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On the inverse Collatz-Sinogowitz irregularity problem

  • Abdullah Alazemi , Milica Anđelić EMAIL logo and Darko Dimitrov
Published/Copyright: May 16, 2023

Abstract

The Collatz-Sinogowitz irregularity index is the oldest known numerical measure of graph irregularity. For a simple and connected graph G of order n and size m , it is defined as CS ( G ) = λ 1 2 m / n , where λ 1 is the largest eigenvalue of the adjacency matrix of G , and 2 m / n is the average vertex degree of G . Here, the Collatz-Sinogowitz inverse irregularity problem is studied. For every integer i 0 , it is shown that there exists a graph G such that CS ( G ) = i . Also, for every interval I i = ( i , i + 1 ) , it is shown that there are infinitely many graphs whose Collatz-Sinogowitz irregularity lies in I i .

MSC 2010: 05C50

1 Introduction

Let G be a simple graph, with vertex set V ( G ) = { v 1 , v 2 , , v n } and edge set E ( G ) = { e 1 , e 2 , , e m } . The quantities n and m are called the order and size of G , respectively. The vertex degree d G ( u ) is the cardinality of the set of edges incident with u . A graph is regular if all its vertices have equal vertex degrees; contrarily, it is irregular. How much irregular a given graph is could be of high importance in solving many problems. It seems that the oldest numerical measure of graph irregularity was proposed by Collatz and Sinogowitz [1]. It is defined as:

CS ( G ) = λ 1 2 m n ,

where λ 1 denotes the largest eigenvalue of the adjacency matrix of G , commonly called the spectral radius of G . Note that 2 m / n is the average vertex degree of a graph G . It is well known that if a graph is regular, then λ 1 = 2 m / n and λ 1 > 2 m / n otherwise [1].

A more direct measure of irregularity was presented by Bell [2], who suggested that the variance Var ( G ) of the vertex degrees

Var ( G ) = 1 n v V ( G ) d G ( v ) 2 1 n v V ( G ) d G ( v ) 2

serves for this purpose.

Another well-established irregularity metric is the Albertson irregularity [3], defined as:

irr ( G ) = u v E ( G ) d G ( u ) d G ( v ) .

The quantity d G ( u ) d G ( v ) in the aforementioned formula is called the imbalance of an edge e = u v . In order to evade the calculation of the absolute value, one inherently came up with the so-called σ -irregularity introduced in [4], which is defined as:

σ ( G ) = u v E ( G ) ( d G ( u ) d G ( v ) ) 2 .

This irregularity measure not necessarily is the same for graphs with the same degree sequence. Recently in [5], the following variant of σ -irregularity was introduced:

σ t ( G ) = 1 2 ( u , v ) V 2 ( G ) ( d G ( u ) d G ( v ) ) 2 ,

where V 2 ( G ) is the Cartesian product of V ( G ) with itself. It was named the total σ -irregularity and has the same value for all graphs with same degree sequence.

Before we proceed with the results on the inverse problem of Collatz-Sinogowitz irregularity, an additional necessary notation will be introduced. If the subgraph is obtained by removing at least one vertex or edge from the whole graph, then it is called a proper subgraph. A connected graph with equal number of vertices and edges is called a unicyclic graph. A graph G , with a vertex u labeled as root, is denoted by ( G , u ) . The coalescence ( G , u ) ( H , v ) of two disjoint rooted graphs ( G , u ) and ( H , v ) is a graph obtained after identifying u and v . The eigenvalues λ 1 λ 2 λ n of ( 0 , 1 ) -adjacency matrix A of a simple graph G comprise its spectrum, i.e., they are the roots of its characteristic polynomial ϕ ( G , λ ) = det ( λ I A ) (or simply of ϕ G ( λ ) ).

Obtaining graphs with a previously determined value(s) of particular graph invariant(s) (known as an inverse problem regarding the considered graph invariant) could be very purposive and helpful for solving theoretical and practical problems. For example, generating chemical structure(s), which have the desired value of a given invariant, could significantly help in the research and production of chemical compounds with prescribed properties. For the Albertson irregularity, the Bell irregularity, the σ -irregularity, the σ t -irregularity, and the total irregularity, some initial results with respect to the inverse problems can be found in [4,5,6].

