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Some inequalities on the spectral radius of nonnegative tensors

  • Chao Ma , Hao Liang , Qimiao Xie EMAIL logo and Pengcheng Wang
Published/Copyright: May 21, 2020

Abstract

The eigenvalues and the spectral radius of nonnegative tensors have been extensively studied in recent years. In this paper, we investigate the analytic properties of nonnegative tensors and give some inequalities on the spectral radius.

MSC 2010: 15A18; 15A39; 15A69

1 Introduction

In recent years, problems related to tensors have drawn much people’s attention. As a generalization of matrix theory, fruitful research achievements have been made in topics such as tensor decomposition, tensor eigenvalues and structured tensors [1,2,3]. Tensors also have wide applications in quantum entanglement, higher order Markov chains, magnetic resonance imaging, machine learning, data analysis, polynomial optimization, nonlinear optimization, hypergraph partitioning, etc. [4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19].

In 2005, Qi [20] and Lim [21] independently defined the concept of eigenvalues of tensors. In 2008, Chang et al. established the Perron–Frobenius theorem for nonnegative tensors [22]. In 2010, Yang and Yang introduced the definition of spectral radius of tensors [23]. Some bounds on the spectral radius of nonnegative tensors are given in [24,25,26,27,28].

In the proof of Theorem 2.3 in [23], the authors considered the sequence of nonnegative tensors and gave the limit formula regarding the spectral radius. Note that the result holds when the sequence is monotonic. We want to know whether the result still holds when the sequence is not monotonic and try to investigate the continuity of the spectral radius of nonnegative tensors by some inequalities. Recently, Sun et al. generalized some inequalities on the spectral radius of the Hadamard product of nonnegative matrices to nonnegative tensors [29]. Their beautiful results make us interested in the further study of the Hadamard product of tensors.

In this paper, we mainly investigate the analytic properties of the spectral radius of nonnegative tensors. We discuss the continuity of the spectral radius by means of limit formulas as well as tensor inequalities involving norms. We also give some inequalities on the spectral radius of the Hadamard product of nonnegative tensors. These results can be seen as a generalization of the existing inequalities on the spectral radius of nonnegative matrices.

The paper is organized as follows. In Section 2, we collect some definitions, notations and helpful lemmas. In Section 3, we discuss the continuity of the spectral radius. In Section 4, we give some inequalities on the spectral radius involving the Hadamard product.

2 Preliminaries

A real mth order n-dimensional tensor (hypermatrix) A = ( a i 1 i 2 i m ) is a multiarray of real entries a i 1 i 2 i m , where i j ∈ {1, 2,…,n} for j ∈ {1, 2,…,m}. When m = 2, A is a matrix of order n. The set of all mth order n-dimensional real tensors is denoted as T m,n . Throughout this paper, we assume that m, n ≥ 2.

A tensor is said to be nonnegative (positive) if each of its entry is nonnegative (positive). Denote by O the zero tensor, and by J the tensor with each entry equal to 1. For a tensor A , A ( > ) O implies that A is nonnegative (positive). For two tensors A and , A or A implies that A is nonnegative. Let | A | be the tensor obtained from A by taking the absolute values of the entries. Then, | A | is nonnegative and A | A | . A = ( a i 1 i 2 i m ) T m , n is said to be reducible, if there is a nonempty proper index subset I { 1 , 2 , , n } such that

a i 1 i 2 i m = 0 ,   i 1 I ,   i 2 , i 3 , , i m I .

A tensor is said to be irreducible if it is not reducible.

The inner product of A = ( a i 1 i 2 i m ) , = ( b i 1 i 2 i m ) T m , n , denoted by A , , is defined as follows:

A , = i 1 , i 2 , , i m = 1 n a i 1 i 2 i m b i 1 i 2 i m .

The Frobenius norm of A is defined and denoted as | | A | | F = A , A . Denote by n the set of real vectors of dimension n. + n ( + + n ) represents the cone { x = ( x 1 , x 2 , , x n ) T n   |   x i ( > ) 0 ,   i = 1 , 2 , , n } .

