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Fibonacci vector and matrix p-norms

  • Francisco Salas-Molina EMAIL logo , David Pla-Santamaria , Maria Luisa Vercher-Ferrándiz and Javier Reig-Mullor
Published/Copyright: October 9, 2025

Abstract

This article delves into vector and matrix norms of Fibonacci numbers. Two classes of Fibonacci vectors and a parametric p -norm are defined. From this definition, several properties of the Fibonacci vector and matrix p -norms are described by varying parameter p . A closed-form expression is given to obtain the value of p , setting the difference between the p -norm and the infinite norm below a given threshold. A new symmetric k -Fibonacci matrix is defined, and a simple reorganization simplifies the computation of its p -norm. The analysis is extended to p -distances when considering the norm of the difference of two vectors (matrices) of the same size.

MSC 2020: 11B39; 15A60

1 Introduction

Within matrix theory, the concept of a norm has emerged as a fundamental tool in the analysis of mathematical structures, providing a rigorous means to quantify the magnitude or distance of algebraic entities such as vectors and matrices. Norms are applied in a wide range of disciplines, including optimization, linear algebra, and machine learning, where they facilitate the characterization of structural and functional properties of mathematical objects [1]. Vector norms, such as the Euclidean norm, measure the length of a vector, while matrix norms generalize these notions to matrices, offering insights into their behavior and structure. Among these, the Frobenius norm, denoted by A 2 , is one of the most widely utilized due to its computational simplicity and interpretability

(1) A 2 = i = 1 m j = 1 n a i j 2 1 2 .

The Fibonacci sequence { 1 , 1 , 2 , 3 , 5 , 8 , 13 , } is defined through the n th Fibonacci number F n and the classical recurrence relation:

(2) F 1 = F 2 = 1 , F n = F n 1 + F n 2 , n > 2 .

Combining matrix theory and Fibonacci numbers leads to examining determinants, norms, and characteristic properties associated with various matrix types. Some recent examples are the study of r -min and r -max matrices populated with special cases of Fibonacci numbers [2,3]. Other studies deal with circulant matrices [4] or tridiagonal matrices and trigonometric identities to propose a method for complex factorization of bi-periodic Fibonacci numbers [5].

This article investigates the norms of vectors and matrices composed of Fibonacci numbers. Building upon previous studies in this area [69], we examine their theoretical underpinnings and derive several key properties. The principal contribution is a comprehensive analysis of the behavior of Fibonacci vector and matrix p -norms as the parameter p varies. In particular, we derive a closed-form expression for the value of p that minimizes the difference between the p -norm and the infinity norm, allowing for an arbitrarily small discrepancy.

Furthermore, we introduce a novel class of symmetric k -Fibonacci matrices and propose a reorganization technique that significantly simplifies the computation of their p -norms. To build a k -Fibonacci matrix, we rely on the concept of k -Fibonacci sequence { g ( k ) n } defined as follows [6]:

(3) g ( k ) 1 = = g ( k ) k 2 = 0 , g ( k ) k 1 = g ( k ) k = 1

and for n > k 2 :

(4) g ( k ) n = g ( k ) n 1 + g ( k ) n 2 + + g ( k ) n k .

The k -Fibonacci sequence reduces to the Fibonacci sequence when k = 2 . From the k -Fibonacci sequence, an n × n symmetric k -Fibonacci matrix Q ( k ) n = [ q ( k ) i j ] is defined [6]

(5) q ( k ) i j = q ( k ) j i = l = 1 i g l 2 , i = j , l = 1 k q i , j l , i + 1 j ,

where g ( k ) i j = 0 for j 0 .

The definition of matrix Q ( k ) n implies the presence of non- k -Fibonacci numbers. For instance, q ( 2 ) 33 = l = 1 3 g l 2 = g 1 2 + g 2 2 + g 3 2 = 1 2 + 1 2 + 2 2 = 6 , which is not a Fibonacci number. To solve this limitation, we propose the definition of a new n × n   S -type symmetric k -Fibonacci matrix, denoted by S ( k ) n , to ensure that all matrix elements are k -Fibonacci numbers and each element is the sum of k previous elements in rows and columns. By reorganizing the elements of S ( 2 ) n , we show a triangular structure of Fibonacci numbers with a clear pattern that simplifies the computation of its p -norm. Several other properties are also discussed.

