulate and prove a digital analogue of the Jordan curve theorem – see the following example.

Example 2.9

Let u be a closure operator on Z 2 and G be a simple undirected graph (without loops) with the vertex set Z 2 . A circuit in G is said to be a simple closed curve in G with respect to u if it is a minimal (with respect to set inclusion of vertex sets) circuit in G that is a connected subset of ( Z 2 , u ) . A simple closed curve in G with respect to u is called a Jordan curve (with respect to u ) if it separates the space ( Z 2 , u ) into exactly two components, i.e., if the subspace Z 2 J of ( Z 2 , u ) has exactly two components.

Let z = ( x , y ) Z 2 be a point. We put

H ( z ) = { ( x + i , y ) ; i { 1 , 0 , 1 } } , V ( z ) = { ( x , y + i ) ; i { 1 , 0 , 1 } } , D ( z ) = { ( x + i , y + i ) ; i { 1 , 0 , 1 } } , D ( z ) = { ( x + i , y i ) ; i { 1 , 0 , 1 } } .

Next, we put

A ( z ) = H ( z ) V ( z ) D ( z ) D ( z ) .

In the literature, the points of H ( z ) V ( z ) and A ( z ) different from z are said to be 4-adjacent and 8-adjacent to z , respectively. Here, for all z Z 2 , each of the sets H ( z ) , V ( z ) , D ( z ) , and D ( z ) will be called a basic segment. Note that basic segments may be regarded as digital (three-element) line segments (where H ( z ) is oriented horizontally, V ( z ) is oriented vertically, and D ( z ) and D ( z ) are oriented diagonally in Z 2 ).

For every point z Z 2 , we put

w { z } = H ( z ) if z = ( 4 k + 2 , y ) where k Z and y 4 l + 2 for every l Z , V ( z ) if z = ( x , 4 l + 2 ) where l Z and x 4 k + 2 for every k Z , A ( z ) if z = ( 4 k + 2 , 4 l + 2 ) , k , l Z , { z } otherwise

and, for every two-element subset { z , t } Z 2 , we put w { z , t } = w { z } w { t } z , t where

z , t = H ( z ) if z = ( 4 k + 2 + i , l ) and t = ( 4 k + 2 , l ) , k , l Z , i { 1 , 1 } , V ( z ) if z = ( k , 4 l + 2 + i ) and t = ( k , 4 l + 2 ) , k , l Z , i { 1 , 1 } , D ( z ) if z = ( 4 k + 2 + i , 4 l + 2 + i ) and t = ( 4 k + 2 , 4 l + 2 ) , k , l Z , i { 1 , 1 } , D ( z ) if z = ( 4 k + 2 + i , 4 l + 2 i ) and t = ( 4 k + 2 , 4 l + 2 ) , k , l Z , i { 1 , 1 } , { z , t } otherwise.

It was pointed out by one of the referees that z , t = { z , t , z + 2 ( t z ) } if one of the following three conditions is satisfied

  1. z = ( 4 k + 2 , 4 l + 2 ) and t w ( z ) = A ( z ) ,

  2. z = ( 4 k + 2 , 4 l ) and t w ( z ) = H ( z ) ,

  3. z = ( 4 k , 4 l + 2 ) and t w ( z ) = V ( z )

or one of the three conditions obtained by interchanging z and t in (1)–(3) is satisfied while z , t = { z , t } otherwise.

Now, putting w A = { w B ; B A , card B < 3 } for every subset A X (card A > 2 ), we obtain an S 3 -closure operator on Z 2 . The closure operator w is demonstrated in Figure 1. For any point z Z 2 , a point u Z 2 , u z , belongs to w { z } if and only if there is an edge from z to u in the directed graph demonstrated in the left part of Figure 1. If { z , t } Z 2 is a two-element subset, then a point u Z 2 with u w { z } w { t } belongs to w { z , t } if and only if, in the directed graph demonstrated in the right part of Figure 1, z and t are the end points of a dotted line segment containing no other point of Z 2 (the dotted line segments are not edges of the graph), there is an edge from z or t to u , and the points z , t , and u lie on a line (with z or t lying between the other two points so that the set { z , t , u } is a basic segment with t w { z } or z w { t } – cf, the directed graph in the left part of the figure).