Let A = ( a i 1 i 2 i m ) T m , n , and let x = (x 1, x 2,…,x n ) T be a complex vector of dimension n. Then, A x m 1 is a vector of dimension n with its ith component as

( A x m 1 ) i = i 2 , , i m = 1 n a i i 2 i m x i 2 x i m

for i = 1, 2,…,n. Denote by 0 the zero vector. A complex number λ is called an eigenvalue of A if it together with x 0 forms a solution to the following system of homogeneous polynomial equations:

A x m 1 = λ x [ m 1 ] ,

where x [ m 1 ] = ( x 1 m 1 , x 2 m 1 , , x n m 1 ) T . The nonzero vector x is called an eigenvector of A corresponding to the eigenvalue λ. The spectral radius of A is defined and denoted as

ρ ( A ) = max { | λ | : λ   is an eigenvalue of   A } .

It is well known that the Perron–Frobenius theorem is a fundamental result for nonnegative matrices [30, p. 123]. Chang, Pearson and Zhang generalized this theorem to nonnegative tensors. Yang and Yang gave some further results on the Perron–Frobenius theorem for nonnegative tensors. We summarize some of their results as follows.

Lemma 2.1

[22] Let A T m , n be nonnegative. Then, there exists λ 0 0 and x 0 + n such that A x 0 m 1 = λ 0 x 0 [ m 1 ] .

Lemma 2.2

[22] Let A T m , n be irreducible nonnegative. Then, there exists λ 0 > 0 and x 0 + + n such that A x 0 m 1 = λ 0 x 0 [ m 1 ] . Moreover, if λ is an eigenvalue with a nonnegative eigenvector, then λ = λ 0. If λ is an eigenvalue of A , then |λ| ≤ λ 0.

Lemma 2.3

[23] Let A , T m , n be nonnegative. Then,

  1. ρ ( A ) is an eigenvalue of A with a nonnegative eigenvector corresponding to it;

  2. If λ is an eigenvalue of A with a positive eigenvector, then λ = ρ ( A ) ;

  3. If A , then ρ ( A ) ρ ( ) ;

  4. ρ ( A ) = max x + n \ { 0 } min x i 0 ( A x m 1 ) i x i m 1 ;

  5. If x + + n , then ρ ( A ) max 1 i n ( A x m 1 ) i x i m 1 ;

  6. Let A k = A + 1 k J , k = 1, 2,… Then, lim k ρ ( A k ) = ρ ( A ) .

3 Continuity of the spectral radius of nonnegative tensors

Suppose A T m , n , and { A k } k = 1 is a set of mth order n-dimensional tensors. lim k A k = A means lim k ( A k ) i 1 i 2 i m = ( A ) i 1 i 2 i m for any i 1, i 2,…,i m .

Lemma 3.1

Let A T m , n be nonnegative, and let { k } k = 1 be a set of mth order n-dimensional nonnegative tensors with lim k k = O . If A has an eigenvalue with a positive eigenvector corresponding to it, then lim k ρ ( A + k ) = ρ ( A ) .

Proof

By Lemma 2.3 (ii), there exists x = ( x 1 , x 2 , , x n ) T + + n such that A x m 1 = ρ ( A ) x [ m 1 ] . Then, by Lemma 2.3 (iii) and (v),

ρ ( A ) ρ ( A + k ) max 1 i n ( ( A + k ) x m 1 ) i x i m 1 = ρ ( A ) + max 1 i n ( k x m 1 ) i x i m 1 .

Since lim k k = O , lim k max 1 i n ( k x m 1 ) i x i m 1 = 0 . Thus, lim k ρ ( A + k ) = ρ ( A ) .□

Lemma 3.2

Let A T m , n be nonnegative, and let { k } k = 1 be a set of mth order n-dimensional nonnegative tensors such that k A for k = 1, 2,… with lim k k = O . Then, lim k ρ ( A k ) = ρ ( A ) .

Proof

By Lemma 2.3 (i), there exists nonzero y = ( y 1 , y 2 , , y n ) T + n such that A y m 1 = ρ ( A ) y [ m 1 ] . Then, by Lemma 2.3 (iii) and (iv),

ρ ( A ) ρ ( A k ) min y i 0 ( ( A k ) y m 1 ) i y i m 1 = ρ ( A ) max y i 0 ( k y m 1 ) i y i m 1 .