The implications of our findings are twofold. First, exploring norms in the context of Fibonacci-based structures yields theoretical insights and potential applications in number theory. Second, the ability to approximate the infinity norm through an optimally chosen p -norm may enhance algorithmic efficiency in numerical computations. Additionally, introducing symmetric k -Fibonacci matrices provides a new framework for simplifying norm evaluations in structured matrix analysis.

This article is structured as follows. Section 2 provides useful background on Fibonacci numbers and k -Fibonacci number. After a general definition of norm and p -norm, Sections 3 and 4 describe a number of properties involving, respectively, Fibonacci vector and matrix p -norms. Section 5 relies on vector p -norms to introduce additional results on distances between Fibonacci vectors, and Section 6 concludes describing natural extensions of this work.

2 Useful background

The Fibonacci sequence F n is defined as:

(6) F 1 = F 2 = 1 and, for n > 2 , F n = F n 1 + F n 2 .

F n is called the n th Fibonacci number, and the Fibonacci sequence is

(7) ( F 0 0 ) , 1 , 1 , 2 , 3 , 5 8 , 13 , 21 , 34 , 55 , 89 , 144 ,

A closed-form expression for the n th Fibonacci number is given by the Binet formula [10] involving the golden ratio φ :

(8) F n = φ n + ( φ ) n 5 = φ n + ( 1 φ ) n 5 .

The sum of the first n Fibonacci numbers is [11]

(9) i = 1 n F n = F n + 2 1 .

The sum of the squares of the first n Fibonacci numbers is [11]

(10) i = 1 n F n 2 = F n F n + 1 .

Finally, the sum of the cubes of the first n Fibonacci numbers is [11]

(11) i = 1 n F n 3 = 1 2 ( F n F n + 1 2 + ( 1 ) n F n 1 + 1 ) .

Generalized k -Fibonacci numbers were studied in [68] with alternative definitions. The k -Fibonacci sequence { g ( k ) n } is defined in [6] as

(12) g ( k ) 1 = = g ( k ) k 2 = 0 , g ( k ) k 1 = g ( k ) k = 1

and for n > k 2 :

(13) g ( k ) n = g ( k ) n 1 + g ( k ) n 2 + + g ( k ) n k

that reduces to the Fibonacci sequence when k = 2 . From this k -Fibonacci sequence, two types of Fibonacci matrices were also introduced in [6]. First, an n × n k -Fibonacci matrix ( k ) n = [ f ( k ) i j ] is defined as

(14) f ( k ) i j = g i j + 1 i j + 1 0 0 i j + 1 < 0 .

This definition places consecutive k -Fibonacci numbers in a lower triangular matrix form. This matrix is useful to find consecutive k -Fibonacci numbers from the first to the n th k -Fibonacci number. An example of a 2-Fibonacci matrix of order 5 is

(15) ( 2 ) 5 = 1 0 0 0 0 1 1 0 0 0 2 1 1 0 0 3 2 1 1 0 5 3 2 1 1 .

Second, an n × n symmetric k -Fibonacci matrix Q ( k ) n = [ q ( k ) i j ] is defined as

(16) q ( k ) i j = q ( k ) j i = l = 1 i g l 2 , i = j , l = 1 k q i , j l , i + 1 j ,

where g ( k ) i j = 0 for j 0 . An example of a 2-Fibonacci symmetric matrix of order 5 is

(17) Q ( 2 ) 5 = 1 1 2 3 5 1 2 3 5 8 2 3 6 9 15 3 5 9 15 24 5 8 15 24 40 .

This definition implies the presence of non- k -Fibonacci numbers such as 6, 9, 15, 24, and 40 in the previous example.

3 Fibonacci vector p -norms

Before discussing Fibonacci vector p -norms, let us first define norms:

Definition 1

Norm  [1]. Let V be an n -dimensional vector space over the field of real numbers R . Function : V R is a norm if for all x , y V , and all c R :

  • Non-negativity: x 0 .

  • Positivity: x = 0 x = 0 n , where 0 n is an n -dimensional vector of zeros.

