Home Mathematics Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials
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Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials

  • Taekyun Kim , Dae San Kim , Dmitry V. Dolgy and Jin-Woo Park EMAIL logo
Published/Copyright: December 31, 2021

Abstract

The aim of this paper is to study the Poisson random variables in relation to the Lah-Bell polynomials and the degenerate binomial and degenerate Poisson random variables in connection with the degenerate Lah-Bell polynomials. Among other things, we show that the rising factorial moments of the degenerate Poisson random variable with parameter α are given by the degenerate Lah-Bell polynomials evaluated at α . We also show that the probability-generating function of the degenerate Poisson random variable is equal to the generating function of the degenerate Lah-Bell polynomials. Also, we show similar results for the Poisson random variables. Here the n th Lah-Bell number counts the number of ways a set of n elements can be partitioned into non-empty linearly ordered subsets, the Lah-Bell polynomials are natural extensions of the Lah-Bell numbers and the degenerate Lah-Bell polynomials are degenerate versions of the Lah-Bell polynomials.

MSC 2010: 65C50; 11B73; 11B84

1 Introduction

The aim of this paper is to study the Poisson random variables in relation to the Lah-Bell polynomials and the degenerate binomial and degenerate Poisson random variables in connection with the degenerate Lah-Bell polynomials. Here Lah-Bell polynomials B n L ( x ) are natural extension of the Lah-Bell numbers B n L , which are defined as the number of ways a set of n elements can be partitioned into non-empty linearly ordered subsets (see [1]). Thus, we have B n L = k = 0 n L ( n , k ) , where L ( n , k ) counts the number of ways a set of n elements can be partitioned into k non-empty linearly ordered subsets, called the unsigned Lah numbers (see [2]). The motivation for our introduction of the degenerate binomial and degenerate Poisson random variables is as follows. Let us assume that the probability of success in a trial is p . Then we might wonder if the probability of success in the ninth trial is still p after failing eight times in the trial experiment. Because there is a psychological burden for one to be successful, it seems plausible that the probability is less than p . This speculation motivated our study of the degenerate binomial and degenerate Poisson random variables.

The outline of our main results is as follows. We derive the expectation and variance of the degenerate binomial and degenerate Poisson random variables. Then we introduce the degenerate Lah-Bell polynomials which are degenerate versions of the Lah-Bell polynomials. Then, among other things, we show that the rising factorial moments of the degenerate Poisson random variable with parameter α are given by the degenerate Lah-Bell polynomials evaluated at α . We also show that the probability-generating function of the degenerate Poisson random variable is equal to the generating function of the degenerate Lah-Bell polynomials. In addition, we show that the rising factorial moments of the Poisson random variable with parameter α are given by the Lah-Bell polynomials evaluated at α . Furthermore, we show that the probability-generating function of the Poisson random variable is equal to the generating function of the Lah-Bell polynomials.

The novelty of this paper is that it reveals the connection between the rising factorial moments of the Poisson random variable and the Lah-Bell polynomials and that between the rising factorial moments of the degenerate Poisson random variable and the degenerate Lah-Bell polynomials. For the rest of this section, we recall the necessary facts that will be needed throughout this paper.

For any 0 λ R , the degenerate exponential functions are defined by (see [3])

(1) e λ x ( t ) = k = 0 ( x ) k , λ k ! t k ,

where ( x ) 0 , λ = 1 , ( x ) n , λ = x ( x λ ) ( x ( n 1 ) λ ) , ( n 1 ) . Note that

lim λ 0 e λ x ( t ) = e x t , e λ ( t ) = e λ 1 ( t ) .

For n , k 0 , the unsigned Lah numbers are given by (see [1,2,4,5])

(2) L ( n , k ) = n 1 k 1 n ! k ! .

In [3], the Lah-Bell polynomials are defined by

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

For x = 1 , B n L = B n L ( 1 ) ( n 0 ) , are called the Lah-Bell numbers. Here we recall from [1] that B n L counts the number of ways a set of n elements can be partitioned into non-empty linearly ordered subsets. From (3), we note that (see [1])

(4) B n L ( x ) = k = 0 n x k L ( n , k ) , ( n 0 ) .

