Abstract

Recently, Kim-Kim introduced the degenerate Whitney numbers of the first and second kind involving the degenerate Dowling polynomials and numbers. In this paper, we introduce the fully degenerate Dowling polynomials and the fully degenerate Bell polynomials and derive some identities involving these polynomials. We also obtain the generating functions, expressions, and recurrence relations for the fully degenerate Dowling polynomials and the fully degenerate Bell polynomials and other special polynomials and numbers.

1. Introduction

The definition and properties of some special polynomials are important, and many academics have studied the definitions and properties of some polynomials or degenerate polynomials [1ā€“4]. Kim and Kim [5] introduced the degenerate Dowling polynomials and degenerate Whitney numbers of the first and second kind and obtain some explicit identities. Kim and Kim [6] introduced degenerate r-Dowling polynomials related to the degenerate r-Whitney numbers of the second kind.

Let be a finite lattice [5, 6], which means it is a finite poset such that every pair of elements in has a supremum and an infimum . A finite lattice is geometric if it is a finite semimodular lattice which is also atomic. For a finite geometric lattice of rank , Dowling [7] defined the Whitney numbers of the first kind and the Whitney numbers of the second kind. In particular, if is the Dowling lattices [5ā€“7] of rank over a finite group of order , then the Whitney numbers of the first kind and the Whitney numbers of the second kind are, respectively, denoted by and .

At the first, we give some definitions and identities needed in this paper. For any nonzero , the degenerate exponential functions are defined bywhere (see [5, 6, 8ā€“11]).

The degenerate Whitney numbers and are defined by the following generating functions with parallel structures,where (see [5, 6]).

Equivalently, relations (2) and (3) are given by

For , the degenerate Dowling polynomials (see [5, 11]) are given bywhen , are the degenerate Dowling numbers. Note thatwhere are the Dowling polynomials.

From (6), we have(see [6, 11]).

The degenerate Bell polynomials (see [5, 8ā€“12]) are defined bywhen , are the degenerate Bell numbers.

From (9), we note thatwhere , (see [9]).

The fully degenerate Bell polynomials (see [8, 9, 13]) are defined by

From [13], we have

In [9], we note that

The degenerate Stirling numbers of the first kind and the second kind (see [6, 8, 9, 11, 14]) are defined by

By the inversion of (14) and (15), we have

Recently, we are interested in the degenerate Dowling polynomials and numbers and the degenerate Bell polynomials and numbers. In this paper, we study the fully degenerate Dowling polynomials and numbers and the fully degenerate Bell polynomials and numbers. Meanwhile, we derive some identities and expressions of them.

2. Fully Degenerate Dowling Polynomials

In this section, we introduce the fully degenerate Dowling polynomials. We also show several identities and properties related to the fully degenerate Dowling polynomials and numbers.

The fully degenerate Dowling polynomials are defined bywhen , are called the fully degenerate Dowling numbers.

The four identities in the following lemma can be shown just as in Theorem 1, Corollary 1, Theorem 10, and Theorem 17 of [5].

Lemma 1. For ,

Lemma 2. For with ,

Lemma 3. For ,

Lemma 4. For with ,

Theorem 5. For , we have

Proof. By Lemma 1 and (18), we haveSo, from (24), we obtain Theorem 5.

Theorem 6. For , we have

Proof. From (18), we haveFrom (26), we obtain Theorem 6.

In particular, when , we note that

Theorem 7. For , we have

Proof. From (18), we getSo, by (29), we obtain Theorem 7.

Theorem 8. For , we have

Proof. By (18), we getFrom (31), we get Theorem 8.

In particular, when , we have

Theorem 9. For ,

Proof. From Theorem 5 and Lemma 3, we note thatFrom (34), we obtain Theorem 9.

Theorem 10. For ,

Proof. By Theorem 5 and Lemma 2, let , we haveBy (36), we obtain Theorem 10.

Theorem 11. For ,

Proof. By (13), Theorem 5 and Lemma 4, we note thatBy (38), we obtain Theorem 11.

From [13], we have

We note that

From (40), we note that

So, we have

From (42), we have

Theorem 12. For ,

Proof. By (18), (41), and (43), we haveTherefore, from (45), we obtain Theorem 12.

3. Remarks

Recently, the degenerate Poisson random variable with parameter , probability mass function is given by (see [15])

Now, we would like to give the relation between the fully degenerate Dowling polynomials and degenerate Poisson random variables. So, we slightly modify our fully degenerate Dowling polynomials which are given by

Theorem 13. where is the degenerate Poisson random variable with parameters .

Proof. Let be the degenerate Poisson random variable with parameters , then we haveOn the other hand, we easily getSo, by (49) and (50), we obtain Theorem 13.

4. Conclusion

In this paper, we introduced the fully degenerate Dowling polynomials and the fully degenerate Bell polynomials , which are degenerate versions of the Dowling polynomials and the Bell polynomials .

We showed the fully degenerate Dowling polynomials with Whitney numbers in Theorem 5. We used different methods for the fully degenerate Dowling polynomials to obtain some identities related to the Stirling numbers of the first kind and the second kind, the degenerate Stirling numbers of the second kind and the fully degenerate Bell polynomials in Theorems 6ā€“8 and 11. Meanwhile, we investigated the recurrence relations for the fully degenerate Dowling polynomials in Theorem 9. In particular, we let and , and we have also obtained the special relation between the fully degenerate Dowling polynomials and the degenerate Stirling numbers of the second kind in Theorem 10. Furthermore, we used the differential equation to obtain the identities associated with the fully degenerate Dowling polynomials in Theorem 12. Assume that is the degenerate Poisson random variable with parameter , we showed that the Poisson degenerate central moments is equal to in Theorem 13.

This has profound implications for us to continue to study various degenerate versions of many special polynomials and numbers in the future.

Data Availability

No data were used to support the findings of this study.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this article.

Acknowledgments

This research was funded by the National Natural Science Foundation of China (No. 12271320, 11871317) and Key Research and Development Program of Shaanxi (No. 2023-ZDLGY-02, 2023-YBGY-016).