Home Mathematics On a generalization of derangement polynomials and numbers
Article Open Access

On a generalization of derangement polynomials and numbers

  • and EMAIL logo
Published/Copyright: December 2, 2025
Become an author with De Gruyter Brill

Abstract

In T. Kim, D. S. Kim, and D. V. Dolgy, Probabilistic derangement numbers and polynomials, Math. Comput. Model. Dyn. Syst. 31 (2025), no. 1, 2529188, Kim-Kim defined the probabilistic derangement polynomials and numbers and found some properties of those polynomials and numbers. In this paper, we define another probabilistic derangement polynomials which are different from the one defined by Kim-Kim, and find explicit formulas and interesting identities of Stirling numbers of the first and the second kind, Bell polynomials, Fubini polynomials, Stirling numbers of the first and the second kind and those polynomials and numbers.

MSC 2020: 05A10; 05A15; 11B73; 11B83; 60C05

1 Introduction

Let X be a set with n elements, say X = 1,2 , , n . A permutation of X with no fixed point is called a derangement, and the number of derangements of X is called the nth derangement number and denoted by D n . By the inclusion-exclusion principle, the nth derangement number is (see [1], [2], [3], [4])

(1.1) D n = n ! k = 0 n ( 1 ) k k ! .

By (1.1), we see the generating function of the derangement numbers are (see [1], [2], [3], [4])

(1.2) n = 0 D n t n n ! = 1 1 t e t .

As a natural extension, the derangement polynomials are defined by the generating function to be (see [5], [6], [7])

(1.3) n = 0 D n ( x ) t n n ! = 1 1 t e ( x 1 ) t .

When x = 0, D n (0) = D n is the nth derangement numbers.

The derangement numbers and polynomials are interesting things in the special function theory, combinatorics, applied mathematics. In [8], Garsia-Remmel generalized the derangement numbers to the q-derangement numbers, and Clarke-Sved found a relationship between Bell numbers and derangement numbers in [9]. Briggs-Remmel defined the p, q-analogue of the derangement numbers, extending some work of Garsia and Remmel and showed that these p, q-analogues satisfy recurrences that naturally extend the classical recurrences for the derangement numbers (see [10]). In [7], Kim-Kim-Lee-Jang defined the degenerate version of the derangement polynomials and found some interesting identities of those polynomials and numbers, and Kim-Kim defined the probabilistic derangement polynomials which was a generalization of those polynomials and derived some properties of those polynomials and numbers (see [11]).

From now on, we list some important numbers or polynomials in the combinatorics that we will need for this paper.

For nonzero integers n and k with nk, the Stirling numbers of the first kind and the second kind S 1(n, k), S 2(n, k), respectively, are defined by generating function to be (see [2],12])

(1.4) ( x ) n = k = 0 n S 1 ( n , k ) x k  and  x n = k = 0 n S 2 ( n , k ) ( x ) k ,

where (x)0 = 1, (x) n = x(x − 1)…(xn + 1), (n ≥ 1).

By (1.4), we see that for each nonnegative integer k,

1 k ! log ( 1 + t ) k = l = k S 1 ( l , k ) t l l !  and  1 k ! e t 1 k = l = k S 2 ( l , k ) t l l ! ,

(see [2],12]).

The Bell polynomials are defined by the generating function to be (see [12])

e x e t 1 = n = 0 B e l n ( x ) t n n ! .

In the special case x = 1, Bel n = Bel n (1) are called the Bell numbers which counts the possible partitions of given set with n elements.

The Fubini polynomials are defined as follows (see [13]):

1 1 x e t 1 = n = 0 F n ( x ) t n n ! .

When x = 1, F n = F n (1) are called the Fubini numbers which counts the ordered partitions of a set with n elements.

For λ ≠ 0, the Apostol-Bernoulli polynomials are defined by the generating function to be (see [14],15])

t λ e t 1 e x t = n = 0 B n ( x | λ ) t n n ! .

In the special case x = 0, B n (λ) = B n (0|λ) are called the Apostol-Bernoulli numbers. Note that if we put λ = 1, then B n (x|λ) = B n (x) are the B. polynomials. By the definition of Apostol-Bernoulli polynomials, if λ ≠ 1, then we see that B 0(x|λ) = 0, B 1 ( x | λ ) = 1 λ 1 .

Let Y be a random variable with the moment generating function of Y.

(1.5) E e Y t = n = 0 E Y n t n n ! , ( | t | < r )

exists for some r > 0 (see [11],16]). Note that if Y = 1, then E e Y t = e t .