A sample space is the set of all possible outcomes of an experiment and an event is any subset of the sample space. A random variable X is a real valued function on a sample space. If X takes any values in a countable set, then X is called a discrete random variable. If X takes any values in an interval on the real line, then X is called a continuous random variable.

For a discrete random variable X , the probability mass function p ( a ) of X is defined as (see [6,7, 8,9])

(5) p ( a ) = P { X = a } .

Suppose that n independent trials, each of which results in a “success” with probability p and in a “failure” with probability 1 p , are to be performed. If X denotes the number of successes that occur in n trials, then X is called the binomial random variable with parameter n , p , which is denoted by X B ( n , p ) . Let X B ( n , p ) . Then the probability mass function of X is given by

(6) p ( i ) = n i p i ( 1 p ) n i , i = 0 , 1 , 2 , , n .

A Poisson random variable indicates how many events occurred within a given period of time. A random variable X , 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 X is given by (see [8])

(7) p ( i ) = e α α i i ! .

Let f ( x ) be a real valued function and let X be a random variable. Then we define (see [8])

(8) E [ f ( X ) ] = i = 0 f ( i ) p ( i ) ,

where p ( x ) is the probability mass function of X .

It is well known that the Bell polynomials are defined by (see [3,10,11])

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

Let us take f ( x ) = x n , ( n 0 ) . Then we have the moments of the Poisson random variable X with parameter α ( > 0 ) as follows (see [11]):

(10) E [ X n ] = B n ( α ) , ( n 0 ) .

2 Poisson random variables

The falling factorial sequence is given by

( x ) 0 = 1 , ( x ) n = x ( x 1 ) ( x n + 1 ) , ( n 1 ) ,

while the rising factorial sequence is given by (see [1, 2,3,4,6,7,8,10,11,12])

x 0 = 1 , x n = x ( x + 1 ) ( x + n 1 ) , ( n 1 ) .

Replacing t by log ( 1 + t ) in (9), we get

(11) e x t = k = 0 B k ( x ) 1 k ! ( log ( 1 + t ) ) k = k = 0 B k ( x ) n = k S 1 ( n , k ) t n n ! = n = 0 k = 0 n B k ( x ) S 1 ( n , k ) t n n ! ,

where S 1 ( n , k ) are the Stirling numbers of the first kind defined by

(12) ( x ) n = k = 0 n S 1 ( n , k ) x k , ( n 0 ) .

Therefore, by (11), we obtain the following lemma.

Lemma 1

For n 0 , we have

x n = k = 0 n S 1 ( n , k ) B k ( x )

and

B n ( x ) = k = 0 n S 2 ( n , k ) x k .

Let X be the Poisson random variable with parameter α ( > 0 ) . Then we have

(13) E [ ( X ) n ] = k = 0 n S 1 ( n , k ) E [ X k ] = k = 0 n S 1 ( n , k ) B k ( α ) .

From Lemma 1 and (13), we note the well-known fact about the falling factorial moments of the random variable X , namely, the expectation of the falling factorial of the random variable X :

(14) E [ ( X ) n ] = k = 0 n S 1 ( n , k ) B k ( α ) = α n , ( n 0 ) .

On the other hand, the rising factorial moment of X , namely the expectation of the rising factorial of X , is given by

(15) E [ X n ] = k = 0 k n p ( k ) = e α k = 0 k n k ! α k .

From (3), we can derive the following equation:

(16) n = 0 B n L ( α ) t n n ! = e α e α 1 1 t = e α k = 0 α k 1 k ! 1 1 t k = e α k = 0 α k k ! n = 0 k n t n n ! = n = 0 e α k = 0 k n k ! α k t n n ! .

Comparing the coefficients on both sides of (16), we have the following identity:

(17) B n L ( α ) = e α k = 0 k n k ! α k ,

where n is a non-negative integer.

Therefore, by (14), (15) and (17), we obtain the following theorem. In particular, it shows that the rising factorial moments of the Poisson random variable with parameter α are given by the Lah-Bell polynomials evaluated at α . This fact seems to be new.

Theorem 2

Let X be the Poisson random variable with parameter α ( > 0 ) . Then we have

E [ ( X ) n ] = α n

and

E [ X n ] = B n L ( α ) , ( n 0 ) .