In the sequel, we investigate the Collatz-Sinogowitz inverse irregularity problem.

2 The Collatz-Sinogowitz inverse irregularity problem

Here, we consider two variants of the inverse problem. First, we want to find a graph G , if there exists any, such that CS ( G ) = k , k N . Second, we consider the real values of the Collatz-Sinogowitz index. Namely, we ask if for each interval I i = ( i , i + 1 ) , i = 1 , 2 , there are infinitely many graphs whose values of Collatz-Sinogowitz irregularity lie in I i . We present solutions to both problems.

The following results will be used later in this section.

Theorem 2.1

[7] Let H be a proper subgraph of a connected graph G. Then,

λ 1 ( H ) < λ 1 ( G ) .

Theorem 2.2

[8] Let ( G , u ) ( H , v ) be the coalescence of two connected rooted graphs ( G , u ) and ( H , v ) . Then,

λ 1 ( ( G , u ) ( H , v ) ) λ 1 ( G , u ) 2 + λ 1 ( H , v ) 2 .

The equality holds if and only if ( G , u ) ( H , v ) is a star.

Now, we present solutions to both variants of the inverse problem with respect to the Collatz-Sinogowitz irregularity. First, we find solutions within the class of unicyclic graphs. Later, we investigate the starlike graphs and the complete bipartite graphs.

2.1 Unicyclic graphs

Theorem 2.3

For every non-negative integer i,

  1. there exists a unicyclic graph whose Collatz-Sinogowitz irregularity equals i;

  2. there are infinitely many unicyclic graphs whose Collatz-Sinogowitz irregularities lie in the interval ( i , i + 1 ) .

Proof

(i) For i = 0 , any cycle on n vertices, n 3 , fulfills the statement of the proposition. For i 1 , consider the unicyclic graph G depicted in Figure 1.

It enables the following equitable partition D : U 1 U 2 U 3 , where

  • U 1 = { u V ( G ) : d ( u ) = 1 } ,

  • U 2 = { u V ( G ) : d ( u ) = k + 2 } ,

  • U 3 = { u V ( G ) : d ( u ) = 2 } .

The corresponding quotient matrix is of the form:

D = 0 1 0 k 1 1 0 2 0 .

It is well known that the largest eigenvalue of a graph is also an eigenvalue of any quotient matrix. (For this and other results on equitable partitions the reader is referred to [7].) Therefore, λ 1 is the largest root of

ϕ D ( λ ) = λ 3 λ 2 ( k + 2 ) λ = λ ( λ 2 λ ( k + 2 ) ) ,

i.e., λ 1 = ( 1 + 9 + 4 k ) / 2 . We first observe that λ 1 is an integer if and only if 9 + 4 k is an odd integer, i.e., if and only if 9 + 4 k = ( 2 i + 3 ) 2 , i = 1 , 2 , . Then, it follows that k = i 2 + 3 i .

Observe that in such a way, the integer values of λ 1 , larger than 2, can be obtained.

For an illustration, in Table 1, the first smallest values of the parameters i , k , λ 1 , CS ( G ) are given. Recall that the average degree of any unicyclic graph is 2.

(ii) Consider the graph depicted in Figure 2. It is the coalescence of the graph G from Figure 1 and the path graph P n , n 1 . We assume that G is rooted at one end vertex, denoted by v , and P n is rooted at one end vertex, denoted by w . From Theorem 2.1, we have that

λ 1 ( G , v ) < λ 1 ( ( G , v ) ( P n , w ) ) ,

and by Theorem 2.2, we have

λ 1 ( ( G , v ) ( P n , w ) ) λ 1 ( G ) 2 + λ 1 ( P n ) 2 .