The Poisson random variable indicates how many events occurred within a given period of time. A random variable Y, taking on one of the values 0, 1, 2…, is said to be the Poisson random variable with parameter α > 0, if the probability mass function of Y is given by (see [17],18])

p ( X = i ) = p ( i ) = e α α i i ! .

In [16], Adell-B e ́ nyi defined the probabilistic Stirling numbers of the first kind associated with random variable Y and the second kind S 1 Y ( n , k ) and S 2 Y ( n , k ) , respectively as follows:

(1.6) 1 k ! log E e Y t k = n = k ( 1 ) n k S 1 Y ( n , k ) t n n ! ,

(1.7) 1 k ! E e Y t 1 k = n = k S 2 Y ( n , k ) t n n ! ,

where n, k are nonnegative integers with nk ≥ 0.

In this paper, we defined the probabilistic derangement polynomials and numbers which are different from the one defined by Kim-Kim, and find relationships between probabilistic Stirling numbers of the first and the second kind, Stirling numbers of the first and the second kind, Bell polynomials, Fubini polynomials and those polynomials and numbers. In addition, we give some explicit formulas of those polynomials and numbers.

2 Probabilistic derangement polynomials and numbers

Throughout this paper, let Y be a random variable with the moment generating function of Y (1.5).

In viewpoint of (1.6) or (1.7), we define the probabilistic derangement polynomials as follows:

(2.1) e x t 1 log E e Y t E e Y t = n = 0 d n Y ( x ) t n n ! .

When x = 0, d n Y = d n Y ( 0 ) are called the probabilistic derangement numbers. Note that if we put Y = 1, then d n Y ( x ) = D n ( x ) .

By (2.1), we see that.

(2.2) e x t 1 log E e Y t E e Y t = n = 0 d n Y t n n ! n = 0 x n t n n ! = n = 0 m = 0 n n m d n m Y x m t n n ! .

In addition,

(2.3) n = 0 d n Y ( x ) t n n ! = E e Y t 1 log E e Y t e x t = n = 0 log E e Y t n E e ( x Y ) t = n = 0 n ! 1 n ! log E e Y t n E e ( x Y ) t = n = 0 m = 0 n m ! ( 1 ) n m S 1 Y ( n , m ) t n n ! n = 0 E ( x Y ) n t n n ! = n = 0 a = 0 n m = 0 a n a ( 1 ) a m m ! S 1 Y ( a , m ) E ( x Y ) n a t n n ! ,

when log E e Y t < 1 . By (2.2) and (2.3), we obtain the following theorem.

Theorem 2.1.

For each nonnegative integer n, we have

d n Y ( x ) = m = 0 n n m d n m Y x m = a = 0 n m = 0 a n a ( 1 ) a m m ! S 1 Y ( a , m ) E ( x Y ) n a .

Note that, by (1.7), we get.

(2.4) log E e Y t = n = 1 ( 1 ) n + 1 E e Y t 1 n n = n = 1 ( 1 ) n + 1 ( n 1 ) ! l = n S 2 Y ( l , n ) t l l ! = n = 1 m = 1 n ( 1 ) m + 1 ( m 1 ) ! S 2 Y ( n , m ) t n n ! ,

where E e Y t < 1 . By (2.1) and (2.4), we have

(2.5) 1 log E e Y t n = 0 d n Y ( x ) t n n ! = n = 0 d n Y ( x ) t n n ! log E e Y t n = 0 d n Y ( x ) t n n ! = d 0 Y ( x ) + n = 1 d n Y ( x ) r = 1 n m = 1 r ( 1 ) m + 1 n r ( m 1 ) ! S 2 Y ( r , m ) d n r Y ( x ) t n n ! .

and

(2.6) e x t E e Y t = n = 0 x n t n n ! n = 0 ( 1 ) n E Y n t n n ! = n = 0 m = 0 n ( 1 ) m n m E Y m x n m t n n ! .

Hence, by (2.5) and (2.6), we obtain the following theorem.

Theorem 2.2.

For each positive integer n, we have

d n Y ( x ) = r = 1 n m = 1 r ( 1 ) m + 1 n r ( m 1 ) ! S 2 Y ( r , m ) d n r Y ( x ) + m = 0 n ( 1 ) m n m E Y m x n m .

In particular, if we put x = 0, then

( 1 ) n E Y n = d n Y r = 1 n m = 1 r ( 1 ) m + 1 n r ( m 1 ) ! S 2 Y ( r , m ) d n r Y .