Let X be the Poisson random variable with parameter α ( > 0 ) . From (7) and (8), we have

(18) E 1 1 t X = k = 0 1 1 t k p ( k ) = k = 0 1 1 t k e α α k k ! = e α e α 1 t = e α 1 1 t 1 .

Now, by (3) and (18), we obtain the following theorem which says that the probability-generating function of X is equal to the generating function of the Lah-Bell polynomials.

Theorem 3

Let X be the Poisson random variable with parameter α ( > 0 ) . Then we have

E 1 1 t X = e α 1 1 t 1 = n = 0 B n L ( α ) t n n ! .

From Theorem 3 and (10), we note that

(19) n = 0 B n L ( α ) t n n ! = k = 0 E [ X k ] ( log ( 1 t ) ) k k ! = k = 0 ( 1 ) k B k ( α ) n = k ( 1 ) n S 1 ( n , k ) t n n ! = n = 0 k = 0 n ( 1 ) n k S 1 ( n , k ) B k ( α ) t n n ! .

Therefore, by Theorem 2, (4) and (19), we obtain the following theorem.

Theorem 4

Let X be the Poisson random variable with parameter α ( > 0 ) . Then we have

E [ X n ] = B n L ( α ) = k = 0 n L ( n , k ) α k = k = 0 n ( 1 ) n k S 1 ( n , k ) B k ( α ) .

3 Degenerate binomial and degenerate Poisson random variables

In this section, we assume that λ ( 0 , 1 ) , and p is the probability of success of an experiment. For λ ( 0 , 1 ) , X λ is the degenerate binomial random variable with parameter n , p , denoted by X λ B λ ( n , p ) , if the probability mass function of X λ is given by

(20) p λ ( i ) = P { X λ = i } = n i ( p ) i , λ ( 1 p ) n i , λ 1 ( 1 ) n , λ ,

where i = 0 , 1 , 2 , , n .

From (20), we note that

i = 0 p λ ( i ) = 1 ( 1 ) n , λ i = 0 n n i ( p ) i , λ ( 1 p ) n i , λ = 1 .

For X λ B λ ( n , k ) , we have

(21) E [ X λ ] = i = 0 i p λ ( i ) = 1 ( 1 ) n , λ i = 0 i n i ( p ) i , λ ( 1 p ) n i , λ = n ( 1 ) n , λ i = 1 n 1 i 1 ( p ) i , λ ( 1 p ) n i , λ = n ( 1 ) n , λ i = 0 n 1 i ( p ) i + 1 , λ ( 1 p ) n 1 i , λ = n p ( 1 ) n , λ i = 0 n 1 n 1 i ( p λ ) i , λ ( 1 p ) n 1 i , λ = n p ( 1 ) n , λ ( p λ + 1 p ) n 1 , λ = n p ( 1 ) n , λ ( 1 λ ) n 1 , λ .

Therefore, we obtain the following theorem.

Theorem 5

For X λ B λ ( n , p ) , ( n 0 ) , we have

E [ X λ ] = n p ( 1 ) n , λ ( 1 λ ) n 1 , λ .

Note that

lim λ 0 E [ X λ ] = n p = E [ X ] ,

where X is the binomial random variable with parameter n , p .

For X λ B λ ( n , p ) , we observe that

(22) E [ X λ 2 ] = i = 0 i 2 p λ ( i ) = 1 ( 1 ) n , λ i = 0 i 2 n i ( p ) i , λ ( 1 p ) n i , λ = 1 ( 1 ) n , λ i = 0 i ( i 1 + 1 ) n i ( p ) i , λ ( 1 p ) n i , λ = 1 ( 1 ) n , λ i = 0 i ( i 1 ) n i ( p ) i , λ ( 1 p ) n i , λ + E [ X λ ] = n ( n 1 ) ( 1 ) n , λ i = 2 n 2 i 2 ( p ) i , λ ( 1 p ) n i , λ + E [ X λ ] = n ( n 1 ) ( 1 ) n , λ i = 0 n 2 n 2 i ( p ) i + 2 , λ ( 1 p ) n 2 i , λ + E [ X λ ] = n ( n 1 ) p ( p λ ) ( 1 ) n , λ i = 0 n 2 n 2 i ( p 2 λ ) i , λ ( 1 p ) n 2 i , λ + E [ X λ ] = n ( n 1 ) p ( p λ ) ( 1 ) n , λ ( p 2 λ + 1 p ) n 2 , λ + E [ X λ ] = n ( n 1 ) p ( p λ ) ( 1 ) n , λ ( 1 2 λ ) n 2 , λ + n p ( 1 ) n , λ ( 1 λ ) n 1 , λ = n p ( 1 2 λ ) n 2 , λ ( 1 ) n , λ { ( p λ ) ( n 1 ) + ( 1 λ ) } = n p ( 1 ) n , λ ( 1 2 λ ) n 2 , , λ ( p ( n 1 ) + 1 n λ ) .