Since lim k k = O , lim k max y i 0 ( k y m 1 ) i y i m 1 = 0 . Thus, lim k ρ ( A k ) = ρ ( A ) .□

Theorem 3.3

Let A T m , n be nonnegative, and suppose A has an eigenvalue with a positive eigenvector corresponding to it. Let { A k } k = 1 be a set of mth order n-dimensional nonnegative tensors with lim k A k = A . Then, lim k ρ ( A k ) = ρ ( A ) .

Proof

Let A A k = k + k , k = 1, 2,…, where

( k + ) i 1 i 2 i m = { ( A A k ) i 1 i 2 i m , if ( A A k ) i 1 i 2 i m > 0 ; 0 , otherwise .

Then, k + 0 ,   k 0 ,   A k + 0 ,   lim k k + = 0 , lim k k = 0 . Since A k = A + k k + A + k , by Lemma 2.3 (iii), ρ ( A k ) ρ ( A + k ) . Then, by Lemma 3.1, lim k ρ ( A k ) lim k ρ ( A + k ) = ρ ( A ) . Since A k A k k = A k + , by Lemma 2.3 (iii), ρ ( A k ) ρ ( A k + ) . Then, by Lemma 3.2, lim k ρ ( A k ) lim k ρ ( A k + ) = ρ ( A ) . This completes the proof.□

Let A = ( a i 1 i 2 i m ) T m , n . If the entries a i 1 i 2 i m are invariant under any permutation of their indices, then A is called a symmetric tensor. The set of all mth order n-dimensional real symmetric tensors is denoted as S m,n . Let x = (x 1, x 2,…,x n ) T . Define

A x m = i 1 , i 2 , , i m = 1 n a i 1 i 2 i m x i 1 x i 2 x i m .

Lemma 3.4

Let A T m , n be positive, and let x = ( x 1 , x 2 , , x n ) T + + n , u = ( u 1 , u 2 , , u n ) T + n , v = ( v 1 , v 2 , , v n ) T + n . Then,

A x m i 1 , i 2 , , i m = 1 n ( v i 1 u i 2 u i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m v T ( A u m 1 ) i 1 , i 2 , , i m = 1 n ( x i 1 x i 2 x i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m .

Proof

Since the function f(t) = log t is concave on (0, +∞), we have

log ( i 1 , i 2 , , i m = 1 n a i 1 i 2 i m x i 1 x i 2 x i m A x m v i 1 u i 2 u i m x i 1 x i 2 x i m ) i 1 , i 2 , , i m = 1 n a i 1 i 2 i m x i 1 x i 2 x i m A x m log v i 1 u i 2 u i m x i 1 x i 2 x i m .

Then,

log v T ( A u m 1 ) A x m log i 1 , i 2 , , i m = 1 n ( v i 1 u i 2 u i m x i 1 x i 2 x i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m ,

which implies

v T ( A u m 1 ) A x m i 1 , i 2 , , i m = 1 n ( v i 1 u i 2 u i m x i 1 x i 2 x i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m .

This completes the proof.□

Lemma 3.5

Let A S m , n be nonnegative, and let x = ( x 1 , x 2 , , x n ) T + n . Then, A x m ρ ( A ) i = 1 n x i m .

Proof

By Lemma 2.3 (vi), it suffices to consider the case when A is positive. First suppose x = ( x 1 , x 2 , , x n ) T + + n . Note that Lemma 2.2 implies that ρ ( A ) is an eigenvalue of A with a positive eigenvector corresponding to it. Let u = ( u 1 , u 2 , , u n ) T + + n be the eigenvector corresponding to ρ ( A ) , and let v = ( v 1 , v 2 , , v n ) T + + n with v i = x i m u i m 1 , i = 1, 2,…,n. Since A is symmetric,

i 1 , i 2 , , i m = 1 n ( v i 1 u i 2 u i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m = i = 1 n ( v i u i m 1 ) x i ( A x m 1 ) i A x m ,

i 1 , i 2 , , i m = 1 n ( x i 1 x i 2 x i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m = i = 1 n ( x i m ) x i ( A x m 1 ) i A x m .

Thus,

i 1 , i 2 , , i m = 1 n ( v i 1 u i 2 u i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m = i 1 , i 2 , , i m =1 n ( x i 1 x i 2 x i m ) a i 1 i 2 i m x i 1 x i 2 x i m A x m .