Clearly, any sequence ( ( x i , y i ) i 2 ) ( Z 2 ) 3 satisfying one of the following nine conditions is a w -connected element:

  1. x 0 = x 1 = x 2 and y 0 = y 1 = y 2 ,

  2. x 0 = x 1 = x 2 and there is k Z such that y i = 4 k + i for all i < 3 ,

  3. x 0 = x 1 = x 2 and there is k Z such that y i = 4 k i for all i < 3 ,

  4. y 0 = y 1 = y 2 and there is k Z such that x i = 4 k + i for all i < 3 ,

  5. y 0 = y 1 = y 2 and there is k Z such that x i = 4 k i for all i < 3 ,

  6. there is k Z such that x i = 4 k + i for all i < 3 and there is l Z such that y i = 4 l + i for all i < 3 ,

  7. there is k Z such that x i = 4 k + i for all i < 3 and there is l Z such that y i = 4 l i for all i < 3 ,

  8. there is k Z such that x i = 4 k i for all i < 3 and there is l Z such that y i = 4 l + i for all i < 3 , and

  9. there is k Z such that x i = 4 k i for all i < 3 and there is l Z such that y i = 4 l i for all i < 3 .

It may easily be seen that, for any subset A Z 2 , z w A if and only if there exists a sequence ( ( x i , y i ) i 2 ) ( Z 2 ) 3 satisfying one of the above nine conditions such that z = ( x i 0 , y i 0 ) for some i 0 , 0 < i 0 2 , and ( x i , y i ) A for all i < 2 . Thus, w = w 2 so that w is a 2-discrete closure operator on Z 2 . The w -connected elements ( ( x i , y i ) i 2 ) ( Z 2 ) 3 satisfying (an arbitrary single) one of the conditions (2)–(9) are demonstrated in Figure 2 by directed line segments with the starting point ( x 0 , y 0 ) and the end point ( x 2 , y 2 ) (so that ( x 1 , y 1 ) is the midpoint of the segment).

We denote by H the graph with the vertex set Z 2 such that, for all z , t Z 2 , z and t are adjacent in H if and only if they are different and one of the following two conditions is satisfied:

  1. z w { t } or t w { z } ,

  2. there is a point u Z 2 , z u t , such that either z w { u } and t w { u , z } or t w { u } and z w { u , t } .

A graphical representation of (a section of) the graph H is given by Figure 2 when forgetting all edge directions.

The following results may be proved by applying Theorem 2.8 (in [17)], they were obtained by the help of Lemma 3.3 proved there, which is nothing but a straightforward consequence of Theorem 2.8):

  1. The closure space ( Z 2 , w ) is connected.

  2. Every circuit C in the graph H that turns only at some of the points ( 4 k , 4 l ) , k , l Z , is a Jordan curve in H with respect to the closure operator w and has the property that its union with any of the two components of the subspace Z 2 C of ( Z 2 , w ) is connected.

Jordan curves in the graph H with respect to the closure operator w will be briefly called Jordan curves in the closure space ( Z 2 , w ) . The possible turning points of the Jordan curves in ( Z 2 , w ) determined in statement (2) are the points ( 4 k , 4 l ) , k , l Z , where the curves may turn at the acute angle π 4 . This is an advantage over the Jordan curves with respect to the Khalimsky topology because they may never turn at the acute angle π 4 – cf. [16].

Figure 1 
               Closure operator 
                     
                        
                        
                           w
                        
                        w
                     
                  .
Figure 1

Closure operator w .

Figure 2 
               
                  
                     
                        
                        
                           w
                        
                        w
                     
                  -connected elements satisfying (an arbitrary but) one of the conditions (2)–(9).
Figure 2

w -connected elements satisfying (an arbitrary but) one of the conditions (2)–(9).

3 Conclusion

We have introduced, for every ordinal α > 0 , closure operators that generalize the quasi-discrete closure operators [4]. These closure operators, called α -discrete, are studied. In particular, it is shown that the connectivity with respect to α -discrete closure operators is a certain type of path connectivity. This enables us to apply the operators to solving various problems of a discrete nature based on connectivity. One such application in digital topology is discussed. We have shown that there is a 2-discrete closure operator on the digital plane Z 2 allowing for a digital analogue of the Jordan curve theorem, thus providing a convenient structure on Z 2 for the study of digital images.

Acknowledgments

The author thanks the referees for their helpful comments.

  1. Funding information: This research was supported by the Brno University of Technology from the Specific Reasearch Project no. FSI-S-20-6187.

  2. Author contributions: The author have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The author states no conflict of interest.