  • Homogeneity: c x = c x .

  • Triangle inequality: x + y x + y .

A special class of norms is the p -norm, denoted by x p for any vector x = ( x 1 , x 2 , , x n ) , and defined as follows:

(18) x p = i = 1 n x i p 1 p .

Consider an n -dimensional Fibonacci vector by extracting the first column vector of matrices ( 2 ) n or Q ( 2 ) n , denoted by q n = ( F 1 , F 2 , , F n ) . Then, its p -norm is

(19) q n p = i = 1 n F i p 1 p .

In what follows, we derive several properties from basic identities described in Section 2:

  1. q n p > 0 for n 1 ,

  2. q n 1 = i = 1 n F i = F n + 2 1 ,

  3. q n 2 2 = i = 1 n F i 2 = F n F n + 1 ,

  4. q n 3 3 = i = 1 n F i 3 = 1 2 ( F n F n + 1 2 + ( 1 ) n F n 1 1 ) ,

  5. q n = lim p i = 1 n F i p 1 p = max { F 1 , F 2 , , F n } = F n ,

  6. q n = lim p i = 1 n F i p 1 p = min { F 1 , F 2 , , F n } = F 1 ,

  7. q n 1 = i = 1 n 1 F i 1 = 5 i = 1 n 1 φ i ( 1 φ ) i 1 ,

  8. q n 0 n = i = 1 n F i .

By focusing on the value of p that places the difference between the p -norm and the infinite norm below a given threshold, we derive the following result:

Theorem 1

Given q n , there exists some p < such that q n p q n ε for some value ε > 0 . The threshold value of p is given by

(20) p ln n ln ( ε F n + 1 ) .

Proof

Recall Hölder’s inequality [12,13] in R n and assume that r = s p > 1 with s and p in the open interval [ 1 , ] . Then, we have

(21) i = 1 n a i b i i = 1 n a i r 1 r i = 1 n b i r r 1 1 1 r .

Apply to the case a i = q i p and b i = 1 :

(22) i = 1 n q i p i = 1 n ( q i p ) s p p s i = 1 n 1 s s p 1 p s = i = 1 n q i s p s n 1 p s .

Raise both sides of the inequality to the ( 1 p ) th power and simplify:

(23) i = 1 n q i p 1 p i = 1 n q i s p s n 1 p s 1 p .

Reorganize the terms to establish the relation between a p -norm and s -norm:

(24) q n p n 1 p 1 s q n s .

Set s = and subtract q n from both sides of the inequality:

(25) q n p q n n 1 p q n q n ε .

Apply Property 5:

(26) n 1 p F n F n ε .

Taking natural logarithms, we find the threshold value for p :

(27) ln n 1 p ln ( ε F n + 1 )

(28)□ p ln n ln ( ε F n + 1 ) .

From inequality equation (24), two additional properties are derived:

  1. q n p q n s p < s ,

  2. q n p is decreasing in p .

Let us focus now on r -dimensional Fibonacci vectors to define an ( n , r ) -Fibonacci vector as

(29) q n , r = ( F n + 1 , F n + 2 , , F n + r ) .

Along the lines of properties (1)–(10), different values of p lead to the following properties for n , r 1 :

  1. q n , r p > 0 ,

  2. q n , r 1 = q n + r 1 q n 1 = F n + r + 2 F n + 2 ,

  3. q n , r 2 2 = q n + r 2 2 q n 2 2 = F n + r F n + r + 1 F n F n + 1 ,

  4. q n , r 3 3 = q n + r 3 3 q n 3 3 = 1 2 ( F n + r F n + r + 1 2 + ( 1 ) n + r F n + r 1 1 ) 1 2 ( F n F n + 1 2 + ( 1 ) n F n 1 1 ) ,

  5. q n , r 1 = 5 i = n + 1 n + r 1 φ i ( 1 φ ) i 1 ,

  6. q n , r = F n + r ,

  7. q n , r = F n + 1 ,

  8. q n , r 0 n = i = n + 1 n + r F i ,

  9. q n , r p q n , r s p < s ,

  10. q n , r p is decreasing in p .