Note that, by (1.6),

(2.7) n = 0 d n Y ( x ) t n n ! = e x t 1 log E e Y t E e Y t = n = 0 x n t n n ! n = 0 n ! 1 n ! log E e Y t n n = 0 ( 1 ) n E Y n t n n ! = n = 0 x n t n n ! n = 0 m = 0 n ( 1 ) n m m ! S 1 Y ( n , m ) t n n ! n = 0 ( 1 ) n E Y n t n n ! = n = 0 r = 0 n m = 0 r ( 1 ) r m n r m ! S 1 Y ( r , m ) x n r t n n ! n = 0 ( 1 ) n E Y n t n n ! = n = 0 a = 0 n r = 0 a m = 0 r ( 1 ) n a + r m n a a r m ! S 1 Y ( r , m ) E Y n a x a r t n n ! .

By (2.7), we obtain the following theorem.

Theorem 2.3.

For each nonnegative integer n, we have

d n Y ( x ) = a = 0 n r = 0 a m = 0 r ( 1 ) n a + r m n a a r m ! S 1 Y ( r , m ) E Y n a x a r .

In particular, if we put x = 0, then

d n Y = a = 0 n m = 0 a ( 1 ) n m n a m ! S 1 Y ( a , m ) E Y n a .

Note that

(2.8) E e Y t = e log E e Y t = n = 0 1 n ! log E e Y t n = n = 0 m = 0 n ( 1 ) n m S 1 Y ( n , m ) t n n ! ,

and, by (1.7), we get

(2.9) E e Y t = log e E e Y t = log e E e Y t 1 + 1 = m = 1 ( m 1 ) ! ( 1 ) m + 1 1 m ! e E e Y t 1 m = m = 1 ( 1 ) m + 1 ( m 1 ) ! l = m S 2 ( l , m ) 1 l ! E e Y t l = m = 1 ( 1 ) m + 1 ( m 1 ) ! l = m S 2 ( l , m ) 1 l ! r = 0 l ( l ) r 1 r ! E e Y t 1 r = m = 1 ( 1 ) m + 1 ( m 1 ) ! l = m S 2 ( l , m ) 1 l ! r = 0 l ( l ) r a = r S 2 Y ( a , r ) t a a ! = m = 1 ( 1 ) m + 1 ( m 1 ) ! l = 0 S 2 ( l + m , m ) 1 ( l + m ) ! n = 0 r = 0 n ( l + m ) r S 2 Y ( n , r ) t n n ! = m = 1 a = 1 m ( 1 ) a + 1 ( a 1 ) ! S 2 ( m , a ) m ! n = 0 r = 0 n ( m ) r S 2 Y ( n , r ) t n n ! = n = 0 m = 1 a = 1 m r = 0 n ( 1 ) a + 1 ( a 1 ) ! S 2 ( m , a ) ( m r ) ! S 2 Y ( n , r ) t n n ! ,

when E e Y t 1 < 1 . Since E e Y t = n = 0 E Y n t n n ! , by (2.8) and (2.9), we obtain the following theorem.

Theorem 2.4.

For each nonnegative integer n, we have

E Y n = m = 0 n ( 1 ) n m S 1 Y ( n , m ) = m = 1 a = 1 m r = 0 n ( 1 ) a + 1 ( a 1 ) ! S 2 ( m , a ) ( m r ) ! S 2 Y ( n , r ) .

Let Y be the Poisson random variable with parameter α > 0. Then

(2.10) E e Y t = y e y t e α α y y ! = e α e t 1  and  E e Y t = e α e t 1 , ( see [ 17 , 18 ] ) ,

and by (2.10), we see that

(2.11) n = 0 d n Y ( x ) t n n ! = e x t 1 log E e Y t E e Y t = e x t 1 α e t 1 e α e t 1 = n = 0 x n t n n ! n = 0 α n e t 1 n n = 0 ( 1 ) n B e l n ( α ) t n n ! = n = 0 x n t n n ! n = 0 m = 0 n α m m ! S 2 ( n , m ) t n n ! n = 0 ( 1 ) n B e l n ( α ) t n n ! = n = 0 x n t n n ! n = 0 a = 0 n m = 0 a n a ( 1 ) n a α m m ! S 2 ( a , m ) B e l n a ( α ) t n n ! = n = 0 b = 0 n a = 0 b m = 0 a n b b a ( 1 ) b a α m m ! S 2 ( a , m ) B e l b a ( α ) x n b t n n ! ,

where α ( e t 1 ) < 1 . In addition, by (2.10), we know that

(2.12) e x t 1 log E e Y t E e Y t = e x t n = 0 F n ( α ) t n n ! n = 0 ( 1 ) n B e l ( α ) t n n ! = n = 0 x n t n n ! n = 0 m = 0 n n m ( 1 ) n m F m ( α ) B e l n m ( α ) t n n ! = n = 0 a = 0 n m = 0 a a m n a ( 1 ) a m F m ( α ) B e l a m ( α ) x n a t n n ! .