We consider the graph G with λ 1 ( G ) = i , i 3 (i.e., CS ( G ) = i 2 ). Also, by [9], λ 1 ( P n ) < 2 . Thus, we have that

i < λ 1 ( ( G , v ) ( P n , w ) ) λ 1 ( G ) 2 + λ 1 ( P n ) 2 i 2 + 4 < i + 1 ,

for i 2 . Therefore, it can be deduced that the spectral radius of ( G , v ) ( P n , w ) lies in the interval ( i , i + 1 ) , i 3 , for any length n of P n . Consequently, CS ( ( G , v ) ( P n , w ) ) lies in the interval ( i 2 , i 1 ) , i 3 .

It remains to prove that there are infinitely many unicyclic graphs whose CS index lies in the interval ( 0 , 1 ) . Here, we consider the coalescence of a cycle of an arbitrary order k 3 and a path of order n 2 , ( C k , v ) ( P n , w ) . In this case,

2 < λ 1 ( ( C k , v ) ( P n , w ) ) λ 1 ( C k ) 2 + λ 1 ( P n ) 2 < 4 + 4 < 3 .

Thus, CS ( ( C k , v ) ( P n , w ) ) ( 0 , 1 ) , for any k 3 and any n 2 .

This completes the proof.□

Figure 1 
                  Unicyclic graph, which with certain values of the parameter 
                        
                           
                           
                              k
                           
                           k
                        
                      may have an arbitrary non-negative integer value of Collatz-Sinogowitz irregularity.
Figure 1

Unicyclic graph, which with certain values of the parameter k may have an arbitrary non-negative integer value of Collatz-Sinogowitz irregularity.

Figure 2 
                  The coalescence of the graph 
                        
                           
                           
                              G
                           
                           G
                        
                      from Figure 1 and the path graph 
                        
                           
                           
                              
                                 
                                    P
                                 
                                 
                                    n
                                 
                              
                           
                           {P}_{n}
                        
                     , 
                        
                           
                           
                              n
                              ≥
                              1
                           
                           n\ge 1
                        
                     .
Figure 2

The coalescence of the graph G from Figure 1 and the path graph P n , n 1 .

Table 1

Values of the parameters i , k , λ 1 , CS ( G )

i 1 2 3 4 5 6 7 8 9 10
k 4 10 18 28 40 54 70 88 108 130
λ 1 3 4 5 6 7 8 9 10 11 12
CS ( G ) 1 2 3 4 5 6 7 8 9 10

Remark 2.1

There are unicyclic graphs, different from those considered in Theorem 2.3, whose Collatz-Sinogowitz irregularity is an integer. As examples, consider the graphs depicted in Figure 3. These graphs also enable equitable partitions, and their largest eigenvalues are the roots of the following polynomials.

  • G 1 : λ 4 ( k + 3 ) λ 2 2 λ + k . The remaining eigenvalues are 0 with multiplicity k 1 and 1 with multiplicity 1, due to k vertices with the same neighborhoods and 2 vertices with the same closed neighborhood. If the number of pendant edges is 6, then λ 1 ( G 1 ) = 3 and CS ( G 1 ) = 1 .

  • G 2 : λ ( λ 4 ( k + + 3 ) λ 2 2 λ + k + k + ) . The remaining eigenvalue is 0 with the multiplicity k + 2 , assuming that the numbers of pendant edges are k and , respectively. For k = 6 and = 22 , λ 1 ( G 2 ) = 5 and CS ( G 2 ) = 3 .

Also, there exist unicyclic graphs with non-negative integer values of their Collatz-Sinogowitz irregularity and the length of the cycle larger than 3.

Figure 3 
                  Unicyclic graphs, which are not isomorphic to those in Figure 1, but have non-negative integer values of their Collatz-Sinogowitz irregularity. It holds that 
                        
                           
                           
                              
                                 
                                    λ
                                 
                                 
                                    1
                                 
                              
                              
                                 (
                                 
                                    
                                       
                                          G
                                       
                                       
                                          1
                                       
                                    
                                 
                                 )
                              
                              =
                              3
                           
                           {\lambda }_{1}\left({G}_{1})=3
                        
                      (
                        
                           
                           
                              
                              CS
                              
                              
                                 (
                                 
                                    
                                       
                                          G
                                       
                                       
                                          1
                                       
                                    
                                 
                                 )
                              