By using Theorem 5 and (22), the variance Var ( X λ ) of the random variable X λ is given by

(23) Var ( X λ ) = E [ X λ 2 ] ( E [ X λ ] ) 2 = n p ( 1 ) n , λ ( 1 2 λ ) n 2 , λ ( p ( n 1 ) + 1 n λ ) n p ( 1 ) n , λ ( 1 λ ) n 1 , λ 2 = n p ( 1 ) n , λ ( 1 2 λ ) n 2 , λ ( p ( n 1 ) + 1 n λ ) n p ( 1 ) n , λ ( 1 λ ) ( 1 2 λ ) n 2 , λ 2 = n p ( 1 2 λ ) n 2 , λ ( 1 ) n , λ p ( n 1 ) + 1 n λ n p ( 1 ) n , λ ( 1 λ ) 2 ( 1 2 λ ) n 2 , λ = n p ( 1 ) n , λ ( 1 2 λ ) n 2 , λ ( ( n 1 ) p + 1 n λ E [ X λ ] ( 1 λ ) ) .

Therefore, we obtain the following theorem.

Theorem 6

For X λ B λ ( n , p ) , we have

Var ( X λ ) = n p ( 1 ) n , λ ( 1 2 λ ) n 2 , λ ( ( n 1 ) p + 1 n λ E [ X λ ] ( 1 λ ) ) .

Note that

lim λ 0 Var ( X λ ) = n p ( 1 p ) = Var ( X ) ,

where X is the binomial random variable with parameters n , p .

The generating function of the moments of X λ B λ ( n , p ) is given by

n = 0 E [ X λ n ] t n n ! = E [ e X λ t ] = 1 ( 1 ) n , λ i = 0 n e i t n i ( p ) i , λ ( 1 p ) n i , λ .

Thus, we have

E [ X λ n ] = d n d t n E [ e X λ t ] t = 0 = 1 ( 1 ) n , λ i = 0 n n i i n ( p ) i , λ ( 1 p ) n i , λ .

For λ ( 0 , 1 ) , X λ is the degenerate Poisson random variable with parameter α ( > 0 ) , if the probability mass function of X λ is given by

(24) p λ ( i ) = P { X λ = i } = e λ 1 ( α ) α i i ! ( 1 ) i , λ ,

where i = 0 , 1 , 2 , .

By (24), we get

i = 0 p λ ( i ) = e λ 1 ( α ) i = 0 ( 1 ) i , λ i ! α i = e λ 1 ( α ) e λ ( α ) = 1 .

It is easy to show that

E [ X λ ] = α 1 + α λ

and

E [ X λ 2 ] = α + α 2 ( 1 + α λ ) 2 .

Thus, we have

Var ( X λ ) = E [ X λ 2 ] ( E [ X λ ] ) 2 = α ( 1 + α λ ) 2 .

Let X λ be the degenerate Poisson random variable with parameter α ( > 0 ) . Then we have

(25) E [ X λ n ] = i = 0 i n p λ ( i ) = i = 0 i n e λ 1 ( α ) ( 1 ) n , λ i ! α i = e λ 1 ( α ) i = 0 ( 1 ) i , λ i n i ! α i .

In view of (3), we may consider the degenerate Lah-Bell polynomials given by

(26) e λ 1 ( x ) e λ x 1 1 t = n = 0 B n , λ L ( x ) t n n ! .