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

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Received: 2021-12-16
Revised: 2022-04-11
Accepted: 2022-04-28
Published Online: 2022-08-23

© 2022 Josef Šlapal, published by De Gruyter

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

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  34. Bifurcation and chaos in a discrete predator-prey system of Leslie type with Michaelis-Menten prey harvesting
  35. A posteriori error estimates of characteristic mixed finite elements for convection-diffusion control problems
  36. Dynamical analysis of a Lotka Volterra commensalism model with additive Allee effect
  37. An efficient finite element method based on dimension reduction scheme for a fourth-order Steklov eigenvalue problem
  38. Connectivity with respect to α-discrete closure operators
  39. Khasminskii-type theorem for a class of stochastic functional differential equations
  40. On some new Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in (p, q)-calculus with applications
  41. New properties for the Ramanujan R-function
  42. Shooting method in the application of boundary value problems for differential equations with sign-changing weight function
  43. Ground state solution for some new Kirchhoff-type equations with Hartree-type nonlinearities and critical or supercritical growth
  44. Existence and uniqueness of solutions for the stochastic Volterra-Levin equation with variable delays
  45. Ambrosetti-Prodi-type results for a class of difference equations with nonlinearities indefinite in sign
  46. Research of cooperation strategy of government-enterprise digital transformation based on differential game
  47. Malmquist-type theorems on some complex differential-difference equations
  48. Disjoint diskcyclicity of weighted shifts
  49. Construction of special soliton solutions to the stochastic Riccati equation
  50. Remarks on the generalized interpolative contractions and some fixed-point theorems with application
  51. Analysis of a deteriorating system with delayed repair and unreliable repair equipment
  52. On the critical fractional Schrödinger-Kirchhoff-Poisson equations with electromagnetic fields
  53. The exact solutions of generalized Davey-Stewartson equations with arbitrary power nonlinearities using the dynamical system and the first integral methods
  54. Regularity of models associated with Markov jump processes
  55. Multiplicity solutions for a class of p-Laplacian fractional differential equations via variational methods
  56. Minimal period problem for second-order Hamiltonian systems with asymptotically linear nonlinearities
  57. Convergence rate of the modified Levenberg-Marquardt method under Hölderian local error bound
  58. Non-binary quantum codes from constacyclic codes over 𝔽q[u1, u2,…,uk]/⟨ui3 = ui, uiuj = ujui
  59. On the general position number of two classes of graphs
  60. A posteriori regularization method for the two-dimensional inverse heat conduction problem
  61. Orbital stability and Zhukovskiǐ quasi-stability in impulsive dynamical systems
  62. Approximations related to the complete p-elliptic integrals
  63. A note on commutators of strongly singular Calderón-Zygmund operators
  64. Generalized Munn rings
  65. Double domination in maximal outerplanar graphs
  66. Existence and uniqueness of solutions to the norm minimum problem on digraphs
  67. On the p-integrable trajectories of the nonlinear control system described by the Urysohn-type integral equation
  68. Robust estimation for varying coefficient partially functional linear regression models based on exponential squared loss function
  69. Hessian equations of Krylov type on compact Hermitian manifolds
  70. Class fields generated by coordinates of elliptic curves
  71. The lattice of (2, 1)-congruences on a left restriction semigroup
  72. A numerical solution of problem for essentially loaded differential equations with an integro-multipoint condition
  73. On stochastic accelerated gradient with convergence rate
  74. Displacement structure of the DMP inverse
  75. Dependence of eigenvalues of Sturm-Liouville problems on time scales with eigenparameter-dependent boundary conditions
  76. Existence of positive solutions of discrete third-order three-point BVP with sign-changing Green's function
  77. Some new fixed point theorems for nonexpansive-type mappings in geodesic spaces
  78. Generalized 4-connectivity of hierarchical star networks
  79. Spectra and reticulation of semihoops
  80. Stein-Weiss inequality for local mixed radial-angular Morrey spaces
  81. Eigenvalues of transition weight matrix for a family of weighted networks
  82. A modified Tikhonov regularization for unknown source in space fractional diffusion equation
  83. Modular forms of half-integral weight on Γ0(4) with few nonvanishing coefficients modulo
  84. Some estimates for commutators of bilinear pseudo-differential operators
  85. Extension of isometries in real Hilbert spaces
  86. Existence of positive periodic solutions for first-order nonlinear differential equations with multiple time-varying delays
  87. B-Fredholm elements in primitive C*-algebras
  88. Unique solvability for an inverse problem of a nonlinear parabolic PDE with nonlocal integral overdetermination condition