                              =
                              1
                           
                           \hspace{0.1em}\text{CS}\hspace{0.1em}\left({G}_{1})=1
                        
                     ) and 
                        
                           
                           
                              
                                 
                                    λ
                                 
                                 
                                    1
                                 
                              
                              
                                 (
                                 
                                    
                                       
                                          G
                                       
                                       
                                          2
                                       
                                    
                                 
                                 )
                              
                              =
                              5
                           
                           {\lambda }_{1}\left({G}_{2})=5
                        
                      (
                        
                           
                           
                              
                              CS
                              
                              
                                 (
                                 
                                    
                                       
                                          G
                                       
                                       
                                          2
                                       
                                    
                                 
                                 )
                              
                              =
                              3
                           
                           \hspace{0.1em}\text{CS}\hspace{0.1em}\left({G}_{2})=3
                        
                     ).
Figure 3

Unicyclic graphs, which are not isomorphic to those in Figure 1, but have non-negative integer values of their Collatz-Sinogowitz irregularity. It holds that λ 1 ( G 1 ) = 3 ( CS ( G 1 ) = 1 ) and λ 1 ( G 2 ) = 5 ( CS ( G 2 ) = 3 ).

Proposition 2.1

Let i be a positive integer. Then, there is a unicyclic graph, whose Collatz-Sinogowitz irregularity is i and the length of its cycle is larger than 3.

Proof

In [10], one can find that the unicyclic graphs U C ( k , , k ) of arbitrary girth such that to each vertex of the cycle k , pendant edges are attached, have the largest eigenvalue equal to k + 1 + 1 , no matter what the length of the cycle is. Hence,

CS ( U C ( k , , k ) ) = k + 1 1 .

By taking k = ( i + 1 ) 2 1 , i 1 , we obtain that CS ( U C ( i 2 + 2 i , , i 2 + 2 i ) ) = i , independently of the graph’s girth.□

By applying the same construction as in the proof of Theorem 2.3(ii), i.e., a coalescence of a graph G with an integer value of the Collatz-Sinogowitz irregularity and an arbitrarily long path, an infinite number of graphs with the Collatz-Sinogowitz irregularity within a given interval can be obtained. Alternatively, instead of using a coalescence of G and an arbitrarily long path, it is to expect that one can obtain the desired results by subdividing arbitrarily times an edge of a cycle of G .

Next, we extend our results in the class of bipartite graphs.

2.2 Bipartite graphs

In the class of bipartite graphs, we investigate the inverse Collatz-Sinogowitz irregularity problem for two subclasses, the starlike trees and complete bipartite graphs.

2.2.1 Starlikes trees

A tree that has exactly one vertex of degree at least three is called starlike tree. For a starlike tree, denoted as S ( n 1 , n 2 , , n k ) , with a vertex v of degree k 3 , it holds that

S ( n 1 , n 2 , , n k ) v = P n 1 P n 2 P n k ,

where P n i , i = 1 , , k , is the path on n i vertices. Up to isomorphism, the starlike tree is uniquely determined by parameters n 1 , n 2 , , n k . In 2001, Lepović and Gutman presented a sharp lower bound and a tight upper bound on the spectral radius of the starlike trees.

Theorem 2.4

[11] Let λ 1 be the spectral radius of the starlike tree S ( n 1 , n 2 , , n k ) . Then for any positive integers, n 1 n 2 n k 1 , k λ 1 ( S ( n 1 , n 2 , , n k ) ) < k / k 1 .

Using the aforementioned result, we are able to prove the following result for starlike graphs.

Theorem 2.5

For every non-negative integer i, there are infinitely many starlike trees whose Collatz-Sinogowitz irregularity lies in the interval ( i , i + 1 ) .