By (2.11) and (2.12), we obtain the following theorem.

Theorem 2.5.

Let Y be the Poisson random variable with parameter α > 0. For each nonnegative integer n, we have

d n Y ( x ) = b = 0 n a = 0 b m = 0 a n b b a ( 1 ) b a α m m ! S 2 ( a , m ) B e l b a ( α ) x n b = a = 0 n m = 0 a a m n a ( 1 ) a m F m ( α ) B e l a m ( α ) x n a .

In particular, if we put x = 0, then

d n Y = a = 0 n m = 0 a n a ( 1 ) n a α m m ! S 2 ( n , m ) B e l n a ( α ) = a = 0 n m = 0 a a m n a ( 1 ) a m F m ( α ) B e l a m ( α ) x n a .

A continuous random variable Y whose density function defined by

f ( y ) = β e β y β y α 1 Γ ( α ) , if  y 0 , 0 , if  y < 0 ,

for some α, β > 0 is called the gamma random variable with parameter α, β, and denoted by Y ∼Γ(α, β).

Let Y ∼Γ(1, 1). Then

(2.13) E e Y t = 0 e y e y t d y = 1 1 t  and  E e Y t = 0 e y e y t d y = 1 1 + t ,

and thus, by (2.13), we get

(2.14) n = 0 d n Y ( x ) t n n ! = e x t 1 log E e Y t E e Y t = e x t 1 + log ( 1 t ) 1 1 + t .

Replacing t bt 1 − e t in (2.14), we have

(2.15) e x 1 e t 1 + t 1 2 e t = 1 1 + t n = 0 ( 1 ) n B e l n ( x ) t n n ! 1 2 t n = 0 B n 1 2 t n n ! = 1 2 ( 1 + t ) n = 0 m = 0 n n m ( 1 ) n + m + 1 B m + 1 1 2 m + 1 B e l n m ( x ) t n n ! ,

and

(2.16) n = 0 d n Y ( x ) 1 n ! 1 e t n = n = 0 d n Y ( x ) ( 1 ) n l = n S 2 ( l , n ) t l l ! = n = 0 m = 0 n ( 1 ) m d m Y ( x ) S 2 ( n , m ) t n n ! .

By (2.15) and (2.16), we see that

(2.17) ( 1 + t ) n = 0 m = 0 n ( 1 ) m d m Y ( x ) S 2 ( n , m ) t n n ! = 1 2 n = 0 m = 0 n n m ( 1 ) n + m + 1 m + 1 B m + 1 1 2 B e l n m ( x ) t n n ! .

Since S 2(0, m) = S 2(m − 1, m) = 0 for each m N , by (2.17), we see that

(2.18) ( 1 + t ) n = 0 m = 0 n ( 1 ) m d m Y ( x ) S 2 ( n , m ) t n n ! = n = 0 m = 0 n ( 1 ) m d m Y ( x ) S 2 ( n , m ) t n n ! + n = 0 m = 0 n ( 1 ) m d m Y ( x ) S 2 ( n , m ) t n + 1 n ! = n = 0 m = 0 n ( 1 ) m d m Y ( x ) S 2 ( n , m ) t n n ! + n = 1 m = 0 n ( 1 ) m n S 2 ( n 1 , m ) d m Y ( x ) t n n ! = 1 + n = 1 m = 0 n ( 1 ) m S 2 ( n , m ) + n S 2 ( n 1 , m ) d m Y ( x ) t n n ! .

By (2.18), we obtain the following theorem.

Theorem 2.6.

Let Y ∼Γ(1, 1). For each positive integer n, we have

2 m = 0 n ( 1 ) m S 2 ( n , m ) + n S 2 ( n 1 , m ) d m Y ( x ) = m = 0 n n m ( 1 ) n + m + 1 m + 1 B m + 1 1 2 B e l n m ( x ) .

Let Y be Bernoulli random variable with probability success p. Then.

(2.19) E e Y t = p e t 1 + 1  and  E e Y t = p e t 1 + 1 .

and by (2.19), we see that

n = 0 d n Y ( x ) t n n ! = e x t 1 log p e t 1 p e t 1 + 1 ,

and so we have

(2.20) 1 1 + p e t 1 n = 0 d n Y ( x ) t n n ! = e x t m = 0 log p e t 1 + 1 m .