4 Fibonacci matrix p -norms

Given matrix A of size m × n , let us consider an entry-wise matrix norm defined as follows:

(30) A p = vec ( A ) p = i = 1 m j = 1 n a i j p 1 p ,

where vec ( A ) is a vectorization function of matrix A that produces a vector v of m n elements obtained by arranging the elements of A in row-major order, i.e., by arranging them sequentially row by row. Formally, v n ( i 1 ) + j = a i j , where a i j is the ( i , j ) -entry of matrix A. Note that when p = 2 , A 2 is the Frobenius matrix norm.

Consider the 2-Fibonacci matrix of order n as defined in the introduction [6]:

(31) ( 2 ) n = F 1 0 0 0 0 F 2 F 1 0 0 0 F 3 F 2 F 1 0 F n F n 1 F n 2 F 1 .

Note that ( 2 ) n is built from the concatenation of n vectors q i with i { 1 , , n } . Then, p -norm of ( 2 ) n is given by

(32) ( 2 ) n p p = i = 1 n q i p p .

Different values of p lead to the following properties:

  1. ( 2 ) n 1 = i = 1 n q i 1 = i = 1 n ( F i + 2 1 ) = q 2 , n + 2 1 n ,

  2. ( 2 ) n 2 2 = i = 1 n q i 2 2 = i = 1 n F i F i + 1 ,

  3. ( 2 ) n 3 3 = i = 1 n q i 3 3 = 1 2 i = 1 n ( F i F i + 1 2 + ( 1 ) i F i 1 1 ) ,

  4. ( 2 ) n = F n ,

  5. ( 2 ) n = 0 ,

  6. ( 2 ) n 1 = ,

  7. ( 2 ) n 0 n = 0 .

A limitation of the symmetric k -Fibonacci matrix Q ( k ) n = [ q ( k ) i j ] described in [6] is that it cannot be fully represented by k -Fibonacci numbers. Let us define a new n × n   S -type symmetric k -Fibonacci matrix, denoted by S ( k ) n = [ s ( k ) i j ] , and defined as

(33) s ( k ) i j = s ( k ) j i = g ( k ) i + j 1 .

This definition ensures that all matrix elements are k -Fibonacci numbers and each element is the sum of k preceding elements in rows and columns. Then, a 2-Fibonacci symmetric matrix of order n is

(34) S ( 2 ) n = F 1 F 2 F 3 F n F 2 F 3 F 4 F n + 1 F 3 F 4 F 5 F n + 2 F n F n + 1 F n + 2 F 2 n 1 .

Reorganizing the elements of S ( 2 ) n leads to a triangular structure with a clear pattern:

(35) S * ( 2 ) n = F 1 0 0 0 F 2 F 2 0 0 F 3 F 3 F 3 0 F n 1 F n 1 F n 1 0 F n F n F n F n F n + 1 F n + 1 F n + 1 0 F 2 n 2 F 2 n 2 0 0 0 F 2 n 1 0 0 0 0 .

An example of this reorganization for the elements of S ( 2 ) 5 is shown in Table 1. Note that the sum of the entries of the i th row in the table is ( 5 5 i ) F i , where F i is the i th Fibonacci number. By induction, for matrix S ( 2 ) n of order n , the sum of the elements of the i th row is ( n n i ) F i . Analogously, the sum of the squared entries of the i th row is ( 5 5 i ) F i 2 . And the product of the entries of the i th row equals F i 5 5 i . The totals of the last three columns of Table 1 correspond to the norms S ( 2 ) 5 , S ( 2 ) 5 2 2 , S ( 2 ) 5 0 5 .

Table 1

Reorganization of S ( 2 ) 5 , sum of entries and squared entries, and product of entries

Row i Entry a i j j a i j j a i j 2 j a i j
1 1 1 1 1
2 1 1 2 2 1
3 2 2 2 6 12 8
4 3 3 3 3 12 36 81
5 5 5 5 5 5 25 125 3125
6 8 8 8 8 32 256 4096
7 13 13 13 39 507 2197
8 21 21 42 882 441
9 34 34 1156 34
Totals 193 2977 9984

Another example of this reorganization for the elements of S ( 3 ) 6 is shown in Table 2. Note that the structure of the reorganization and the emerging pattern that allows for easy computation of norms is independent of k . In other words, the reorganization in equation (35) is valid for any k -Fibonacci matrix S ( k ) n , provided that at least 2 n 1 elements of the sequence are defined. This property leads to the following result for the p -norm of any S ( k ) n matrix:

(36) S ( k ) n p p = i = 1 2 n 1 ( n n i ) F i p .