Proof

Consider an arbitrary starlike graph with k 4 branches, S ( n 1 , n 2 , , n k ) . By Theorem 2.4, it holds that k λ 1 ( S ( n 1 , n 2 , , n k ) ) < k / k 1 . Since k 4 , the starlike tree must have at least five vertices. Therefore, for the average degree of S ( n 1 , n 2 , , n k ) , we have that 1.6 d ¯ < 2 . Consequently, it follows that k 2 < CS ( S ( n 1 , n 2 , , n k ) ) < k / k 1 1.6 . Now, assume that k = q 2 , where q is an integer greater than 1. Under these assumptions, k / k 1 1.6 < q 1 holds, and hence, it can be deduced that q 2 < CS ( S ( n 1 , n 2 , , n k ) ) < q 1 . By replacing q 2 with i , we obtain that i < CS ( S ( n 1 , n 2 , , n k ) ) < i + 1 , where i is a non-negative integer. The last relation is satisfied for any starlike tree with k arbitrary long branches ( k = ( i + 2 ) 2 , i = 0 , 1 , ).□

In the following proposition, we show that the intervals in Theorem 2.5 must be open.

Proposition 2.2

The Collatz-Sinogowitz irregularity of a starlike graph cannot be an integer.

Proof

The largest eigenvalue λ 1 of a starlike tree T is a root of its characteristic polynomial, which is a monic polynomial with integer coefficients. Therefore, if λ 1 Q , then λ 1 N . Otherwise, λ 1 R \ Q . Hence,

  1. If λ 1 N , then CS ( T ) = λ 1 2 + 2 n Z .

  2. If λ 1 R \ Q , then CS ( T ) = λ 1 2 + 2 n R \ Z , and therefore, it is not an integer.□

The argumentation in the proof of Proposition 2.2 leads to the following conclusion.

Corollary 2.1

The Collatz-Sinogowitz irregularity of a graph is an integer if and only if both λ 1 ( G ) and 2 m / n are integers.

Finally, in the sequel, we consider the complete bipartite graphs.

2.2.2 Complete bipartite graphs

The spectral radius and the average degree of a complete bipartite graph K q , r are q r and 2 q r / n , respectively [9, p. 8], and thus, Collatz-Sinogowitz irregularity of a complete bipartite graph is

(1) CS ( K q , r ) = q r 2 q r n .

With the next two propositions, we show that the Collatz-Sinogowitz irregularity of a complete bipartite graph can be an even integer, but not an odd integer.

Proposition 2.3

The Collatz-Sinogowitz irregularity of a complete bipartite graph cannot be an odd integer.

Proof

Let G be a complete bipartite graph such that CS ( G ) is an integer. Then, by Corollary 2.1, both λ 1 ( G ) and 2 m / n are integers. Let d = g c d ( q , r ) , q = q d , r = r d , and g c d ( q , r ) = 1 . Then, 2 q r q + r = 2 q r d q + r . If p is a prime factor of q + r , then either p = 2 or p is a factor of d . (If p is a factor of q , then it is also a factor of r , which contradicts the fact that g c d ( q , r ) = 1 .) If q + r is odd, then any prime factor of q + r is also a prime factor of d , i.e., d = ( q + r ) c , for some c N . Hence, in this case, q = q ( q + r ) c and r = r ( q + r ) c , provided that g c d ( q , r ) = 1 and q + r is odd, i.e., exactly one of q , r is even.

Then,

CS ( G ) = c ( q + r ) q r 2 c q r ,

with q r being an even integer ( q r is even). Consequently, CS ( G ) is also even.

If q + r is even, then q + r = 2 k , for some k N . From 2 q r q + r = 2 q r d q + r = q r d k , similarly as in the previous case, we conclude that d = k b for some b N . Hence, q = q k b , r = r k b , g c d ( q , r ) = 1 , provided that q + r is even, i.e., both q and r are odd.

Then,

CS ( G ) = k b q r q r b

is even as a difference of two odd numbers.□

Proposition 2.4

For every positive even integer k, there exists an irregular complete bipartite graph whose Collatz-Sinogowitz irregularity is k.

Proof

Consider the complete bipartite graph K q , r . We may assume that q < r . Observe that when q = r , the graph is regular; then, λ 1 = d ¯ and CS ( K q , r ) = 0 .

Let set q = 5 i and r = 20 i ( n = 25 i ), i 1 . Then,

CS ( K q , r ) = q r 2 q r n = 2 i .

We conclude the current section with the following result.