Note that

n = 0 lim λ 0 B n , λ L ( x ) t n n ! = e x 1 1 t 1 = n = 0 B n L ( x ) t n n ! .

Thus, we have

lim λ 0 B n , λ L ( x ) = B n L ( x ) , ( n 0 ) .

Now, we observe that

(27) e λ 1 ( x ) e λ x 1 1 t = e λ 1 ( x ) k = 0 ( 1 ) k , λ x k 1 k ! 1 1 t k = e λ 1 ( x ) k = 0 ( 1 ) k , λ x k 1 k ! n = 0 k n n ! t n = n = 0 e λ 1 ( x ) k = 0 ( 1 ) k , λ k n k ! x k t n n ! .

From (25), (26) and (27), we obtain the next result. In particular, it says that the rising factorial moments of the degenerate Poisson random variable with parameter α are given by the degenerate Lah-Bell polynomials evaluated at α .

Theorem 7

For n 0 , we have

B n , λ L ( x ) = e λ 1 ( x ) k = 0 ( 1 ) k , λ k n k ! x k .

For the degenerate Poisson random variable X λ with parameter α > 0 , we have

E [ X λ n ] = B n , λ L ( α ) , ( n 0 ) .

The degenerate Bell polynomials are defined in [3] as

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

Note that

n = 0 lim λ 0 B n , λ ( x ) t n n ! = e x ( e t 1 ) = n = 0 B n ( x ) t n n ! ,

where B n ( x ) are the ordinary Bell polynomials. Thus, we have

lim λ 0 B n , λ ( x ) = B n ( x ) , ( n 0 ) .

Replacing t by log ( 1 t ) in (28), we get

(29) e λ 1 ( x ) e λ x 1 1 t = k = 0 B k , λ ( x ) ( 1 ) k 1 k ! ( log ( 1 t ) ) k = n = 0 k = 0 n ( 1 ) n k S 1 ( n , k ) B k , λ ( x ) t n n ! .

Therefore, by (26), (28) and (29), we obtain the following theorem.

Theorem 8

For n 0 , we have

(30) B n , λ L ( x ) = k = 0 n ( 1 ) n k S 1 ( n , k ) B k , λ ( x )

and

B n , λ ( x ) = k = 0 n ( 1 ) n k S 2 ( n , k ) B k , λ L ( x ) ,

where S 2 ( n , k ) , ( n , k 0 ) , are the Stirling numbers of the second kind defined by

x n = k = 0 n S 2 ( n , k ) ( x ) k .

From Theorem 11 of [3], we recall that

(31) B n , λ ( x ) = k = 0 n ( 1 ) k , λ x 1 + λ x k S 2 ( n , k ) .

Combining (30) and (31), we have another expression for B n , λ ( x ) as follows:

(32) B n , λ L ( x ) = l = 0 n k = l n ( 1 ) n k S 1 ( n , k ) S 2 ( k , l ) ( 1 ) l , λ x 1 + λ x l .

Let X λ be the degenerate Poisson random variable with parameter α ( > 0 ) . Then we have

(33) E 1 1 t X λ = i = 0 1 1 t i p λ ( i ) = e λ 1 ( α ) i = 0 ( 1 ) i , λ α i i ! 1 1 t i = e λ 1 ( α ) e λ α 1 1 t .

Therefore, we obtain the following theorem from Theorem 7, (32) and (33). In particular, it states that the probability-generating function of X λ is equal to the generating function of the degenerate Lah-Bell polynomials.

Theorem 9

Let X λ be the degenerate Poisson random variable with parameter α > 0 . Then we have

E 1 1 t X λ = e λ 1 ( α ) e λ α 1 1 t

and

E [ X λ n ] = l = 0 n k = l n ( 1 ) n k S 1 ( n , k ) S 2 ( k , l ) ( 1 ) l , λ α 1 + λ α l , ( n 0 ) .

4 Conclusion

In this paper, we introduced the degenerate Lah-Bell polynomials which are degenerate versions of the recently introduced Lah-Bell polynomials. As stated in the Section 1, the novelty of this paper is that it reveals the connection between the rising factorial moments of the Poisson random variable and the Lah-Bell polynomials and that between the rising factorial moments of the degenerate Poisson random variable and the degenerate Lah-Bell polynomials.