Table 2

Reorganization of S ( 3 ) 6 , sum of entries and squared entries, and product of entries

Row i Entry a i j j a i j j a i j 2 j a i j
1 1 1 1 1
2 1 1 2 2 1
3 2 2 2 6 12 8
4 4 4 4 4 16 64 256
5 7 7 7 7 7 35 245 16807
6 13 13 13 13 13 13 78 1014 4826809
7 24 24 24 24 24 120 2880 7962624
8 44 44 44 44 176 7744 3748096
9 81 81 81 243 19683 531441
10 149 149 298 44402 22201
11 274 274 75076 274
Totals 1249 151123 17108518

Without loss of generality by assuming that F i represents a general k -Fibonacci number, we set p to different values to derive the following S ( k ) n p p norm properties:

  1. S ( k ) n 1 = i = 1 2 n 1 ( n n i ) F i ,

  2. S ( k ) n 2 2 = i = 1 2 n 1 ( n n i ) F i 2 ,

  3. S ( k ) n 3 3 = i = 1 2 n 1 ( n n i ) F i 3 ,

  4. S ( k ) n = F 2 n 1 ,

  5. S ( k ) n = F 1 ,

  6. S ( k ) n 1 = i = 1 2 n 1 ( n n i ) F i 1 ,

  7. S ( k ) n 0 n = i = 1 2 n 1 F i n n i .

Summarizing, the main motivation to propose S ( k ) n is to produce a symmetric matrix with the desired property of ensuring that all entries are Fibonacci numbers. In addition to its concise definition, the main implication is the advantage of computing matrix norms using simple closed-form expressions, as shown in Properties 29–34. These expressions stem from a key reorganization step that allows for the detection of clear patterns in the structure of the proposed matrices disregarding the value of k .

5 Distances between vectors and matrices

When considering two vectors (matrices) of the same size, the p -norm of the difference of the two vectors (matrices) implies a p -distance between them. To provide a general p -distance definition that applies to vectors and matrices, it is convenient to transform matrices into vectors through the vectorization operator defined in Section 4. Then, the p -distance between two n -dimensional Fibonacci vectors x and y is defined as:

Definition 2

Given x , y F ( k ) n , where F ( k ) n denotes the set of all k -Fibonacci vectors of size n , the p -distance between x and y is defined as

(37) x y p = i = 1 n x i y i p 1 p .

Consider two ( n , r ) -Fibonacci vectors whose elements are separated by d positions in the sequence x = q n + d , r and y = q n , r . Then

(38) x y = ( F n + d + 1 F n + 1 , F n + d + 2 F n + 2 , , F n + d + r F n + r )

and

(39) x y p p = ( F n + d + 1 F n + 1 ) p + ( F n + d + 2 F n + 2 ) p + + ( F n + d + r F n + r ) p .

From the fundamental identity of Fibonacci numbers F n + 1 F n 1 = F n , for d = 2 , we have

(40) x y p p ( d = 2 ) = F n + 2 p + F n + 3 p + + F n + r + 1 p = i = 1 r F n + i + 1 p .

Setting d = 3 implies that F n + 4 F n + 1 = F 3 F n + 2 and F n + 3 + r F n + r = F 3 F n + r + 1 , leading to

(41) x y p p ( d = 3 ) = ( F 3 F n + 2 ) p + + ( F 3 F n + r + 1 ) p = F 3 p i = 1 r F n + i + 1 p .

Consider now the sum and the difference of two ( n , r ) -Fibonacci vectors whose elements are separated by d positions in the sequence:

(42) x + y = ( F n + d + 1 + F n + 1 , F n + d + 2 + F n + 2 , , F n + d + r + F n + r )

(43) x y = ( F n + d + 1 F n + 1 , F n + d + 2 F n + 2 , , F n + d + r F n + r ) .