By Lemma 3.4, A x m v T ( A u m 1 ) = v T ρ ( A ) u [ m 1 ] = ρ ( A ) i = 1 n v i u i m 1 = ρ ( A ) i = 1 n x i m .

Next suppose x = ( x 1 , x 2 , , x n ) T + n . For k = 1, 2,…, let x ( k ) = x + 1 k e , where e is the vector with each component equal to 1. Then, x ( k ) + + n and lim k x ( k ) = x . By what we have proved above, A ( x ( k ) ) m ρ ( A ) i = 1 n ( x i + 1 k ) m for k = 1, 2,…. The conclusion holds when k → ∞.□

Theorem 3.6

Let A , S m , n be nonnegative. Then, ρ ( A + ) ρ ( A ) + ρ ( ) .

Proof

By Lemma 2.3 (i), let x = ( x 1 , x 2 , , x n ) + n be the eigenvector of A + corresponding to ρ ( A + ) with i = 1 n x i m = 1 . Then, by Lemma 3.5, ρ ( A + ) = ρ ( A + ) i = 1 n x i m = i = 1 n x i ( ( A + ) x m 1 ) i = ( A + ) x m = A x m + x m ρ ( A ) i = 1 n x i m + ρ ( ) i = 1 n x i m = ρ ( A ) + ρ ( ) .

Let x = ( x 1 , x 2 , , x n ) T n . Denote by x m the tensor in T m,n with its (i 1, i 2,…,i m ) entry as x i 1 x i 2 x i m .

Lemma 3.7

Let x = ( x 1 , x 2 , , x n ) T + n with i = 1 n x i m = 1 . Then, | | x m | | F n m 2 1 .

Proof

Since i = 1 n x i m = 1 with m ≥ 2 by the power mean inequality [31, p. 203], we have ( x 1 2 + x 2 2 + + x n 2 n ) 1 2 ( x 1 m + x 2 m + + x n m n ) 1 m = ( 1 n ) 1 m . Then, | | x m | | F 2 = i 1 , i 2 , , i m = 1 n x i 1 2 x i 2 2 x i m 2 = ( x 1 2 + x 2 2 + + x n 2 ) m n m 2 . This completes the proof.□

Lemma 3.8

Let A T m , n be nonnegative. Then, ρ ( A ) n m 2 1 | | A | | F .

Proof

Let x = ( x 1 , x 2 , , x n ) T + n be the eigenvector of A corresponding to ρ ( A ) with i = 1 n x i m = 1 . By Lemma 3.7 and the Cauchy–Schwarz inequality, ρ ( A ) = ρ ( A ) i = 1 n x i m = i = 1 n x i ( A x m 1 ) i = i , i 2 , , i m = 1 n a i i 2 i m x i x i 2 x i m = A , x m | | A | | F | | x m | | F n m 2 1 | | A | | F .□

Theorem 3.9

Let A , S m , n be nonnegative. Then, | ρ ( A ) ρ ( ) | n m 2 1 | | A | | F .

Proof

Since A | A | , A | A | + . By Theorem 3.6, ρ ( A ) ρ ( | A | + ) ρ ( | A | ) + ρ ( ) . Thus, ρ ( A ) ρ ( ) ρ ( | A | ) . Similarly, ρ ( ) ρ ( A ) ρ ( | A | ) . Then, by Lemma 3.8, | ρ ( A ) ρ ( ) | ρ ( | A | ) n m 2 1 | | A | | F .□

4 Some inequalities involving the Hadamard product

Let A = ( a i 1 i 2 i m ) , = ( b i 1 i 2 i m ) T m , n . The Hadamard product of A and is defined and denoted as A = ( a i 1 i 2 i m b i 1 i 2 i m ) T m , n . Let A = ( a i 1 i 2 i m ) be nonnegative, and let α be a positive real number. The αth Hadamard power of A is the tensor A [ α ] = ( a i 1 i 2 i m α ) . Similarly, for two vectors x = (x 1, x 2,…,x n ) T and y = (y 1, y 2,…,y n ) T , let x y = ( x 1 y 1 , x 2 y 2 , , x n y n ) T ; for x + n and α > 0 let x [ α ] = ( x 1 α , x 2 α , , x n α ) .