The details of the results obtained are as follows. For Poisson random variable X with parameter α > 0 , we showed that the rising factorial moments of X are given by the Lah-Bell polynomials evaluated at α (Theorem 2) and also by an expression involving Bell polynomials evaluated at α (Theorem 4). We also showed that the probability-generating function of X is equal to the generating function of the Lah-Bell polynomials (Theorem 3). Let X λ B λ ( n , p ) be the degenerate binomial random variable with parameter n , p . Then we derived the expectation of X λ (Theorem 5) and the variance of X λ (Theorem 6). Now, let X λ denote the degenerate Poisson random variable with parameter α . Then we showed that the rising factorial moments of X λ are given by the degenerate Lah-Bell polynomials evaluated at α (Theorem 7) and also by another expression involving the Stirling numbers of both kinds (Theorem 9). We also showed that the probability-generating function of X λ is equal to the generating function of the degenerate Lah-Bell polynomials (Theorem 9). Furthermore, we obtained relations between the degenerate Lah-Bell polynomials and the degenerate Bell polynomials (Theorem 8).

Here, we would like to mention that studying various degenerate versions of some special numbers and polynomials, which was initiated by Carlitz when he investigated the degenerate Bernoulli and Euler polynomials and numbers, regained interests of some mathematicians in recent years. They have been studied by using several different tools like generating functions, combinatorial methods, p -adic analysis, umbral calculus, special functions, differential equations, and probability theory as we did in the present paper.

It is one of our future projects to continue to study various degenerate versions of some special polynomials and numbers and to find their applications in physics, science, and engineering as well as in mathematics.

  1. Funding information: This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) 2020R1F1A1A01075658.

  2. Author contributions: T.K. and D.S.K. conceived of the framework and structured the whole paper; T.K. and D.S.K. wrote the paper; D.S.K. completed the revision of the article; and J.W.P. and D.V.D. checked the errors of the article. All authors have read and agreed to the published version of the manuscript.

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

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Received: 2021-05-01
Revised: 2021-10-01
Accepted: 2021-10-22
Published Online: 2021-12-31