Note that

(2.21) 1 1 + p e t 1 n = 0 d n Y ( x ) t n n ! = m = 0 ( p ) m e t 1 m n = 0 d n Y ( x ) t n n ! = m = 0 ( p ) m m ! 1 m ! e t 1 m n = 0 d n Y ( x ) t n n ! = m = 0 ( p ) m m ! l = m S 2 ( l , m ) ( 1 ) l t l l ! n = 0 d n Y ( x ) t n n ! = n = 0 m = 0 n r = 0 m n m ( 1 ) m + r r ! S 2 ( m , r ) d n m Y ( x ) t n n ! ,

and

(2.22) e x t m = 0 log p e t 1 + 1 m = e x t m = 0 m ! 1 m ! log p e t 1 + 1 m = e x t m = 0 m ! l = m S 1 ( l , m ) p e t 1 l l ! = e x t m = 0 m ! l = m S 1 ( l , m ) p l r = l ( 1 ) r S 2 ( r , l ) t r r ! = n = 0 x n t n n ! n = 0 l = 0 n a = n l n ( 1 ) n p a S 1 ( a , n l ) S 2 ( n , a ) ( n l ) ! t n n ! = n = 0 b = 0 n l = 0 b a = b l b n b ( 1 ) n b p a S 1 ( a , b l ) S 2 ( b , a ) ( b l ) ! x n b t n n ! .

By (2.21) and (2.22), we obtain the following theorem.

Theorem 2.7.

Let Y be Bernoulli random variable with probability success p. For each nonnegative integer n, we have

m = 0 n r = 0 m n m ( 1 ) m + r r ! S 2 ( m , r ) d n m Y ( x ) = b = 0 n l = 0 b a = b l b n b ( 1 ) n b p a S 1 ( a , b l ) S 2 ( b , a ) ( b l ) ! x n b .

In particular, if we take x = 0, then

m = 0 n r = 0 m n m ( 1 ) m + r r ! S 2 ( m , r ) d n m Y = l = 0 n a = n l n p a S 1 ( a , n l ) S 2 ( n , a ) ( n l ) ! .


Corresponding author: Jin-Woo Park, Department of Mathematics Education, Daegu University, Gyeongsan-si, 38453, Republic of Korea, E-mail: 

Acknowledgements

The authors would like to thank the referees for their valuable and detailed comments which have significantly improved the presentation of this paper.

  1. Research funding: This research was supported by the Daegu University Research Grant, 2024.

  2. Author contributions: All authors contributed equally to this work.

  3. Conflict of interest: The authors state that there is no conflict of interest.

  4. Ethical approval: Not applicable.

  5. Data availability statement: Not applicable.

References

[1] L. Carlitz, The number of derangements of a sequence with given specification, Fibonacci Quart. 16 (1978), 255–258, https://doi.org/10.1080/00150517.1978.12430325.Search in Google Scholar

[2] L. Comtet, Advanced Combinatorics: The Art of Finite and Infinite Expansions, D. Reidel Publishing Co., Dordrecht, 1974.10.1007/978-94-010-2196-8Search in Google Scholar

[3] Z. Du and C. M. da Fonseca, An identity involving derangement numbers and Bell numbers, Appl. Anal. Discrete Math. 16 (2022), no. 2, 485–494, https://doi.org/10.2298/aadm200705010d.Search in Google Scholar

[4] J. Zhang, D. Gray, H. Wang, and X. D. Zhang, On the combinatorics of derangements and related permutations, Appl. Math. Comput. 431 (2022), 10, Paper No. 127341, https://doi.org/10.1016/j.amc.2022.127341.Search in Google Scholar

[5] H. K. Kim, Some identities of the degenerate higher order derangement polynomials and numbers, Symmetry 13 (2021), 176, https://doi.org/10.3390/sym13020176.Search in Google Scholar

[6] T. Kim, D. S. Kim, G. W. Jang, and J. Kwon, A note on some identities of derangement polynomials, J. Inequal. Appl. 2018 (2018), 40, https://doi.org/10.1186/s13660-018-1636-8.Search in Google Scholar PubMed PubMed Central

[7] T. Kim, D. S. Kim, H. Lee, and L. C. Jang, A note on degenerate derangement polynomials and numbers, AIMS Math. 6 (2021), no. 6, 6469–6481, https://doi.org/10.3934/math.2021380.Search in Google Scholar