Theorem 4.1

Let A T m , n be nonnegative. Then, ( ρ ( A [ r ] ) ) 1 r ( ρ ( A [ s ] ) ) 1 s , with rs > 0.

Proof

By Lemma 2.3 (vi), we may suppose A is positive. Let A [ s ] = = ( b i 1 i 2 i m ) > O , and let t = r s 1 . It suffices to prove that ρ ( [ t ] ) ( ρ ( ) ) t . By Lemma 2.2, there exists x = ( x 1 , x 2 , , x n ) T + + n such that x m 1 = ρ ( ) x [ m 1 ] . Then, for i = 1, 2,…,n,

( [ t ] ( x [ t ] ) m 1 ) i = i 2 , , i m = 1 n b i , i 2 i m t x i 2 t x i m t ( i 2 , , i m = 1 n b i , i 2 i m x i 2 x i m ) t = ( ( x m 1 ) i ) t = ( ( ρ ( ) x [ m 1 ] ) i ) t = ( ρ ( ) ) t ( x i t ) m 1 .

By Lemma 2.3 (v),

ρ ( [ t ] ) max 1 i n ( [ t ] ( x [ t ] ) m 1 ) i ( x i t ) m 1 ( ρ ( ) ) t .

This completes the proof.□

Theorem 4.2

Let A 1 , A 2 , , A k T m , n be nonnegative. Then, ρ ( A 1 [ α 1 ] A 2 [ α 2 ] A k [ α k ] ) ( ρ ( A 1 ) ) α 1 ( ρ ( A 2 ) ) α 2 ( ρ ( A k ) ) α k with α i >0 and i =1 k α i 1 .

Proof

By continuity of the spectral radius, we may suppose A 1 , A 2 , , A k are all positive. Let α = i =1 k α i 1, and let A i = ( a i 1 i 2 i m ( i ) ) , i = 1, 2,…,k. By Theorem 4.1,

(1) ρ ( A 1 [ α 1 ] A 2 [ α 2 ] A k [ α k ] ) = ρ ( ( A 1 [ α 1 α ] A 2 [ α 2 α ] A k [ α k α ] ) [ α ] ) ( ρ ( A 1 [ α 1 α ] A 2 [ α 2 α ] A k [ α k α ] ) ) α .

By Lemma 2.2, for i = 1, 2,…,k, there exist x ( i ) = ( x 1 ( i ) , x 2 ( i ) , , x n ( i ) ) T + + n such that A i ( x ( i ) ) m 1 = ρ ( A i ) ( x ( i ) ) [ m 1 ] . Let A = A 1 [ α 1 α ] A 2 [ α 2 α ] A k [ α k α ] , and let x = ( x ( 1 ) ) [ α 1 α ] ( x ( 2 ) ) [ α 2 α ] ( x ( k ) ) [ α k α ] = ( x 1 , x 2 , , x n ) T + + n . For i = 1, 2,…,n,

( A x m 1 ) i = i 2 , , i m = 1 n ( ( a i , i 2 i m ( 1 ) ) α 1 α ( a i , i 2 i m ( k ) ) α k α ) ( ( x i 2 ( 1 ) ) α 1 α ( x i 2 ( k ) ) α k α ) ( ( x i m ( 1 ) ) α 1 α ( x i m ( k ) ) α k α ) = i 2 , , i m = 1 n ( a i , i 2 i m ( 1 ) x i 2 ( 1 ) x i m ( 1 ) ) α 1 α ( a i , i 2 i m ( k ) x i 2 ( k ) x i m ( k ) ) α k α ( i 2 , , i m = 1 n a i , i 2 i m ( 1 ) x i 2 ( 1 ) x i m ( 1 ) ) α 1 α ( i 2 , , i m = 1 n a i , i 2 i m ( k ) x i 2 ( k ) x i m ( k ) ) α k α = ( ( A 1 ( x ( 1 ) ) m 1 ) i ) α 1 α ( ( A k ( x ( k ) ) m 1 ) i ) α k α = ( ρ ( A 1 ) ( x i ( 1 ) ) m 1 ) α 1 α ( ρ ( A k ) ( x i ( k ) ) m 1 ) α k α = ( ρ ( A 1 ) ) α 1 α ( ρ ( A k ) ) α k α ( ( x i ( 1 ) ) α 1 α ( x i ( k ) ) α k α ) m 1 = ( ρ ( A 1 ) ) α 1 α ( ρ ( A k ) ) α k α x i m 1 .