Then, the addition of the 1-norms of the sum and difference vectors is

(44) x + y + x y = 2 ( F n + d + 1 + + F n + d + r ) = 2 ( F n + r + d + 2 F n + d + 2 )

Similarly, using the parallelogram law in inner product spaces for 2-norms, we have

(45) x + y 2 2 + x y 2 2 = 2 ( x 2 2 + y 2 2 )

(46) x 2 2 = F n + r + d F n + r + d + 1 F n + d F n + d + 1

(47) y 2 2 = F n + r F n + r + 1 F n F n + 1

(48) 2 ( x 2 2 + y 2 2 ) = 2 ( F n + r + d F n + r + d + 1 F n + d F n + d + 1 + F n + r F n + r + 1 F n F n + 1 ) .

By considering the golden ratio,

(49) lim n F n + 1 F n = φ

we can approximate the product of two consecutive Fibonacci numbers through

(50) F n F n + 1 φ F n 2

to further simplify the addition of the 2-norms of the sum and difference of ( n , r ) -Fibonacci vectors whose elements are separated by d positions in the sequence:

(51) x + y 2 2 + x y 2 2 = 2 ( x 2 2 + y 2 2 ) 2 φ ( F n + r + d 2 F n + d 2 + F n + r 2 F n 2 ) .

6 Conclusions

By defining a p -norm over the set of vectors and matrices populated with Fibonacci numbers, several essential properties are derived by varying parameter p . Given the decreasing character of the difference of p -norms as p increases, a closed-form expression is given to obtain the value of p that makes the difference between the p -norm and the infinite norm as small as needed. A new symmetric k -Fibonacci matrix is defined, and a reorganization of its elements leads to a pattern that simplifies the computation of its p -norms. The analysis of p -distances between same-sized vectors (matrices) is illustrated by specific examples when the elements are separated by two and three positions in the sequence.

The proposed symmetric k -Fibonacci matrix represents an extension of the work by [6] ensuring that all entries are k -Fibonacci numbers. Connecting with the main topic of this article, the advantage of this new class of matrices is the possibility to compute norms through a closed-form expression derived from a key reorganization of its elements. Acknowledging that the generalization of the results in this article for the S ( k ) class of matrix to the ( k ) and Q ( k ) classes is not a trivial question because of the different structures derived from their definition, we consider that this research question represents an interesting future line of research.

Acknowledgments

The authors are deeply grateful to the reviewers for their valuable comments that improved the manuscript.

  1. Funding information: This work was supported by AFE-Edutainment at the Universitat Politènica de València (www.afe.webs.upv.es).

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and consented to its submission to the journal, reviewed all the results, and approved the final version of the manuscript. All authors contributed equally in this work.

  3. Conflict of interest: The authors state no conflict of interest.

  4. Data availability statement: No datasets were generated or analyzed during the current study.

References

[1] R. A. Horn and C. R. Johnson, Matrix analysis, Cambridge University Press, Cambridge, 2012. Search in Google Scholar

[2] C. Kızılateş and N. Terzioğlu, On r-min and r-max matrices, J. Appl. Math. Comput. 68 (2022), no. 6, 4559–4588. 10.1007/s12190-022-01717-ySearch in Google Scholar

[3] M. Anđelić, C. M. Da Fonseca, C. Kızılateş, and N. Terzioğlu, r-min and r-max matrices with harmonic higher order Gauss Fibonacci numbers entries, J. Appl. Math. Comput. (2025), 1–25. 10.1007/s12190-025-02530-zSearch in Google Scholar

[4] E. Andrade, D. Carrasco-Olivera, and C. Manzaneda, On circulant-like matrices properties involving Horadam, Fibonacci, Jacobsthal and Pell numbers, Linear Algebra Appl. 617 (2021), 100–120. 10.1016/j.laa.2021.01.016Search in Google Scholar

[5] B. Shi and C. Kızılateş, An algorithm for complex factorization of the bi-periodic Fibonacci and Lucas polynomials, Notes Number Theory Discret Math. 31 (2025), no. 2, 269–279. 10.7546/nntdm.2025.31.2.269-279Search in Google Scholar

[6] G.-Y. Lee and J.-S. Kim, The linear algebra of the k-Fibonacci matrix, Linear Algebra Appl. 373 (2003), 75–87. 10.1016/S0024-3795(02)00596-7Search in Google Scholar