[8] A. M. Garsia and J. Remmel, A combinatorial interpretation of q-derangement and q-Laguerre numbers, European J. Combin. 1 (1980), no. 1, 47–59, https://doi.org/10.1016/s0195-6698(80)80021-7.Search in Google Scholar

[9] R. J. Clarke and M. Sved, Derangements and Bell numbers, Math. Mag. 66 (1993), no. 5, 299–303, https://doi.org/10.1080/0025570x.1993.11996148.Search in Google Scholar

[10] K. S. Briggs and J. B. Remmel, A p,q-analogue of the generalized derangement numbers, Ann. Comb. 13 (2009), no. 1, 1–25, https://doi.org/10.1007/s00026-009-0010-4.Search in Google Scholar

[11] T. Kim, D. S. Kim, and D. V. Dolgy, Probabilistic derangement numbers and polynomials, Math. Comput. Model. Dyn. Syst. 31 (2025), no. 1, 2529188, https://doi.org/10.1080/13873954.2025.2529188.Search in Google Scholar

[12] D. S. Kim and T. Kim, Some identities of Bell polynomials, Sci. China Math. 58 (2015), no. 10, 2095–2104, https://doi.org/10.1007/s11425-015-5006-4.Search in Google Scholar

[13] L. Kargın, Some formulae for products of Fubini polynomials with applications, arXiv:1701.01023v1 [math.CA] 23. Doc., (2016).Search in Google Scholar

[14] T. M. Apostol, On the Lerch Zeta function, Pacific J. Math. 1 (1951), 161–167, https://doi.org/10.2140/pjm.1951.1.161.Search in Google Scholar

[15] Q. M. Luo, On the Apostol-Bernoulli polynomials, Cent. Eur. J. Math. 2 (2004), no. 4, 509–515, https://doi.org/10.2478/bf02475959.Search in Google Scholar

[16] J. A. Adell and B. Bényi, Probabilistic Stirling numbers and applicatiosns. Aequart. Math. 98 (2024), 1627–1646. https://doi.org/10.1007/s00010-024-01073-1.Search in Google Scholar

[17] T. Kim, D. S. Kim, D. V. Dolgy, and J. W. Park, Degenerate binomial and Poisson randomvariables associated with degenerate Lah-Bell polynomials, Open Math. 19 (2021), no. 1, 1588–1597, https://doi.org/10.1515/math-2021-0116.Search in Google Scholar

[18] S. M. Ross, Introduction to Probability Models (Twelfth Edition). Academic Press, Cambridge, MA, 2019.10.1016/B978-0-12-814346-9.00006-8Search in Google Scholar