Then, by Lemma 2.3 (v), ρ ( A ) max 1 i n ( A x m 1 ) i x i m 1 ( ρ ( A 1 ) ) α 1 α ( ρ ( A k ) ) α k α . Thus, by (1),

ρ ( A 1 [ α 1 ] A k [ α k ] ) ( ρ ( A 1 [ α 1 α ] A k [ α k α ] ) ) α = ( ρ ( A ) ) α ( ρ ( A 1 ) ) α 1 ( ρ ( A k ) ) α k .

5 Conclusion

In this paper, we focus on the analytic properties of the spectral radius of nonnegative tensors. First, we discuss the continuity of the spectral radius. Then, we give some inequalities on the spectral radius involving the Hadamard product. These results generalize some existing results on the spectral properties of nonnegative matrices to nonnegative tensors.

Acknowledgement

The authors would like to express their sincere thanks to referees and editor for their enthusiastic guidance and help. This research was supported by the National Natural Science Foundation of China (Grant No. 11601322, 71503166 and 61573240).

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Received: 2019-05-03
Revised: 2020-02-10
Accepted: 2020-03-15
Published Online: 2020-05-21

© 2020 Chao Ma et al., published by De Gruyter

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

Articles in the same Issue

  1. Regular Articles
  2. Non-occurrence of the Lavrentiev phenomenon for a class of convex nonautonomous Lagrangians
  3. Strong and weak convergence of Ishikawa iterations for best proximity pairs
  4. Curve and surface construction based on the generalized toric-Bernstein basis functions
  5. The non-negative spectrum of a digraph
  6. Bounds on F-index of tricyclic graphs with fixed pendant vertices
  7. Crank-Nicolson orthogonal spline collocation method combined with WSGI difference scheme for the two-dimensional time-fractional diffusion-wave equation
  8. Hardy’s inequalities and integral operators on Herz-Morrey spaces
  9. The 2-pebbling property of squares of paths and Graham’s conjecture
  10. Existence conditions for periodic solutions of second-order neutral delay differential equations with piecewise constant arguments
  11. Orthogonal polynomials for exponential weights x2α(1 – x2)2ρe–2Q(x) on [0, 1)
  12. Rough sets based on fuzzy ideals in distributive lattices
  13. On more general forms of proportional fractional operators
  14. The hyperbolic polygons of type (ϵ, n) and Möbius transformations
  15. Tripled best proximity point in complete metric spaces
  16. Metric completions, the Heine-Borel property, and approachability
  17. Functional identities on upper triangular matrix rings
  18. Uniqueness on entire functions and their nth order exact differences with two shared values
  19. The adaptive finite element method for the Steklov eigenvalue problem in inverse scattering
  20. Existence of a common solution to systems of integral equations via fixed point results
  21. Fixed point results for multivalued mappings of Ćirić type via F-contractions on quasi metric spaces
  22. Some inequalities on the spectral radius of nonnegative tensors
  23. Some results in cone metric spaces with applications in homotopy theory
  24. On the Malcev products of some classes of epigroups, I
  25. Self-injectivity of semigroup algebras
  26. Cauchy matrix and Liouville formula of quaternion impulsive dynamic equations on time scales
  27. On the symmetrized s-divergence
  28. On multivalued Suzuki-type θ-contractions and related applications
  29. Approximation operators based on preconcepts
  30. Two types of hypergeometric degenerate Cauchy numbers
  31. The molecular characterization of anisotropic Herz-type Hardy spaces with two variable exponents
  32. Discussions on the almost 𝒵-contraction
  33. On a predator-prey system interaction under fluctuating water level with nonselective harvesting
  34. On split involutive regular BiHom-Lie superalgebras
  35. Weighted CBMO estimates for commutators of matrix Hausdorff operator on the Heisenberg group
  36. Inverse Sturm-Liouville problem with analytical functions in the boundary condition
  37. The L-ordered L-semihypergroups
  38. Global structure of sign-changing solutions for discrete Dirichlet problems
  39. Analysis of F-contractions in function weighted metric spaces with an application
  40. On finite dual Cayley graphs
  41. Left and right inverse eigenpairs problem with a submatrix constraint for the generalized centrosymmetric matrix
  42. Controllability of fractional stochastic evolution equations with nonlocal conditions and noncompact semigroups
  43. Levinson-type inequalities via new Green functions and Montgomery identity