Theorem 2.6

For every non-negative integer i, the number of complete bipartite graphs, whose Collatz-Sinogowitz irregularity lies in the interval ( i , i + 1 ) , is infinitely large.

Proof

We also assume that q < r . For q = r , we have CS ( K q , r ) = 0 . After an elementary analysis, applying the first- and second-derivative criteria, it can be obtained that CS ( K q , r ) has its maximum either for q max = 0.087378 r or for q max = 0.087378 r . The value of CS ( K q max , r ) is approximately 0.134884 r (the exact value, due to the ceiling and flooring, can be obtained for particular r ).

Let q q max , and let CS ( K q , r ) [ i 1 , i ] . We want to show that when q increases by one, then the value of CS lies in [ i 1 , i ] or in [ i 2 , i 1 ] . This will follow if we prove that

f ( q , r ) = CS ( K q . r ) CS ( K q + 1 , r ) = 2 r 2 ( q + r ) ( q + r + 1 ) + q r ( q + 1 ) r < 1 ,

for q q max . It can be easily checked that for any positive fixed r q , f ( q , r ) / q < 0 , which means that f ( q , r ) is a decreasing function in q , and its maximum is obtained when q = q max . It follows that

f ( 0.1 r , r ) > f ( q max , r ) f ( q , r ) .

It is easy to verify that f ( 0.1 r , r ) has one maximum, which is smaller than 0.25, and therefore also, f ( q , r ) < 0.25 . Hence, we have shown that CS ( K q + 1 , r ) lies in the same interval [ i 1 , i ] as CS ( K q , r ) , or in the interval [ i 2 , i 1 ] .

Let r f be a fixed value of r and let CS ( K q max , r f ) [ i 1 , i ] . Due to the facts that CS ( K q , r f ) decreases for q q max , r f q , CS ( K r f , r f ) = 0 , and CS ( K q , r f ) CS ( K q + 1 , r f ) + 1 , it can be concluded that in each interval [ k 1 , k ] , k = i , , 1 , there is at least one value of CS ( q , r f ) , for q [ q max , r f ] (actually, there are at least four values of CS ( q , r f ) , because f ( q , r ) < 0.25 ). Recall that CS ( K q max , r f ) = 0.134884 r f . We can obtain an arbitrary large value for CS ( K q max , r f ) by choosing an appropriate value of r f , or to turn around, we can obtain an arbitrarily large i such that CS ( K q max , r f ) [ i , i + 1 ] , and with at least one value of CS ( q , r f ) in each interval [ k 1 , k ] , k = i , , 1 , for q [ q max , r f ] . This can be satisfied for infinitely many instances r f of r , since r , and thus, we can obtain that in each interval [ i , i + 1 ] , i 0 , there are infinitely many values of CS ( K q , r ) .□

3 Conclusion

In this work, the inverse problem for the Collatz-Sinogowitz irregularity was considered. It was shown that for every interval I i = ( i , i + 1 ) , where i is a non-negative integer, there are infinitely many graphs whose Collatz-Sinogowitz irregularity lies in I i . This was shown within the classes of unicyclic graphs, starlike graphs, and complete bipartite graphs. Also, it was shown that the Collatz-Sinogowitz irregularity of a starlike graph cannot be an integer, while the Collatz-Sinogowitz irregularity of a complete bipartite graph can be an even integer, but not an odd integer. On the other hand, it was proven that for any non-negative integer i , there exists a unicycle graph whose Collatz-Sinogowitz irregularity is i . In general, it was shown that the Collatz-Sinogowitz irregularity of a graph is an integer if and only if both, its spectral radius and its average degree, are integers.

Further investigation of other classes of graphs is of interest. We conclude with the following conjecture. Namely, we believe that Theorem 2.3 can be extended to c -cyclic graphs, for any c 2 .

Conjecture 3.1

For every positive integer i larger than a given constant and for every c 2 ,

  1. there is a connected c -cyclic graph of order n , whose Collatz-Sinogowitz irregularity equals i , provided that n divides 2 ( c 1 ) ;

  2. there are infinitely many connected c -cyclic graphs whose Collatz-Sinogowitz irregularities lie in the interval ( i , i + 1 ) .