© 2021 Taekyun Kim et al., published by De Gruyter

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

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  63. On the evolutionary bifurcation curves for the one-dimensional prescribed mean curvature equation with logistic type
  64. On intersections of two non-incident subgroups of finite p-groups
  65. Global existence and boundedness in a two-species chemotaxis system with nonlinear diffusion
  66. Finite groups with 4p2q elements of maximal order
  67. Positive solutions of a discrete nonlinear third-order three-point eigenvalue problem with sign-changing Green's function
  68. Power moments of automorphic L-functions related to Maass forms for SL3(ℤ)
  69. Entire solutions for several general quadratic trinomial differential difference equations
  70. Strong consistency of regression function estimator with martingale difference errors
  71. Fractional Hermite-Hadamard-type inequalities for interval-valued co-ordinated convex functions
  72. Montgomery identity and Ostrowski-type inequalities via quantum calculus
  73. Universal inequalities of the poly-drifting Laplacian on smooth metric measure spaces
  74. On reducible non-Weierstrass semigroups
  75. so-metrizable spaces and images of metric spaces
  76. Some new parameterized inequalities for co-ordinated convex functions involving generalized fractional integrals
  77. The concept of cone b-Banach space and fixed point theorems
  78. Complete consistency for the estimator of nonparametric regression model based on m-END errors
  79. A posteriori error estimates based on superconvergence of FEM for fractional evolution equations
  80. Solution of integral equations via coupled fixed point theorems in 𝔉-complete metric spaces
  81. Symmetric pairs and pseudosymmetry of Θ-Yetter-Drinfeld categories for Hom-Hopf algebras
  82. A new characterization of the automorphism groups of Mathieu groups
  83. The role of w-tilting modules in relative Gorenstein (co)homology
  84. Primitive and decomposable elements in homology of ΩΣℂP
  85. The G-sequence shadowing property and G-equicontinuity of the inverse limit spaces under group action
  86. Classification of f-biharmonic submanifolds in Lorentz space forms
  87. Some new results on the weaving of K-g-frames in Hilbert spaces
  88. Matrix representation of a cross product and related curl-based differential operators in all space dimensions
  89. Global optimization and applications to a variational inequality problem
  90. Functional equations related to higher derivations in semiprime rings
  91. A partial order on transformation semigroups with restricted range that preserve double direction equivalence
  92. On multi-step methods for singular fractional q-integro-differential equations
  93. Compact perturbations of operators with property (t)
  94. Entire solutions for several complex partial differential-difference equations of Fermat type in ℂ2
  95. Random attractors for stochastic plate equations with memory in unbounded domains
  96. On the convergence of two-step modulus-based matrix splitting iteration method
  97. On the separation method in stochastic reconstruction problem
  98. Robust estimation for partial functional linear regression models based on FPCA and weighted composite quantile regression
  99. Structure of coincidence isometry groups
  100. Sharp function estimates and boundedness for Toeplitz-type operators associated with general fractional integral operators
  101. Oscillatory hyper-Hilbert transform on Wiener amalgam spaces
  102. Euler-type sums involving multiple harmonic sums and binomial coefficients
  103. Poly-falling factorial sequences and poly-rising factorial sequences
  104. Geometric approximations to transition densities of Jump-type Markov processes
  105. Multiple solutions for a quasilinear Choquard equation with critical nonlinearity
  106. Bifurcations and exact traveling wave solutions for the regularized Schamel equation
  107. Almost factorizable weakly type B semigroups
  108. The finite spectrum of Sturm-Liouville problems with n transmission conditions and quadratic eigenparameter-dependent boundary conditions
  109. Ground state sign-changing solutions for a class of quasilinear Schrödinger equations
  110. Epi-quasi normality
  111. Derivative and higher-order Cauchy integral formula of matrix functions
  112. Commutators of multilinear strongly singular integrals on nonhomogeneous metric measure spaces
  113. Solutions to a multi-phase model of sea ice growth
  114. Existence and simulation of positive solutions for m-point fractional differential equations with derivative terms
  115. Bernstein-Walsh type inequalities for derivatives of algebraic polynomials in quasidisks
  116. Review Article
  117. Semiprimeness of semigroup algebras
  118. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part II)
  119. Third-order differential equations with three-point boundary conditions
  120. Fractional calculus, zeta functions and Shannon entropy
  121. Uniqueness of positive solutions for boundary value problems associated with indefinite ϕ-Laplacian-type equations
  122. Synchronization of Caputo fractional neural networks with bounded time variable delays
  123. On quasilinear elliptic problems with finite or infinite potential wells
  124. Deterministic and random approximation by the combination of algebraic polynomials and trigonometric polynomials
  125. On a fractional Schrödinger-Poisson system with strong singularity
  126. Parabolic inequalities in Orlicz spaces with data in L1
  127. Special Issue on Evolution Equations, Theory and Applications (Part II)
  128. Impulsive Caputo-Fabrizio fractional differential equations in b-metric spaces
  129. Existence of a solution of Hilfer fractional hybrid problems via new Krasnoselskii-type fixed point theorems
  130. On a nonlinear system of Riemann-Liouville fractional differential equations with semi-coupled integro-multipoint boundary conditions
  131. Blow-up results of the positive solution for a class of degenerate parabolic equations
  132. Long time decay for 3D Navier-Stokes equations in Fourier-Lei-Lin spaces
  133. On the extinction problem for a p-Laplacian equation with a nonlinear gradient source
  134. General decay rate for a viscoelastic wave equation with distributed delay and Balakrishnan-Taylor damping
  135. On hyponormality on a weighted annulus
  136. Exponential stability of Timoshenko system in thermoelasticity of second sound with a memory and distributed delay term
  137. Convergence results on Picard-Krasnoselskii hybrid iterative process in CAT(0) spaces
  138. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part I)
  139. Marangoni convection in layers of water-based nanofluids under the effect of rotation
  140. A transient analysis to the M(τ)/M(τ)/k queue with time-dependent parameters
  141. Existence of random attractors and the upper semicontinuity for small random perturbations of 2D Navier-Stokes equations with linear damping
  142. Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials
  143. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  144. On the mixed fractional quantum and Hadamard derivatives for impulsive boundary value problems
  145. The Lp dual Minkowski problem about 0 < p < 1 and q > 0
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