  44. The core inverse and constrained matrix approximation problem
  45. A pair of equations in unlike powers of primes and powers of 2
  46. Miscellaneous equalities for idempotent matrices with applications
  47. B-maximal commutators, commutators of B-singular integral operators and B-Riesz potentials on B-Morrey spaces
  48. Rate of convergence of uniform transport processes to a Brownian sheet
  49. Curves in the Lorentz-Minkowski plane with curvature depending on their position
  50. Sequential change-point detection in a multinomial logistic regression model
  51. Tiny zero-sum sequences over some special groups
  52. A boundedness result for Marcinkiewicz integral operator
  53. On a functional equation that has the quadratic-multiplicative property
  54. The spectrum generated by s-numbers and pre-quasi normed Orlicz-Cesáro mean sequence spaces
  55. Positive coincidence points for a class of nonlinear operators and their applications to matrix equations
  56. Asymptotic relations for the products of elements of some positive sequences
  57. Jordan {g,h}-derivations on triangular algebras
  58. A systolic inequality with remainder in the real projective plane
  59. A new characterization of L2(p2)
  60. Nonlinear boundary value problems for mixed-type fractional equations and Ulam-Hyers stability
  61. Asymptotic normality and mean consistency of LS estimators in the errors-in-variables model with dependent errors
  62. Some non-commuting solutions of the Yang-Baxter-like matrix equation
  63. General (p,q)-mixed projection bodies
  64. An extension of the method of brackets. Part 2
  65. A new approach in the context of ordered incomplete partial b-metric spaces
  66. Sharper existence and uniqueness results for solutions to fourth-order boundary value problems and elastic beam analysis
  67. Remark on subgroup intersection graph of finite abelian groups
  68. Detectable sensation of a stochastic smoking model
  69. Almost Kenmotsu 3-h-manifolds with transversely Killing-type Ricci operators
  70. Some inequalities for star duality of the radial Blaschke-Minkowski homomorphisms
  71. Results on nonlocal stochastic integro-differential equations driven by a fractional Brownian motion
  72. On surrounding quasi-contractions on non-triangular metric spaces
  73. SEMT valuation and strength of subdivided star of K 1,4
  74. Weak solutions and optimal controls of stochastic fractional reaction-diffusion systems
  75. Gradient estimates for a weighted nonlinear parabolic equation and applications
  76. On the equivalence of three-dimensional differential systems
  77. Free nonunitary Rota-Baxter family algebras and typed leaf-spaced decorated planar rooted forests
  78. The prime and maximal spectra and the reticulation of residuated lattices with applications to De Morgan residuated lattices
  79. Explicit determinantal formula for a class of banded matrices
  80. Dynamics of a diffusive delayed competition and cooperation system
  81. Error term of the mean value theorem for binary Egyptian fractions
  82. The integral part of a nonlinear form with a square, a cube and a biquadrate
  83. Meromorphic solutions of certain nonlinear difference equations
  84. Characterizations for the potential operators on Carleson curves in local generalized Morrey spaces
  85. Some integral curves with a new frame
  86. Meromorphic exact solutions of the (2 + 1)-dimensional generalized Calogero-Bogoyavlenskii-Schiff equation
  87. Towards a homological generalization of the direct summand theorem
  88. A standard form in (some) free fields: How to construct minimal linear representations
  89. On the determination of the number of positive and negative polynomial zeros and their isolation
  90. Perturbation of the one-dimensional time-independent Schrödinger equation with a rectangular potential barrier
  91. Simply connected topological spaces of weighted composition operators
  92. Generalized derivatives and optimization problems for n-dimensional fuzzy-number-valued functions
  93. A study of uniformities on the space of uniformly continuous mappings
  94. The strong nil-cleanness of semigroup rings
  95. On an equivalence between regular ordered Γ-semigroups and regular ordered semigroups
  96. Evolution of the first eigenvalue of the Laplace operator and the p-Laplace operator under a forced mean curvature flow
  97. Noetherian properties in composite generalized power series rings