Received: 2024-10-14
Accepted: 2025-10-16
Published Online: 2025-12-02

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

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

Articles in the same Issue

  1. Research Articles
  2. On approximation by Stancu variant of Bernstein-Durrmeyer-type operators in movable compact disks
  3. Circular n,m-rung orthopair fuzzy sets and their applications in multicriteria decision-making
  4. Grand Triebel-Lizorkin-Morrey spaces
  5. Coefficient estimates and Fekete-Szegö problem for some classes of univalent functions generalized to a complex order
  6. Proofs of two conjectures involving sums of normalized Narayana numbers
  7. On the Laguerre polynomial approximation errors and lower type of entire functions of irregular growth
  8. New convolutions for the Hartley integral transform imbedded in the Banach algebras and convolution-type integral equations
  9. Some inequalities for rational function with prescribed poles and restricted zeros
  10. Lucas difference sequence spaces defined by Orlicz function in 2-normed spaces
  11. Evaluating the efficacy of fuzzy Bayesian networks for financial risk assessment
  12. Fixed point results for contractions of polynomial type
  13. Estimation for spatial semi-functional partial linear regression model with missing response at random
  14. Investigating the controllability of differential systems with nonlinear fractional delays, characterized by the order 0 < η ≤ 1 < ζ ≤ 2
  15. New forms of bilateral inequalities for K-g-frames
  16. Rate of pole detection using Padé approximants to polynomial expansions
  17. Existence results for nonhomogeneous Choquard equation involving p-biharmonic operator and critical growth
  18. Note on the shape-preservation of a new class of Kantorovich-type operators via divided differences
  19. Geršhgorin-type theorems for Z1-eigenvalues of tensors with applications
  20. New topologies derived from the old one via operators
  21. Blow up solutions for two-dimensional semilinear elliptic problem of Liouville type with nonlinear gradient terms
  22. Infinitely many normalized solutions for Schrödinger equations with local sublinear nonlinearity
  23. Nonparametric expectile shortfall regression for functional data
  24. Advancing analytical solutions: Novel wave insights and methodologies for beta fractional Kuralay-II equations
  25. A generalized p-Laplacian problem with parameters
  26. A study of solutions for several classes of systems of complex nonlinear partial differential difference equations in ℂ2
  27. Towards finding equalities involving mixed products of the Moore-Penrose and group inverses by matrix rank methodology
  28. ω -biprojective and ω ¯ -contractible Banach algebras
  29. Coefficient functionals for Sakaguchi-type-Starlike functions subordinated to the three-leaf function
  30. Solutions of several general quadratic partial differential-difference equations in ℂ2
  31. Inequalities for the generalized trigonometric functions with respect to weighted power mean
  32. Optimization of Lagrange problem with higher-order differential inclusion and special boundary-value conditions
  33. Hankel determinants for q-starlike functions connected with q-sine function
  34. System of partial differential hemivariational inequalities involving nonlocal boundary conditions
  35. A new family of multivalent functions defined by certain forms of the quantum integral operator
  36. A matrix approach to compare BLUEs under a linear regression model and its two competing restricted models with applications
  37. Weighted composition operators on bicomplex Lorentz spaces with their characterization and properties
  38. Behavior of spatial curves under different transformations in Euclidean 4-space
  39. Commutators for the maximal and sharp functions with weighted Lipschitz functions on weighted Morrey spaces
  40. A new kind of Durrmeyer-Stancu-type operators
  41. A study of generalized Mittag-Leffler-type function of arbitrary order
  42. On the approximation of Kantorovich-type Szàsz-Charlier operators
  43. Split quaternion Fourier transforms for two-dimensional real invariant field
  44. Quantum injectivity of G-frames in Hilbert spaces
  45. Some results on disjointly weakly compact sets
  46. On Motzkin sequence spaces via q-analog and compact operators
  47. Existence and multiplicity of nontrivial solutions for Schrödinger-Bopp-Podolsky systems with critical nonlinearity in ℝ3
  48. Stability analysis of linear time-invariant difference-differential system with constant and distributed delays
  49. The discriminant of quasi m-boundary singularities
  50. Norm constrained empirical portfolio optimization with stochastic dominance: Robust optimization non-asymptotics
  51. Fuzzy stability of multi-additive mappings
  52. On inequalities involving n-polynomial exponential-type convex functions
  53. Singularities of multiplicative spherical Darboux image and multiplicative rectifying developable surface
  54. A golden ratio technique for equilibrium problem in reflexive Banach spaces
  55. A parallel inertial three-step iteration monotone hybrid algorithm for a finite family of G-nonexpansive mappings in Hilbert spaces endowed with graphs applicable to signal recovery problems
  56. Multiple and unique nontrivial solutions for fractional differential equations with singular property and derivatives contained in the nonlinear term
  57. New soliton solutions for a nonlinear complex hyperbolic Schrödinger dynamical equation with a truncated M-fractional derivative
  58. On a generalization of derangement polynomials and numbers
  59. The description of entire solutions of complex PDEs and PDDEs
  60. A modified RMIL conjugate gradient-based projection algorithm for constrained nonlinear equations: application to image denoising
  61. Fast solution strategies for time-space fractional linear complementarity problems governing American options pricing
  62. Existence results for Robin problems involving p(x)-Laplacian-like operators with convection term
  63. On asymptotic behaviors of a specific cubic functional equation and its hyperstability