  1. Conflict of interest: The authors declare that there is no conflict of interest regarding the publication of this article.

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Received: 2023-01-30
Revised: 2023-03-03
Accepted: 2023-03-04
Published Online: 2023-05-16

© 2023 the author(s), published by De Gruyter

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

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  37. Well-posedness for bilevel vector equilibrium problems with variable domination structures
  38. Binet's second formula, Hermite's generalization, and two related identities
  39. Non-solid cone b-metric spaces over Banach algebras and fixed point results of contractions with vector-valued coefficients
  40. Multidimensional sampling-Kantorovich operators in BV-spaces
  41. A self-adaptive inertial extragradient method for a class of split pseudomonotone variational inequality problems
  42. Convergence properties for coordinatewise asymptotically negatively associated random vectors in Hilbert space
  43. Relating the super domination and 2-domination numbers in cactus graphs
  44. Compatibility of the method of brackets with classical integration rules
  45. On the inverse Collatz-Sinogowitz irregularity problem
  46. Positive solutions for boundary value problems of a class of second-order differential equation system
  47. Global analysis and control for a vector-borne epidemic model with multi-edge infection on complex networks
  48. Nonexistence of global solutions to Klein-Gordon equations with variable coefficients power-type nonlinearities
  49. On 2r-ideals in commutative rings with zero-divisors
  50. A comparison of some confidence intervals for a binomial proportion based on a shrinkage estimator
  51. The construction of nuclei for normal constituents of Bπ-characters
  52. Weak solution of non-Newtonian polytropic variational inequality in fresh agricultural product supply chain problem
  53. Mean square exponential stability of stochastic function differential equations in the G-framework
  54. Commutators of Hardy-Littlewood operators on p-adic function spaces with variable exponents
  55. Solitons for the coupled matrix nonlinear Schrödinger-type equations and the related Schrödinger flow
  56. The dual index and dual core generalized inverse
  57. Study on Birkhoff orthogonality and symmetry of matrix operators
  58. Uniqueness theorems of the Hahn difference operator of entire function with a Picard exceptional value
  59. Estimates for certain class of rough generalized Marcinkiewicz functions along submanifolds
  60. On semigroups of transformations that preserve a double direction equivalence
  61. Positive solutions for discrete Minkowski curvature systems of the Lane-Emden type
  62. A multigrid discretization scheme based on the shifted inverse iteration for the Steklov eigenvalue problem in inverse scattering
  63. Existence and nonexistence of solutions for elliptic problems with multiple critical exponents
  64. Interpolation inequalities in generalized Orlicz-Sobolev spaces and applications
  65. General Randić indices of a graph and its line graph
  66. On functional reproducing kernels
  67. On the Waring-Goldbach problem for two squares and four cubes
  68. Singular moduli of rth Roots of modular functions
  69. Classification of self-adjoint domains of odd-order differential operators with matrix theory
  70. On the convergence, stability and data dependence results of the JK iteration process in Banach spaces
  71. Hardy spaces associated with some anisotropic mixed-norm Herz spaces and their applications
  72. Remarks on hyponormal Toeplitz operators with nonharmonic symbols
  73. Complete decomposition of the generalized quaternion groups
  74. Injective and coherent endomorphism rings relative to some matrices
  75. Finite spectrum of fourth-order boundary value problems with boundary and transmission conditions dependent on the spectral parameter
  76. Continued fractions related to a group of linear fractional transformations
  77. Multiplicity of solutions for a class of critical Schrödinger-Poisson systems on the Heisenberg group
  78. Approximate controllability for a stochastic elastic system with structural damping and infinite delay
  79. On extremal cacti with respect to the first degree-based entropy
  80. Compression with wildcards: All exact or all minimal hitting sets
  81. Existence and multiplicity of solutions for a class of p-Kirchhoff-type equation RN
  82. Geometric classifications of k-almost Ricci solitons admitting paracontact metrices
  83. Positive periodic solutions for discrete time-delay hematopoiesis model with impulses
  84. On Hermite-Hadamard-type inequalities for systems of partial differential inequalities in the plane