  98. Inequalities for the generalized trigonometric and hyperbolic functions
  99. Blow-up analyses in nonlocal reaction diffusion equations with time-dependent coefficients under Neumann boundary conditions
  100. A new characterization of a proper type B semigroup
  101. Constructions of pseudorandom binary lattices using cyclotomic classes in finite fields
  102. Estimates of entropy numbers in probabilistic setting
  103. Ramsey numbers of partial order graphs (comparability graphs) and implications in ring theory
  104. S-shaped connected component of positive solutions for second-order discrete Neumann boundary value problems
  105. The logarithmic mean of two convex functionals
  106. A modified Tikhonov regularization method based on Hermite expansion for solving the Cauchy problem of the Laplace equation
  107. Approximation properties of tensor norms and operator ideals for Banach spaces
  108. A multi-power and multi-splitting inner-outer iteration for PageRank computation
  109. The edge-regular complete maps
  110. Ramanujan’s function k(τ)=r(τ)r2(2τ) and its modularity
  111. Finite groups with some weakly pronormal subgroups
  112. A new refinement of Jensen’s inequality with applications in information theory
  113. Skew-symmetric and essentially unitary operators via Berezin symbols
  114. The limit Riemann solutions to nonisentropic Chaplygin Euler equations
  115. On singularities of real algebraic sets and applications to kinematics
  116. Results on analytic functions defined by Laplace-Stieltjes transforms with perfect ϕ-type
  117. New (p, q)-estimates for different types of integral inequalities via (α, m)-convex mappings
  118. Boundary value problems of Hilfer-type fractional integro-differential equations and inclusions with nonlocal integro-multipoint boundary conditions
  119. Boundary layer analysis for a 2-D Keller-Segel model
  120. On some extensions of Gauss’ work and applications
  121. A study on strongly convex hyper S-subposets in hyper S-posets
  122. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the real axis
  123. Special Issue on Graph Theory (GWGT 2019), Part II
  124. On applications of bipartite graph associated with algebraic structures
  125. Further new results on strong resolving partitions for graphs
  126. The second out-neighborhood for local tournaments
  127. On the N-spectrum of oriented graphs
  128. The H-force sets of the graphs satisfying the condition of Ore’s theorem
  129. Bipartite graphs with close domination and k-domination numbers
  130. On the sandpile model of modified wheels II
  131. Connected even factors in k-tree
  132. On triangular matroids induced by n3-configurations
  133. The domination number of round digraphs
  134. Special Issue on Variational/Hemivariational Inequalities
  135. A new blow-up criterion for the Nabc family of Camassa-Holm type equation with both dissipation and dispersion
  136. On the finite approximate controllability for Hilfer fractional evolution systems with nonlocal conditions
  137. On the well-posedness of differential quasi-variational-hemivariational inequalities
  138. An efficient approach for the numerical solution of fifth-order KdV equations
  139. Generalized fractional integral inequalities of Hermite-Hadamard-type for a convex function
  140. Karush-Kuhn-Tucker optimality conditions for a class of robust optimization problems with an interval-valued objective function
  141. An equivalent quasinorm for the Lipschitz space of noncommutative martingales
  142. Optimal control of a viscous generalized θ-type dispersive equation with weak dissipation
  143. Special Issue on Problems, Methods and Applications of Nonlinear analysis
  144. Generalized Picone inequalities and their applications to (p,q)-Laplace equations
  145. Positive solutions for parametric (p(z),q(z))-equations
  146. Revisiting the sub- and super-solution method for the classical radial solutions of the mean curvature equation
  147. (p,Q) systems with critical singular exponential nonlinearities in the Heisenberg group
  148. Quasilinear Dirichlet problems with competing operators and convection
  149. Hyers-Ulam-Rassias stability of (m, n)-Jordan derivations
  150. Special Issue on Evolution Equations, Theory and Applications
  151. Instantaneous blow-up of solutions to the Cauchy problem for the fractional Khokhlov-Zabolotskaya equation
  152. Three classes of decomposable distributions
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