[7] S. Falcón and A. Plaza, On the Fibonacci k-numbers, Chaos Solitons Fractals 32 (2007), no. 5, 1615–1624. 10.1016/j.chaos.2006.09.022Search in Google Scholar

[8] S. Falcon and A. Plaza, The k-Fibonacci sequence and the Pascal 2-triangle, Chaos Solitons Fractals 33 (2007), no. 1, 38–49. 10.1016/j.chaos.2006.10.022Search in Google Scholar

[9] S. Falcon, The k-Fibonacci matrix and the Pascal matrix, Open Math. 9 (2011), no. 6, 1403–1410. 10.2478/s11533-011-0089-9Search in Google Scholar

[10] T. Koshy, Fibonacci and Lucas Numbers with Applications, John Wiley & Sons, Hoboken, 2019. 10.1002/9781118742297Search in Google Scholar

[11] A. T. Benjamin and J. J. Quinn, Proofs that really count: the art of combinatorial proof, American Mathematical Society, Washington, 2003. 10.5948/9781614442080Search in Google Scholar

[12] O. Hölder, Ueber einen Mittelwertsatz, Nachrichten von der Königlichen Gesellschaft der Wissenschaften und der Georg-Augusts-Universitaaat zu Göttingen, 1889, pp. 38–47. Search in Google Scholar

[13] L. Maligranda, Why Hölder’s inequality should be called Rogers’ inequality, Math. Inequal. Appl. 1 (1998), no. 1, 69–83. 10.7153/mia-01-05Search in Google Scholar

Received: 2025-02-28
Revised: 2025-08-04
Accepted: 2025-08-20
Published Online: 2025-10-09