  64. The description of entire solutions for some class of complex nonlinear partial differential equation (systems) in C 2
  65. Variations in the geometry of the basins of escape in a modified Hénon–Heiles potential
  66. A Rothe method for a viscoelastic contact problem involving time-fractional derivatives in locking materials
  67. Upper and lower solution method for a higher order ϕ-Laplacian BVPs on an infinite interval
  68. Weyl almost periodic functions on time scales and their Fourier series
  69. Integrable system of null curve and Betchov-Da Rios equation
  70. Fekete–Szegö problems for (β, Φ)-spirllike mapping of complex order γ in Banach space
  71. Modulated convergence: a deferred approach
  72. Infinitely many solutions for an instantaneous and non-instantaneous fourth-order differential system with local assumptions
  73. Existence and nonexistence of normalized solutions for the Biharmonic equation with combined nonlinearities
  74. Ekeland’s variational principle for interval-valued functions with an α-level set in Kaleva-Seikkala’s type fuzzy metric spaces
  75. On Kurzweil integral of fuzzy number valued functions with two variables
  76. On split common null point and common fixed point problems for multivalued demicontractive mappings
  77. Approximation by weighted Durrmeyer-type max-product neural network operators
  78. A new predictor-corrector interior-point algorithm for semidefinite optimization
  79. Densities of measures: fine properties and examples
  80. Review Articles
  81. Characterization generalized derivations of tensor products of nonassociative algebras
  82. On the performance of the new minimax shrinkage estimators for a normal mean vector
  83. Special Issue on Differential Equations and Numerical Analysis - Part II
  84. Existence and optimal control of Hilfer fractional evolution equations
  85. Persistence of a unique periodic wave train in convecting shallow water fluid
  86. Existence results for critical growth Kohn-Laplace equations with jumping nonlinearities
  87. Monotonicity and oscillation for fractional differential equations with Riemann-Liouville derivatives
  88. Nontrivial solutions for a generalized poly-Laplacian system on finite graphs
  89. Stability and bifurcation analysis of a modified chemostat model
  90. Some new quantum derivatives and integrals with their applications in integral error bounds
  91. Special Issue on Nonlinear Evolution Equations and Their Applications - Part II
  92. Analytic solutions of a generalized complex multi-dimensional system with fractional order
  93. Extraction of soliton solutions and Painlevé test for fractional Peyrard-Bishop DNA model
  94. Special Issue on Recent Developments in Fixed-Point Theory and Applications - Part II
  95. Some fixed point results with the vector degree of nondensifiability in generalized Banach spaces and application on coupled Caputo fractional delay differential equations
  96. On the sum form functional equation related to diversity index
  97. Special Issue on International E-Conference on Mathematical and Statistical Sciences - Part II
  98. Simpson, midpoint, and trapezoid-type inequalities for multiplicatively s-convex functions
  99. Converses of nabla Pachpatte-type dynamic inequalities on arbitrary time scales
  100. Special Issue on Blow-up Phenomena in Nonlinear Equations of Mathematical Physics - Part II
  101. Energy decay of a coupled system involving a biharmonic Schrödinger equation with an internal fractional damping
  102. Special Issue on Some Integral Inequalities, Integral Equations, and Applications - Part II
  103. Nonlinear heat equation with viscoelastic term: Global existence and blowup in finite time
  104. New Jensen's bounds for HA-convex mappings with applications to Shannon entropy
  105. Special Issue on Approximation Theory and Special Functions 2024 conference
  106. Ulam-type stability for Caputo-type fractional delay differential equations
  107. Faster approximation to multivariate functions by combined Bernstein-Taylor operators
  108. (λ, ψ)-Bernstein-Kantorovich operators
  109. Some special functions and cylindrical diffusion equation on α-time scale
  110. (q, p)-Mixing Bloch maps
  111. Orthogonalizing q-Bernoulli polynomials
  112. On better approximation order for the max-product Meyer-König and Zeller operator
  113. Moment-based approximation for a renewal reward process with generalized gamma-distributed interference of chance
  114. A note on linear compositions of the Mellin convolution operators in the weighted Mellin-Lebesgue spaces
  115. A new perspective on generalized Laguerre polynomials
  116. Global existence of semilinear system of Klein-Gordon equations in anti-de Sitter spacetime
  117. Estimates for Durrmeyer-type exponential sampling series in Mellin-Orlicz spaces
  118. -αβ-statistical relative uniform convergence for double sequences and its applications
  119. New developments for the Jacobi polynomials
  120. Generalization of Sheffer-λ polynomials
  121. Fractional calculus containing certain bivariate Mittag-Leffler kernel with respect to function
  122. A new type of soft multi rough sets
  123. Special Issue on Variational Methods and Nonlinear PDEs
  124. A note on mean field type equations
  125. Ground states for fractional Kirchhoff double-phase problem with logarithmic nonlinearity
  126. Solution of nonlinear Langevin equations involving Hilfer-Hadamard fractional order derivatives and variable coefficients
  127. Bifurcation, quasi-periodic, and wave solutions to the fractional model of optical fibers in communication systems
  128. Multiplicity and concentration behavior of solutions for the generalized quasilinear Schrödinger equation with critical growth
  129. Ground state solutions to singularly perturbed Chern-Simons-Schrödinger systems with a neutral scalar field
  130. Weak solutions to an asymptotic equation of the variational sine-Gordon equation
  131. Multiplicity of positive solutions for a concave-convex fractional elliptic system with critical growth
Downloaded on 27.3.2026 from https://www.degruyterbrill.com/document/doi/10.1515/dema-2025-0190/html
Scroll to top button