  89. An algebraic semigroup method for discovering maximal frequent itemsets
  90. Class-preserving Coleman automorphisms of some classes of finite groups
  91. Exponential stability of traveling waves for a nonlocal dispersal SIR model with delay
  92. Existence and multiplicity of solutions for second-order Dirichlet problems with nonlinear impulses
  93. The transitivity of primary conjugacy in regular ω-semigroups
  94. Stability estimation of some Markov controlled processes
  95. On nonnil-coherent modules and nonnil-Noetherian modules
  96. N-Tuples of weighted noncommutative Orlicz space and some geometrical properties
  97. The dimension-free estimate for the truncated maximal operator
  98. A human error risk priority number calculation methodology using fuzzy and TOPSIS grey
  99. Compact mappings and s-mappings at subsets
  100. The structural properties of the Gompertz-two-parameter-Lindley distribution and associated inference
  101. A monotone iteration for a nonlinear Euler-Bernoulli beam equation with indefinite weight and Neumann boundary conditions
  102. Delta waves of the isentropic relativistic Euler system coupled with an advection equation for Chaplygin gas
  103. Multiplicity and minimality of periodic solutions to fourth-order super-quadratic difference systems
  104. On the reciprocal sum of the fourth power of Fibonacci numbers
  105. Averaging principle for two-time-scale stochastic differential equations with correlated noise
  106. Phragmén-Lindelöf alternative results and structural stability for Brinkman fluid in porous media in a semi-infinite cylinder
  107. Study on r-truncated degenerate Stirling numbers of the second kind
  108. On 7-valent symmetric graphs of order 2pq and 11-valent symmetric graphs of order 4pq
  109. Some new characterizations of finite p-nilpotent groups
  110. A Billingsley type theorem for Bowen topological entropy of nonautonomous dynamical systems
  111. F4 and PSp (8, ℂ)-Higgs pairs understood as fixed points of the moduli space of E6-Higgs bundles over a compact Riemann surface
  112. On modules related to McCoy modules
  113. On generalized extragradient implicit method for systems of variational inequalities with constraints of variational inclusion and fixed point problems
  114. Solvability for a nonlocal dispersal model governed by time and space integrals
  115. Finite groups whose maximal subgroups of even order are MSN-groups
  116. Symmetric results of a Hénon-type elliptic system with coupled linear part
  117. On the connection between Sp-almost periodic functions defined on time scales and ℝ
  118. On a class of Harada rings
  119. On regular subgroup functors of finite groups
  120. Fast iterative solutions of Riccati and Lyapunov equations
  121. Weak measure expansivity of C2 dynamics
  122. Admissible congruences on type B semigroups
  123. Generalized fractional Hermite-Hadamard type inclusions for co-ordinated convex interval-valued functions
  124. Inverse eigenvalue problems for rank one perturbations of the Sturm-Liouville operator
  125. Data transmission mechanism of vehicle networking based on fuzzy comprehensive evaluation
  126. Dual uniformities in function spaces over uniform continuity
  127. Review Article
  128. On Hahn-Banach theorem and some of its applications
  129. Rapid Communication
  130. Discussion of foundation of mathematics and quantum theory
  131. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part II)
  132. A study of minimax shrinkage estimators dominating the James-Stein estimator under the balanced loss function
  133. Representations by degenerate Daehee polynomials
  134. Multilevel MC method for weak approximation of stochastic differential equation with the exact coupling scheme
  135. Multiple periodic solutions for discrete boundary value problem involving the mean curvature operator
  136. Special Issue on Evolution Equations, Theory and Applications (Part II)
  137. Coupled measure of noncompactness and functional integral equations
  138. Existence results for neutral evolution equations with nonlocal conditions and delay via fractional operator
  139. Global weak solution of 3D-NSE with exponential damping
  140. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  141. Ground state solutions of nonlinear Schrödinger equations involving the fractional p-Laplacian and potential wells
  142. A class of p1(x, ⋅) & p2(x, ⋅)-fractional Kirchhoff-type problem with variable s(x, ⋅)-order and without the Ambrosetti-Rabinowitz condition in ℝN
  143. Jensen-type inequalities for m-convex functions
  144. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part III)
  145. The influence of the noise on the exact solutions of a Kuramoto-Sivashinsky equation
  146. Basic inequalities for statistical submanifolds in Golden-like statistical manifolds
  147. Global existence and blow up of the solution for nonlinear Klein-Gordon equation with variable coefficient nonlinear source term
  148. Hopf bifurcation and Turing instability in a diffusive predator-prey model with hunting cooperation
  149. Efficient fixed-point iteration for generalized nonexpansive mappings and its stability in Banach spaces
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