© 2025 the author(s), published by De Gruyter

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

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  39. On a subclass of multivalent functions defined by generalized multiplier transformation
  40. Singular direction of meromorphic functions with finite logarithmic order
  41. Growth theorems and coefficient bounds for g-starlike mappings of complex order λ
  42. Refinements of inequalities on extremal problems of polynomials
  43. Control Theory and Optimization
  44. Averaging method in optimal control problems for integro-differential equations
  45. On superstability of derivations in Banach algebras
  46. The robust isolated calmness of spectral norm regularized convex matrix optimization problems
  47. Observability on the classes of non-nilpotent solvable three-dimensional Lie groups
  48. Differential Equations
  49. The ill-posedness of the (non-)periodic traveling wave solution for the deformed continuous Heisenberg spin equation
  50. A note on the global existence and boundedness of an N-dimensional parabolic-elliptic predator-prey system with indirect pursuit-evasion interaction
  51. Blow-up of solutions for Euler-Bernoulli equation with nonlinear time delay
  52. Periodic or homoclinic orbit bifurcated from a heteroclinic loop for high-dimensional systems
  53. Regularity of weak solutions to the 3D stationary tropical climate model
  54. Local minimizers for the NLS equation with localized nonlinearity on noncompact metric graphs
  55. Global existence and blow-up of solutions to pseudo-parabolic equation for Baouendi-Grushin operator
  56. Bubbles clustered inside for almost-critical problems
  57. Existence and multiplicity of positive solutions for multiparameter periodic systems
  58. Existence of positive periodic solutions for evolution equations with delay in ordered Banach spaces
  59. On a nonlinear boundary value problems with impulse action
  60. Normalized ground-states for the Sobolev critical Kirchhoff equation with at least mass critical growth
  61. Multiple positive solutions to a p-Kirchhoff equation with logarithmic terms and concave terms
  62. Infinitely many solutions for a class of Kirchhoff-type equations
  63. Real and non-real eigenvalues of regular indefinite Sturm–Liouville problems
  64. Existence of global solutions to a semilinear thermoelastic system in three dimensions
  65. Limiting profile of positive solutions to heterogeneous elliptic BVPs with nonlinear flux decaying to negative infinity on a portion of the boundary
  66. Morse index of circular solutions for repulsive central force problems on surfaces
  67. Differential Geometry
  68. On tangent bundles of Walker four-manifolds
  69. Pedal and negative pedal surfaces of framed curves in the Euclidean 3-space
  70. Discrete Mathematics
  71. Eventually monotonic solutions of the generalized Fibonacci equations
  72. Dynamical Systems Ergodic Theory
  73. Dynamical properties of two-diffusion SIR epidemic model with Markovian switching
  74. A note on weighted measure-theoretic pressure
  75. Pullback attractors for a class of second-order delay evolution equations with dispersive and dissipative terms on unbounded domain
  76. Pullback attractor of the 2D non-autonomous magneto-micropolar fluid equations
  77. Functional Analysis
  78. Spectrum boundary domination of semiregularities in Banach algebras
  79. Approximate multi-Cauchy mappings on certain groupoids
  80. Investigating the modified UO-iteration process in Banach spaces by a digraph
  81. Tilings, sub-tilings, and spectral sets on p-adic space
  82. Continuity and essential norm of operators defined by infinite tridiagonal matrices in weighted Orlicz and l spaces
  83. A family of commuting contraction semigroups on l 1 ( N ) and l ( N )
  84. q-Stirling sequence spaces associated with q-Bell numbers
  85. Chlodowsky variant of Bernstein-type operators on the domain
  86. Hyponormality on a weighted Bergman space of an annulus with a general harmonic symbol
  87. Characterization of derivations on strongly double triangle subspace lattice algebras by local actions
  88. Fixed point approaches to the stability of Jensen’s functional equation
  89. Geometry
  90. The regularity of solutions to the Lp Gauss image problem
  91. Solving the quartic by conics
  92. Group Theory
  93. On a question of permutation groups acting on the power set
  94. A characterization of the translational hull of a weakly type B semigroup with E-properties
  95. Harmonic Analysis
  96. Eigenfunctions on an infinite Schrödinger network
  97. Maximal function and generalized fractional integral operators on the weighted Orlicz-Lorentz-Morrey spaces
  98. Subharmonic functions and associated measures in ℝn
  99. Mathematical Logic, Model Theory and Foundation
  100. A topology related to implication and upsets on a bounded BCK-algebra
  101. Boundedness of fractional sublinear operators on weighted grand Herz-Morrey spaces with variable exponents
  102. Number Theory
  103. Fibonacci vector and matrix p-norms
  104. Recurrence for probabilistic extension of Dowling polynomials
  105. Carmichael numbers composed of Piatetski-Shapiro primes in Beatty sequences
  106. The number of rational points of some classes of algebraic varieties over finite fields
  107. Classification and irreducibility of a class of integer polynomials
  108. Decompositions of the extended Selberg class functions
  109. Joint approximation of analytic functions by the shifts of Hurwitz zeta-functions in short intervals
  110. Fibonacci Cartan and Lucas Cartan numbers
  111. Recurrence relations satisfied by some arithmetic groups
  112. The hybrid power mean involving the Kloosterman sums and Dedekind sums
  113. Numerical Methods
  114. A modified predictor–corrector scheme with graded mesh for numerical solutions of nonlinear Ψ-caputo fractional-order systems
  115. A kind of univariate improved Shepard-Euler operators
  116. Probability and Statistics
  117. Statistical inference and data analysis of the record-based transmuted Burr X model
  118. Multiple G-Stratonovich integral in G-expectation space
  119. p-variation and Chung's LIL of sub-bifractional Brownian motion and applications
  120. Real Analysis
  121. Chebyshev polynomials of the first kind and the univariate Lommel function: Integral representations
  122. Multiple solutions for a class of fourth-order elliptic equations with critical growth
  123. Majorization-type inequalities for (m, M, ψ)-convex functions with applications
  124. The evaluation of a definite integral by the method of brackets illustrating its flexibility
  125. Some new Fejér type inequalities for (h, g; α - m)-convex functions
  126. Some new Hermite-Hadamard type inequalities for product of strongly h-convex functions on ellipsoids and balls
  127. Topology
  128. Unraveling chaos: A topological analysis of simplicial homology groups and their foldings
  129. A generalized fixed-point theorem for set-valued mappings in b-metric spaces
  130. On SI2-convergence in T0-spaces
  131. Generalized quandle polynomials and their applications to stuquandles, stuck links, and RNA folding
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