  85. Existence of solutions for semilinear retarded equations with non-instantaneous impulses, non-local conditions, and infinite delay
  86. On the quadratic residues and their distribution properties
  87. On average theta functions of certain quadratic forms as sums of Eisenstein series
  88. Connected component of positive solutions for one-dimensional p-Laplacian problem with a singular weight
  89. Some identities of degenerate harmonic and degenerate hyperharmonic numbers arising from umbral calculus
  90. Mean ergodic theorems for a sequence of nonexpansive mappings in complete CAT(0) spaces and its applications
  91. On some spaces via topological ideals
  92. Linear maps preserving equivalence or asymptotic equivalence on Banach space
  93. Well-posedness and stability analysis for Timoshenko beam system with Coleman-Gurtin's and Gurtin-Pipkin's thermal laws
  94. On a class of stochastic differential equations driven by the generalized stochastic mixed variational inequalities
  95. Entire solutions of two certain Fermat-type ordinary differential equations
  96. Generalized Lie n-derivations on arbitrary triangular algebras
  97. Markov decision processes approximation with coupled dynamics via Markov deterministic control systems
  98. Notes on pseudodifferential operators commutators and Lipschitz functions
  99. On Graham partitions twisted by the Legendre symbol
  100. Strong limit of processes constructed from a renewal process
  101. Construction of analytical solutions to systems of two stochastic differential equations
  102. Two-distance vertex-distinguishing index of sparse graphs
  103. Regularity and abundance on semigroups of partial transformations with invariant set
  104. Liouville theorems for Kirchhoff-type parabolic equations and system on the Heisenberg group
  105. Spin(8,C)-Higgs pairs over a compact Riemann surface
  106. Properties of locally semi-compact Ir-topological groups
  107. Transcendental entire solutions of several complex product-type nonlinear partial differential equations in ℂ2
  108. Ordering stability of Nash equilibria for a class of differential games
  109. A new reverse half-discrete Hilbert-type inequality with one partial sum involving one derivative function of higher order
  110. About a dubious proof of a correct result about closed Newton Cotes error formulas
  111. Ricci ϕ-invariance on almost cosymplectic three-manifolds
  112. Schur-power convexity of integral mean for convex functions on the coordinates
  113. A characterization of a ∼ admissible congruence on a weakly type B semigroup
  114. On Bohr's inequality for special subclasses of stable starlike harmonic mappings
  115. Properties of meromorphic solutions of first-order differential-difference equations
  116. A double-phase eigenvalue problem with large exponents
  117. On the number of perfect matchings in random polygonal chains
  118. Evolutoids and pedaloids of frontals on timelike surfaces
  119. A series expansion of a logarithmic expression and a decreasing property of the ratio of two logarithmic expressions containing cosine
  120. The 𝔪-WG° inverse in the Minkowski space
  121. Stability result for Lord Shulman swelling porous thermo-elastic soils with distributed delay term
  122. Approximate solvability method for nonlocal impulsive evolution equation
  123. Construction of a functional by a given second-order Ito stochastic equation
  124. Global well-posedness of initial-boundary value problem of fifth-order KdV equation posed on finite interval
  125. On pomonoid of partial transformations of a poset
  126. New fractional integral inequalities via Euler's beta function
  127. An efficient Legendre-Galerkin approximation for the fourth-order equation with singular potential and SSP boundary condition
  128. Eigenfunctions in Finsler Gaussian solitons
  129. On a blow-up criterion for solution of 3D fractional Navier-Stokes-Coriolis equations in Lei-Lin-Gevrey spaces
  130. Some estimates for commutators of sharp maximal function on the p-adic Lebesgue spaces
  131. A preconditioned iterative method for coupled fractional partial differential equation in European option pricing
  132. A digital Jordan surface theorem with respect to a graph connectedness
  133. A quasi-boundary value regularization method for the spherically symmetric backward heat conduction problem
  134. The structure fault tolerance of burnt pancake networks
  135. Average value of the divisor class numbers of real cubic function fields
  136. Uniqueness of exponential polynomials
  137. An application of Hayashi's inequality in numerical integration
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